Patent Application
20220393081
The present invention relates to a light-emitting device including a blue semiconductor light-emitting element, a green phosphor and a red phosphor, and to a method for designing a light-emitting device.
Recent advances toward higher output and higher efficiency in GaN related semiconductor light-emitting elements have been dramatic. In addition, active research is underway to increase efficiency of semiconductor light-emitting elements and various phosphors that use an electron beam as an excitation source. As a result, power-saving capabilities of today's light-emitting devices such as light sources, light source modules including light sources, fixtures including light source modules, and systems including fixtures are advancing rapidly as compared to their conventional counterparts.
For example, it is widely popular to incorporate a GaN related blue light-emitting element as an excitation light source of a yellow phosphor and create a so-called pseudo-white light source from a spectrum of the GaN related blue light-emitting element and a spectrum of the yellow phosphor, use the pseudo-white light source as an illumination light source or create a lighting fixture that incorporates the pseudo-white light source or, further, fabricate a lighting system in which a plurality of such fixtures are arranged in a space (refer to Patent Document 1).
Among packaged LEDs (for example, those that include the GaN related blue light-emitting element, the yellow phosphor, an encapsulant, and the like in a package material) which are a type of an illumination light source that can be incorporated into such modes, there are products with luminous efficacy of a source as a packaged LED exceeding 150 lm/W in a correlated color temperature (CCT) region of around 6000 K (refer to Non-Patent Document 2).
Furthermore, similar advances toward higher efficiency and greater power saving are being made in light sources for liquid crystal display (LCD) backlighting and the like.
However, many have pointed out that such light-emitting devices aiming for higher efficiency do not give sufficient consideration to color appearance. In particular, when used for illumination purposes, “color appearance” when illuminating an object with a light-emitting device such as a light source, fixture, system, or the like is particularly important together with increasing efficiency of the light-emitting device.
Furthermore, some of such light-emitting devices designed with the intention of enhancing efficiency do not give sufficient consideration to color appearance of an illuminated object. Attempts to address this issue include superimposing a spectrum of a red phosphor or a red semiconductor light-emitting element on a spectrum of a blue light-emitting element and a spectrum of a yellow phosphor in order to improve scores of a color rendering index (CRI) (CIE (13.3)) as established by the International Commission on Illumination (Commission Internationale de l'Eclairage/CIE). For example, while an average color rendering index (Ra) and a special color rendering index (R9) with respect to a vivid red color sample for a typical spectrum (CCT=around 6800 K) that does not include a red source are Ra=81 and R9=24 respectively, the scores of the color rendering indices can be improved to Ra=98 and R9=95 when a red source is included (refer to Patent Document 2).
On the other hand, based on novel experimental facts with respect to color appearance of an illuminated object, the present inventor has disclosed an illumination method, and a light-emitting device in general such as an illumination light source, a lighting fixture, and a lighting system, which are capable of realizing a natural, vivid, highly visible and comfortable appearance of colors or an appearance of objects as perceived by a human observer as if the objects were seen under an outdoor high luminance environment, regardless of values of various color rendition indexes (refer to Patent Documents 3 and 4).
According to Patent Documents 3 and 4, a light-emitting device can be realized which is capable of achieving a natural, vivid, highly visible and comfortable appearance of colors or an appearance of objects as perceived by a human observer when an index Acg related to a spectral power distribution of light emitted by a light-emitting device is in a range of −360 or more and −10 or less.
However, while the two patents described above disclose details related to radiant efficiency (luminous efficacy of radiation) K (lm/W) as derived from spectral power distribution, there is no description of efficiency as an actual light source or, in other words, light source efficiency (luminous efficacy of a source) η (lm/W). With an actual LED light source, the latter is equally as important as the former and both are normally respectively treated as independent efficiency indexes. The former (luminous efficacy of radiation K) is efficiency dependent “only on shape” of a spectral power distribution of a light source in its relationship with spectral luminous efficiency V(λ) and is an extremely useful index when considering ideal efficiency. On the other hand, the latter (light source efficiency η) is a quantity indicating how much of power supplied to a light-emitting device is converted into a luminous flux and must also be evaluated from a different perspective from luminous efficacy of radiation.
It is an object of the present invention to improve light source efficiency of “a light-emitting device capable of realizing a natural, vivid, highly visible and comfortable appearance of colors or an appearance of objects” already arrived at by the present inventor by adopting a spectral power distribution having a shape completely different from the shape of conventionally known spectral power distributions while maintaining favorable color appearance characteristics.
As a result of extensive research conducted in order to study a light-emitting device that achieves the object described above, the present inventor arrived at a light-emitting device configured as follows.
A first aspect of a first invention of the present invention is
a light-emitting device at least including, as light-emitting elements:
a blue semiconductor light-emitting element;
a green phosphor; and
a red phosphor, wherein
light emitted from the light-emitting device in a main radiant direction satisfies all of Conditions 1 to 4 below.
when λ denotes wavelength, φSSL1 (λ) denotes a spectral power distribution of light emitted from the light-emitting device in the main radiant direction,
φref1 (λ) denotes a spectral power distribution of reference light which is selected in accordance with a correlated color temperature TSSL1 of the light emitted from the light-emitting device in the main radiant direction,
(XSSL1, YSSL1, ZSSL1) denote tristimulus values of the light emitted from the light-emitting device in the main radiant direction, and
(Xref1, Yref1, Zref1) denote tristimulus values of the reference light which is selected in accordance with TSSL1 of the light emitted from the light-emitting device in the main radiant direction, and
a normalized spectral power distribution SSSL1(λ) of the light emitted from the light-emitting device in the main radiant direction, a normalized spectral power distribution Sref1(λ) of the reference light which is selected in accordance with TSSL1 (λ) of the light emitted from the light-emitting device in the main radiant direction, and a difference ΔSSSL1(λ) of between normalized spectral power distributions are respectively defined as
S
SSL1(λ)=φSSL1(λ)/YSSL1
S
ref1(λ)=φref1(λ)/Yref1
ΔSSSL1(λ)=Sref1(λ)−SSSL1(λ), and
in a case where λSSL1-RL-max (nm) represents a wavelength that provides a longest wavelength local maximum value of SSSL1(λ) in a wavelength range of 380 nm or more and 780 nm or less, and when a wavelength Δ4 that is represented by SSSL1 (λSSL1-RL-max)/2 exists on a longer wavelength-side of λSSL1-RL-max,
an index Acg (φSSL1 (λ)) represented by the following formula (1-1) satisfies
−10.0<Acg(φSSL1(λ))≤120.0,
but
in a case where λSSL1-RL-max (nm) represents a wavelength that provides the longest wavelength local maximum value of SSSL1(λ) in a wavelength range of 380 nm or more and 780 nm or less, and when the wavelength Λ4 that is represented by SSSL1 (λSSL1-RL-max)/2 does not exist on the longer wavelength-side Of λSSL1-RL-max,
an index Acg (φSSL1(λ)) represented by the following formula (1-2) satisfies
−10.0<Acg(φSSL1(λ))≤120.0;
[Expression 1]
A
cg(ϕSSL1(λ))=∫380495ΔSSSL1(λ)dλ+∫495590(−ΔSSSL1(λ))dλ+∫590Λ4ΔSSSL1(λ)dλ (1- 1)
[Expression 2]
A
cg(ϕSSL1(λ))=∫380495ΔSSSL1(λ)dλ+∫495590(−ΔSSSL1(λ))dλ+∫590780ΔSSSL1(λ)dλ (1-2)
a distance Duv(φSSL1(λ)) of the spectral power distribution φSSL1(λ) of light from a black-body radiation locus defined by ANSI C78.377 satisfies
−0.0220≤Duv(φSSL1(λ))≤−0.0070;
when a maximum value of spectral intensity in a range of 430 nm or more and 495 nm or less is defined as φSSL1-BM-max and a minimum value of spectral intensity in a range of 465 nm or more and 525 nm or less is defined as φSSL1-BG-min, the spectral power distribution φSSL1(λ) of light satisfies
0.2250≤φSSL1-BG-min/φSSL1-BM-max≤0.7000; and
in the spectral power distribution φSSL1(λ) of light, when a maximum value of spectral intensity in a range of 590 nm or more and 780 nm or less is defined as φSSL1-RM-max, a wavelength λSSL1-RM-max that provides φSSL1-RM-max satisfies
605(nm)≤λSSL1-RM-max≤653(nm).
The light-emitting device preferably satisfies, in Condition 2 described above,
−0.0184≤Duv(φSSL1(λ))≤−0.0084.
The light-emitting device preferably satisfies, in Condition 4 described above,
605(nm)≤λSSL1-RM-max≤647(nm).
The light-emitting device preferably satisfies Condition 5 below.
In the spectral power distribution φSSL1(λ) of light described above, a wavelength λSSL1-BM-max that provides φSSL1-BM-max satisfies
430(nm)≤λSSL1-RM-max≤480(nm).
The light-emitting device preferably satisfies Condition 6 below.
0.1800≤φSSL1-BG-min/φSSL1-BM-max≤0.8500; and Condition 6
In addition, the light-emitting device preferably satisfies,
in Condition 6 described above,
0.1971≤φSSL1-BG-min/φSSL1-BM-max≤0.7300; and
In the light-emitting device, a luminous efficacy of radiation KSSL1 (lm/W) in a wavelength range of 380 nm or more and 780 nm or less, which is derived from φSSL1(λ), preferably satisfies Condition 7.
210.0lm/W≤KSSL1≤290.0lm/W. Condition 7
In the light-emitting device, TSSL1 (K) preferably satisfies Condition 8.
2600K≤TSSL1≤7700K. Condition 8
In the light-emitting device, φSSL1(λ) preferably does not have effective intensity derived from the light-emitting element in a range of 380 nm or more and 405 nm or less.
In the light-emitting device, the blue semiconductor light-emitting element is preferably configured such that a dominant wavelength λCHIP-BM-dom of the blue semiconductor light-emitting element alone when pulse-driven is 445 nm or more and 475 nm or less.
In the light-emitting device, the green phosphor is preferably a wide-band green phosphor.
In the light-emitting device, the green phosphor is preferably configured such that a wavelength λPHOS-GM-max that provides maximum emission intensity when light is excited by the green phosphor alone is 511 nm or more and 543 nm or less and a full-width at half-maximum WPHOS-GM-fWhm thereof is 90 nm or more and 110 nm or less.
The light-emitting device preferably includes substantially no yellow phosphor.
In the light-emitting device, the red phosphor is preferably configured such that a wavelength λPHOS-RM-max that provides maximum emission intensity when light is excited by the red phosphor alone is 622 nm or more and 663 nm or less and a full-width at half-maximum WPHOS-RM-fwhm thereof is 80 nm or more and 105 nm or less.
In the light-emitting device, the blue semiconductor light-emitting element is preferably an AlInGaN light-emitting element.
In the light-emitting device, the green phosphor is preferably Ca3 (Sc,Mg)2Si3O12:Ce (CSMS phosphor), CaSc2O4:Ce (CSO phosphor), Lu3Al5O12:Ce (LuAG phosphor), or Y3 (Al, Ga)5O12:Ce (G-YAG phosphor).
In the light-emitting device, the red phosphor preferably includes (Sr,Ca)AlSiN3:Eu (SCASN phosphor), CaAlSi(ON)3:Eu (CASON phosphor), or CaAlSiN3:Eu (CASN phosphor).
In the light-emitting device, preferably, the blue semiconductor light-emitting element is an AlInGaN light-emitting element with a dominant wavelength λCHIP-BM-dom when the blue semiconductor light-emitting element alone is pulse-driven, of 452.5 nm or more and 470 nm or less, the green phosphor is CaSc2O4:Ce (CSO phosphor) or Lu3Al5O12:Ce (LuAG phosphor) with a wavelength λPHOS-GM-max that provides maximum emission intensity when light is excited by the green phosphor alone, of 515 nm or more and 535 nm or less, and a full-width at half-maximum WPHOS-GM-fwhm of 90 nm or more and 110 nm or less, and
the red phosphor is CaAlSi(ON)3:Eu (CASON phosphor) or CaAlSiN3:Eu (CASN phosphor) with a wavelength that provides maximum emission intensity λPHOS-RM-max when light is excited by the red phosphor alone, of 640 nm or more and 663 nm or less, and a full-width at half-maximum WPHOS-RM-fwhm of 80 nm or more and 105 nm or less.
The light-emitting device is preferably a packaged LED, a chip-on-board LED, an LED module, an LED light bulb, an LED lighting fixture, or an LED lighting system.
In the light-emitting device, the light emitted from the light-emitting device in the main radiant direction preferably satisfies Conditions I to IV below.
when a*nSSL1 and b*nSSL1 (where n is a natural number from 1 to 15) respectively denote the a* value and b* value in the CIE 1976 L*a*b* color space of the following 15 Munsell renotation color samples of #01 to #15 based on a mathematical assumption that illumination is performed by the light emitted from the light-emitting device in the main radiant direction, and
when a*nref1 and b*nref1 (where n is a natural number from 1 to 15) respectively denote the a* value and b* value in the CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples based on a mathematical assumption that illumination is performed by reference light which is selected in accordance with the correlated color temperature TSSL1(K) of the light emitted in the main radiant direction, each saturation difference ΔCnSSL1 satisfies
−4.00≤ΔCnSSL1≤8.00(where n is a natural number from1to15);
an average saturation difference represented by the following formula (1-3) satisfies
when a maximum saturation difference value is denoted by ΔCSSL-max1 and a minimum saturation difference value is denoted by ΔCSSL-min1, a difference |ΔCSSL-max1−ΔCSSL-min1| between the maximum saturation difference value and the minimum saturation difference value satisfies
2.00≤|ΔCSSL-max1−ΔCSSL-min1|≤10.00,
where ΔCnSSL1=√{(a*nSSL1)2+(b*nSSL1)2}−√{(a*nref1)2+(b*nref1)2},
with the 15 Munsell renotation color samples being:
and
when θnSSL1 (degrees) (where n is a natural number from 1 to 15) denotes a hue angle in the CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples based on a mathematical assumption that illumination is performed by the light emitted from the light-emitting device in the main radiant direction, and
when θnref1 (degrees) (where n is a natural number from 1 to 15) denotes a hue angle in the CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples based on a mathematical assumption that illumination is performed by reference light which is selected in accordance with the correlated color temperature TSSL1 of the light emitted in the main radiant direction, an absolute value of each difference in hue angles |ΔhnSSL1| satisfies
0.00 degree≤|ΔhnSSL1|≤12.50 degrees (where n is a natural number from 1 to 15),
where ΔhnSSL1=θnSSL1−θnref1.
The light-emitting device is also preferably used as a residential uses' illumination device, an exhibition illumination device, a presentation illumination device, a medical illumination device, a work illumination device, an illumination device incorporated in industrial equipments, an illumination device for interior of transportation, an illumination device for works of art, and an illumination device for aged persons.
A second aspect of the first invention of the present invention is
a method for designing a light-emitting device which at least includes, as light-emitting elements:
a blue semiconductor light-emitting element;
a green phosphor; and
a red phosphor,
the method comprising designing the light-emitting device so that light emitted from the light-emitting device in a main radiant direction satisfies all of Conditions 1 to 4 below. Condition 1:
when λ denotes wavelength, φSSL1(λ) denotes a spectral power distribution of light emitted from the light-emitting device in the main radiant direction,
φref1(λ) denotes a spectral power distribution of reference light which is selected in accordance with a correlated color temperature TSSL1 of the light emitted from the light-emitting device in the main radiant direction,
(XSSL1, YSSL1, ZSSL1) denote tristimulus values of the light emitted from the light-emitting device in the main radiant direction, and
(Xref1, Yref1, Zref1) denote tristimulus values of the reference light which is selected in accordance with TSSL1 of the light emitted from the light-emitting device in the main radiant direction, and
a normalized spectral power distribution SSSL1(λ) of the light emitted from the light-emitting device in the main radiant direction, a normalized spectral power distribution Sref1(λ) of the reference light which is selected in accordance with TSSL1(K) of the light emitted from the light-emitting device in the main radiant direction, and a difference ΔSSSL1(λ) of between normalized spectral power distributions are respectively defined as
S
SSL1(λ)=φSSL1(λ)/YSSL1
S
ref1(λ)=φref1(λ)/Yref1
ΔSSSL1(λ)=Sref1(λ)−SSSL1(λ), and
in a case where λSSL1-RL-max (nm) represents a wavelength that provides a longest wavelength local maximum value of SSSL1(λ) in a wavelength range of 380 nm or more and 780 nm or less, and when a wavelength Λ4 that is represented by SSSL1(λSSL1-RL-max)/2 exists on a longer wavelength-side of λSSL1-RL-max,
an index Acg(φSSL1(λ)) represented by the following formula (1-1) satisfies
−10.0<Acg(φSSL1(λ))≤120.0,
but
in a case where λSSL1-RL-max (nm) represents a wavelength that provides the longest wavelength local maximum value of SSSL1(λ) in a wavelength range of 380 nm or more and 780 nm or less, and when the wavelength Λ4 that is represented by SSSL1(λSSL1-RL-max)/2 does not exist on the longer wavelength-side of λSSL1-RL-max,
an index Acg(φSSL1(λ)) represented by the following formula (1-2) satisfies
−10.0<Acg(φSSL1(λ))≤120.0,
[Expression 5]
A
cg(ϕSSL1(λ))=∫380495ΔSSSL1(λ)dλ+∫495590(−ΔSSSL1(λ))dλ+∫590Λ4ΔSSSL1(λ)dλ (1- 1)
[Expression 6]
A
cg(ϕSSL1(λ))=∫380495ΔSSSL1(λ)dλ+∫495590(−ΔSSSL1(λ))dλ+∫590780ΔSSSL1(λ)dλ (1-2)
a distance Duv(φSSL1(λ)) of the spectral power distribution φSSL1(λ) of light from a black-body radiation locus defined by ANSI C78.377 satisfies
−0.0220≤Duv(φSSL1(λ))≤−0.0070;
when a maximum value of spectral intensity in a range of 430 nm or more and 495 nm or less is defined as φSSL1-BM-max and a minimum value of spectral intensity in a range of 465 nm or more and 525 nm or less is defined as φSSL1-BG-min, the spectral power distribution φSSL1(λ) of light satisfies
0.2250≤φSSL1-BG-min/φSSL1-BM-max≤0.7000; and
in the spectral power distribution φSSL1(λ) of light, when a maximum value of spectral intensity in a range of 590 nm or more and 780 nm or less is defined as φSSL1-RM-max, a wavelength λSSL1-RM-max that provides φSSL1-RM-max satisfies
605(nm)≤λSSL1-RM-max≤653(nm).
The method preferably satisfies, in Condition 2 described above,
−0.0184≤Duv(φSSL1(λ))≤−0.0084.
The method preferably satisfies, in Condition 4 described above,
625(nm)≤λSSL1-RM-max≤647(nm).
The method preferably satisfies Condition 5 below.
In the spectral power distribution φSSL1(λ) of light described above, a wavelength λSSL1-BM-max that provides φSSL1-BM-max satisfies
430(nm)≤λSSL1-RM-max≤480(nm).
The method preferably satisfies Condition 6 below.
0.1800≤φSSL1-BG-min/φSSL1-BM-max≤0.8500. Condition 6
In addition, the method preferably satisfies, in Condition 6 described above,
0.1971≤φSSL1-BG-min/φSSL1-BM-max≤0.7300; and
With a light-emitting device according to the first aspect of the first invention of the present invention, light source efficiency can be improved in “a light-emitting device capable of realizing a natural, vivid, highly visible and comfortable appearance of colors or an appearance of objects” while maintaining favorable color appearance characteristics.
In addition, with a method for designing a light-emitting device according to the second aspect of the first invention of the present invention, design guidelines for “a light-emitting device capable of realizing a natural, vivid, highly visible and comfortable appearance of colors or an appearance of objects” can be provided.
While means for solving the problems will be hereinafter described in detail, important terms used in the present specification are defined as follows.
A concept of the novel invention discovered by the present inventor enables a natural, vivid, highly visible and comfortable appearance of colors and appearance of objects to be realized and improves a light source efficiency of a light-emitting body that realizes a natural, vivid, highly visible and comfortable appearance of colors and appearance of objects.
In other words, the novel invention represents a discovery of a spectral power distribution capable of realizing such an appearance of objects. The three inventions below are provided as specific means for implementing the novel invention described above.
(1) An invention related to a light-emitting device which emits light having a spectral power distribution capable of realizing a natural, vivid, highly visible and comfortable appearance of colors and appearance of objects (first invention)
(2) An invention related to a light-emitting device which emits light having a spectral power distribution capable of realizing a natural, vivid, highly visible and comfortable appearance of colors and appearance of objects and which emits light emitted from a plurality of light-emitting areas (second invention)
(3) An invention related to a light-emitting device which emits light having a spectral power distribution capable of realizing a natural, vivid, highly visible and comfortable appearance of colors and appearance of objects and which includes a control element (third invention)
Therefore, in the present specification, a spectral power distribution φ(λ) of light emitted by a light source may be described using different notations (φSSL1(λ), φSSL2(λ), φSSL3(λ), and φelm3(λ)) in accordance with the respective inventions.
In a similar manner, in the present specification, correlated color temperature T may be described using different notations (TSSL1, TSSL2, TSSL3, and Telm3) in accordance with the respective inventions.
In a similar manner, in the present specification, φref(λ), a spectral power distribution of reference light which is selected in accordance with a correlated color temperature T, may be described using different notations (φref1(λ), φref2(λ), φSSL-ref3(λ), and φelm-ref3(λ)) in accordance with the respective inventions.
In a similar manner, in the present specification, tristimulus values of the light (X, Y, Z) may be described using different notations ((XSSL1, YSSL1, ZSSL1), (XSSL2, YSSL2, ZSSL), (XSSL3, YSSL3, ZSSL3), and (Xelm3, Yelm3, Zelm3)) in accordance with the respective inventions.
In a similar manner, in the present specification, (Xref, Yref, Zref), tristimulus values of the reference light which is selected in accordance with T, may be described using different notations ((Xref1, Yref1, Zref1), (Xref2, Yref2, Zref2), (XSSL-ref3, YSSL-ref3, ZSSL-ref3), and (Xelm-ref3, Yelm-ref3, Zelm-ref3)) in accordance with the respective inventions.
In a similar manner, in the present specification, a normalized spectral power distribution S(λ) may be described using different notations (SSSL1(λ), SSSL2(λ), SSSL3(λ), and Selm3(λ)) in accordance with the respective inventions.
In a similar manner, in the present specification, a normalized spectral power distribution Sref(λ) of the reference light which is selected in accordance with T may be described using different notations (Sref1(λ), Sref2(λ), SSSL-ref3(λ), and Selm-ref3(λ)) in accordance with the respective inventions.
In a similar manner, in the present specification, a difference ΔS(λ) of normalized spectral power distributions may be described using different notations (ΔSSSL1(λ), ΔSSSL2(λ), ΔSSSL3(λ), and ΔSelm3(λ)) in accordance with the respective inventions.
In a similar manner, in the present specification, the below-mentioned wavelength λBG-min may be described using different notations (λSSL1-BG-min, λSSL2-BG-min, λSSL3-BG-min, λSSL3-BG-min, and λelm3-BG-min) in accordance with the respective inventions.
In a similar manner, in the present specification, the below-mentioned wavelength λBM-max may be described using different notations (λSSL1-BM-max, λSSL2-BM-max, λSSL3-BM-max, and λelm3-BM-max) in accordance with the respective inventions.
In a similar manner, in the present specification, the below-mentioned wavelength λRM-max may be described using different notations (λSSL1-RM-max, λSSL2-RM-max, λSSL3-RM-max, and λelm3-RM-max) in accordance with the respective inventions.
In a similar manner, in the present specification, the below-mentioned wavelength λRL-max may be described using different notations (λSSL1-RL-max, λSSL2-RL-max, λSSL3-RL-max, and λelm3-RL-max) in accordance with the respective inventions.
In a similar manner, in the present specification, the below-mentioned φBG-min, a minimum value of spectral intensity in a range of 465 nm or more and 525 nm or less, may be described using different notations (φSSL1-BG-min, φSSL2-BG-min, φSSL3-BG-min, and φelm3-BG-min) in accordance with the respective inventions.
In a similar manner, in the present specification, the below-mentioned φBM-max, maximum value of spectral intensity in a range of 430 nm or more and 495 nm or less, may be described using different notations (φSSL1-BM-max, φSSL2-BM-max, φSSL3-BM-max, and φelm3-BM-max) in accordance with the respective inventions.
In a similar manner, in the present specification, the below-mentioned φRM-max, a maximum value of spectral intensity in a range of 590 nm or more and 780 nm or less, may be described using different notations (φSSL1-RM-max, φSSL2-RM-max, φSSL3-RM-max, and φelm3-RM-max) in accordance with the respective inventions.
In a similar manner, in the present specification, the below-mentioned φRL-max, a longest wavelength local maximum value of a normalized spectral power distribution S(λ) which is derived from the spectral power distribution φ(λ) in a range of 380 nm or more and 780 nm or less may be described using different notations (φSSL1-RL-max, φSSL2-RL-max, φSSL3-RL-max, and φelm3-RL-max) in accordance with the respective inventions.
In a similar manner, in the present specification, the below-mentioned index Acg may be described using different notations (Acg(φSSL1(λ)), Acg(φSSL2(λ)), Acg(φSSL3(λ)), and Acg(φelm3(λ)) in accordance with the respective inventions.
In a similar manner, in the present specification, the below-mentioned distance Duv may be described using different notations (Duv(φSSL1 (λ)), Duv(φSSL2(λ)), Duv(φSSL3(λ)), and Duv(φelm3(λ)) in accordance with the respective inventions.
In a similar manner, in the present specification, the below-mentioned a*n value may be described using different notations (a*nSSL1, a*nSSL2, a*nSSL3, and a*nelm3) in accordance with the respective inventions.
In a similar manner, in the present specification, the below-mentioned b*n value may be described using different notations (b*nSSL1, b*nSSL2, b*nSSL3, and b*nelm3) in accordance with the respective inventions.
In a similar manner, in the present specification, the below-mentioned a*nref value may be described using different notations (a*nref1, a*nref2, a*nSSL-ref3, and a*nelm-ref3) in accordance with the respective inventions.
In a similar manner, in the present specification, the below-mentioned b*nref value may be described using different notations (b*nref1, b*nref2, b*nSSL-ref3, and b*nelm-ref3) in accordance with the respective inventions.
In a similar manner, in the present specification, the below-mentioned hue angle θn may be described using different notations (θnSSL1, θnSSL2, θnSSL3, and θnelm3) in accordance with the respective inventions.
In a similar manner, in the present specification, the below-mentioned hue angle θnref may be described using different notations (θnref1, θnref2, θnSSL-ref3, and θnelm-ref3) in accordance with the respective inventions.
In a similar manner, in the present specification, the below-mentioned each difference in hue angles Δhn may be described using different notations (ΔhnSSL1, ΔhnSSL2, ΔhnSSL3, and Δhnelm3) in accordance with the respective inventions.
In a similar manner, in the present specification, the below-mentioned each saturation difference ΔCn may be described using different notations (ΔCnSSL1, ΔCnSSL2, ΔCnSSL3, and ΔCnelm3) in accordance with the respective inventions.
In a similar manner, in the present specification, the below-mentioned average saturation difference SATave may be described using different notations (SATave(φSSL1(λ)), SATave(φSSL2(λ)), SATave(φSSL3(λ)), and SATave(φelm3(λ)) in accordance with the respective inventions.
In a similar manner, in the present specification, the below-mentioned maximum saturation difference value ΔCmax may be described using different notations (ΔCSSL-max1, ΔCSSL-max2, ΔCSSL-max3, and ΔCelm-max3) in accordance with the respective inventions.
In a similar manner, in the present specification, the below-mentioned minimum saturation difference value ΔCmin may be described using different notations (ΔCSSL-min1, ΔCSSL-min2, ΔCSSL-min3, and ΔCelm-min3) in accordance with the respective inventions.
In a similar manner, in the present specification, the below-mentioned luminous efficacy of radiation K may be described using different notations (KSSL1, KSSL2, KSSL3, and Kelm3) in accordance with the respective inventions.
In a similar manner, in the present specification, the below-mentioned light source efficiency η may be described using different notations (ηSSL1, ηSSL2, ηSSL3, and ηelm3) in accordance with the respective inventions.
The present invention includes the first invention, the second invention, and the third invention described above.
The first invention of the present invention includes an aspect related to the light-emitting device described above (a first aspect of the first invention) as well as an aspect related to a method for designing the light-emitting device (a second aspect of the first invention).
The second invention of the present invention includes an aspect related to the light-emitting device described above (a first aspect of the second invention) as well as an aspect related to a method for designing the light-emitting device (a second aspect of the second invention), an aspect related to a method for driving the light-emitting device (a third aspect of the second invention), and an aspect related to an illumination method (a fourth aspect of the second invention).
The third invention of the present invention includes an aspect related to the light-emitting device described above (a first aspect of the third invention) as well as an aspect related to a method for designing the light-emitting device (a second aspect of the third invention), an aspect related to an illumination method (a fourth aspect of the third invention), and an aspect related to a method for manufacturing the light-emitting device (a fifth aspect of the third invention). It should be noted that a third aspect of the third invention of the present invention will not be described for the sake of convenience.
In addition, in the present specification, examples and the like of the first to third inventions of the present invention and the experimental examples and the like described later have the following relationships.
Examples of the first invention of the present invention are Experimental Example 101 to Experimental Example 152 described later.
Comparative Examples of the first invention of the present invention are Comparative Experimental Example 101 to Comparative Experimental Example 127 described later.
A Reference Example of the first invention of the present invention is Reference Experimental Example 101 described later.
Examples of the second invention of the present invention are Experimental Example 201 to Experimental Example 206 described later.
A Comparative Example of the second invention of the present invention is Comparative Experimental Example 201 described later.
Experimental Examples of the second invention of the present invention are Experimental Example 101 to Experimental Example 152 described later.
Comparative Experimental Examples of the second invention of the present invention are Comparative Experimental Example 101 to Comparative Experimental Example 127 described later.
A Reference experimental Example of the second invention of the present invention is Reference Experimental Example 101 described later.
Examples of the third invention of the present invention are Experimental Example 301 to Experimental Example 303 described later.
A Comparative Example of the third invention of the present invention is Comparative Experimental Example 301 described later.
A Reference Example of the third invention of the present invention is Reference Experimental Example 301 described later.
Reference Comparative Examples of the third invention of the present invention are Reference Comparative Experimental Example 301 to Reference Comparative Experimental Example 302 described later.
Experimental Examples of the third invention of the present invention are Experimental Example 101 to Experimental Example 152 described later.
Comparative Experimental Examples of the third invention of the present invention are Comparative Experimental Example 101 to Comparative Experimental Example 127 described later.
A Reference experimental Example of the third invention of the present invention is Reference Experimental Example 101 described later.
<1. First Invention>
The first invention of the present invention includes an aspect related to a light-emitting device (a first aspect of the first invention) as well as an aspect related to a method for designing the light-emitting device (a second aspect of the first invention).
The light-emitting device according to the first aspect of the first invention of the present invention may be a single semiconductor light-emitting element to which a lead wire or the like as a power supplying mechanism is added, a packaged LED to which a heat radiation mechanism or the like is added and which is integrated with a phosphor or the like, a COB (chip-on-board), and the like. Alternatively, the light-emitting device according to the first aspect of the first invention of the present invention may be an LED module generally mounted with a plurality of packaged LEDs including one or more packaged LEDs to which a further robust heat radiation mechanism has been added. Alternatively, the light-emitting device according to the first aspect of the first invention of the present invention may be an LED light bulb or an LED lighting fixture obtained by adding a lens, a light reflecting mechanism, and the like to a packaged LED or the like. Moreover, a lighting system which supports a large number of LED lighting fixtures or the like and which is configured to be capable of illuminating an object may be adopted. The light-emitting device according to the first aspect of the first invention encompasses all of the above.
<Main Radiant Direction>
The first aspect of the first invention is identified by light in a “main radiant direction” among light emitted by the light-emitting device. Therefore, a light-emitting device capable of emitting light including light in the “main radiant direction” which fulfills the requirement of the first aspect of the first invention belongs to the scope of the first aspect of the first invention.
As used herein, the “main radiant direction” according to the first aspect of the first invention refers to a direction in which light is radiated over a suitable range and in a suitable orientation which are in line with usage of the light-emitting device.
For example, the “main radiant direction” may be a direction in which luminous intensity or luminance of the light-emitting device of the first aspect of the first invention is maximum or locally maximum.
In addition, the main radiant direction of the first aspect of the first invention may be a direction having a finite range including a direction in which the luminous intensity or the luminance of the light-emitting device is maximum or locally maximum.
In addition, the main radiant direction of the first aspect of the first invention may be a direction in which radiant intensity or radiance of the light-emitting device is maximum or locally maximum.
In addition, the main radiant direction of the first aspect of the first invention may be a direction having a finite range including a direction in which the radiant intensity or the radiance of the light-emitting device is maximum or locally maximum.
Specific examples will be given below.
When the light-emitting device of the first aspect of the first invention is an individual light-emitting diode (LED), an individual packaged LED, an individual chip-on-board (COB), an individual LED module, an individual LED bulb, an individual composite lamp constituted by a fluorescent lamp and a semiconductor light-emitting element, an individual composite lamp constituted by an incandescent bulb and a semiconductor light-emitting element, or the like, a main radiant direction may be a vertical direction of each light-emitting device or within a finite solid angle which includes the vertical direction and which ranges between, for example, a maximum of π (sr) and a minimum of π/100 (sr).
When the light-emitting device of the first aspect of the first invention is an LED lighting fixture in which a lens, a reflection mechanism, and the like is added to the packaged LED or the like or a lighting fixture which incorporates a fluorescent lamp and a semiconductor light-emitting element and which has light distribution characteristics applicable to so-called direct lighting use, semi-direct lighting use, general diffused lighting use, direct/indirect lighting use, semi-indirect lighting use, and indirect lighting use, a main radiant direction may be a vertical direction of each light-emitting device or within a finite solid angle which includes the vertical direction and which ranges between, for example, a maximum of π (sr) and a minimum of π/100 (sr). In addition, the main radiant direction may be a direction in which luminous intensity or luminance of the light-emitting device of the first aspect of the first invention is maximum or locally maximum.
Furthermore, the main radiant direction may be within a finite solid angle that includes a direction in which luminous intensity or luminance of the light-emitting device of the first aspect of the first invention is maximum or locally maximum and which ranges between, for example, a maximum of π (sr) and a minimum of π/100 (sr). In addition, the main radiant direction may be a direction in which radiant intensity or radiance of the light-emitting device of the first aspect of the first invention is maximum or locally maximum. Furthermore, the main radiant direction may be within a finite solid angle which includes a direction in which radiant intensity or radiance of the light-emitting device of the first aspect of the first invention is maximum or locally maximum and which ranges between, for example, a maximum of π (sr) and a minimum of π/100 (sr).
When the light-emitting device of the first aspect of the first invention is a lighting system in which a plurality of the LED lighting fixtures or lighting fixtures having a fluorescent lamp is mounted, the main radiant direction may be a vertical direction of a planar center of each light-emitting device or within a finite solid angle which includes the vertical direction and which ranges between, for example, a maximum of π (sr) and a minimum of π/100 (sr).
In addition, the main radiant direction may be a direction in which luminous intensity or luminance of the light-emitting device of the first aspect of the first invention is maximum or locally maximum. Furthermore, the main radiant direction may be within a finite solid angle which includes a direction in which luminous intensity or luminance of the light-emitting device of the first aspect of the first invention is maximum or locally maximum and which ranges between, for example, a maximum of π (sr) and a minimum of π/100 (sr). In addition, the main radiant direction may be a direction in which radiant intensity or radiance of the light-emitting device of the first aspect of the first invention is maximum or locally maximum. Furthermore, the main radiant direction may be within a finite solid angle which includes a direction in which radiant intensity or radiance of the light-emitting device of the first aspect of the first invention is maximum or locally maximum and which ranges between, for example, a maximum of π (sr) and a minimum of π/100 (sr).
The spectral power distribution of light emitted from the light-emitting device in the main radiant direction according to the first aspect of the first invention is preferably measured at a distance where luminance at the measurement is practical luminance such as between 5 lx and 10000 lx.
<Drive Environment>
With the light-emitting device according to the first aspect of the first invention, when drive conditions thereof such as a temperature environment, a level of injected current, and drive modes including intermittent lighting/continuous lighting differ, the spectral power distribution of light emitted from the light-emitting device in the main radiant direction differs in a similar manner to general light-emitting devices. From this perspective, if a light-emitting device is capable of emitting light disclosed in the first aspect of the first invention under at least one specific condition that realistically enables the light-emitting device to emit light, then the light-emitting device is considered a light-emitting device within the scope of the disclosure of the first aspect of the first invention.
<Emission of Light by Single Light-Emitting Element and Emission of Light by Light-Emitting Device>
The light-emitting device according to the first aspect of the first invention may be, for example, a packaged LED including a semiconductor light-emitting element and a phosphor, an LED light bulb including a packaged LED, or a light-emitting module, a light-emitting system, or the like which integrates such light-emitting devices. Hereinafter, a member/material which constitutes the light-emitting device according to the first aspect of the first invention and which is capable of emitting light either spontaneously or as a result of being excited by another member will be described as a light-emitting element. Therefore, in the first aspect of the first invention, a semiconductor light-emitting element, a phosphor, and the like may be light-emitting elements.
Although superimposition of light emitted by light-emitting elements form a basis of light emitted from the light-emitting device in the main radiant direction according to the first aspect of the first invention, various factors prevent the superimposition from being simple and straight forward. For example, reciprocal absorption of light between light-emitting elements is a major factor. In addition, the spectral power distribution of the light-emitting device according to the first aspect of the first invention may significantly change from a simple superimposition of spectral power distributions of light-emitting elements due to spectral transmission characteristics of a lens, a filter, or the like that can be included in the light-emitting device. Furthermore, the spectral power distribution of the light-emitting device may also change from a simple superimposition of spectral power distributions of light-emitting elements due to spectral transmission characteristics of a constituent member such as a reflecting film of the light-emitting device which is positioned in a vicinity of a light-emitting element.
Moreover, consideration must also be given to the fact that the spectral power distribution of the light-emitting element cannot be simply derived from a superimposition of spectral power distributions of light-emitting elements due to a “difference” between a widely-used measurement environment for a single light-emitting element and a general measurement environment of a light-emitting device.
In consideration of the above, light-emitting elements in the light-emitting device according to the first aspect of the first invention are defined as follows.
A purple semiconductor light-emitting element is characterized by a peak wavelength λCHIP-VM-max when the purple semiconductor light-emitting element alone is driven by a pulse current.
A blue semiconductor light-emitting element is characterized by a dominant wavelength λCHIP-BM-dom when the blue semiconductor light-emitting element alone is driven by a pulse current.
A phosphor material is characterized by an emission peak wavelength (denoted by λPHOS-GM-max for a green phosphor and denoted by λPHOS-RM-max for a red phosphor) when light is excited by the material alone and by a full-width at half-maximum (denoted by WPHOS-GM-fwhm for a green phosphor and denoted by WPHOS-RM-fwhm for a red phosphor) of an emission spectral power distribution of the material.
On the other hand, a spectral power distribution φSSL1(λ) of the light-emitting device itself according to the first aspect of the first invention is based on characteristics when power is being continuously supplied thereto and is characterized by the following indexes.
Specifically, the spectral power distribution φSSL1(λ) of the light-emitting device is characterized by a maximum value φSSL1-BM-max of spectral intensity and a wavelength λSSL1-BM-max that provides the maximum value φSSL1-BM-max of spectral intensity in a range of 430 nm or more and 495 nm or less,
a minimum value φSSL1-BG-min of spectral intensity and a wavelength λSSL1-BG-min that provides the minimum value φSSL1-BG-min of spectral intensity in a range of 465 nm or more and 525 nm or less,
a maximum value φSSL1-RM-max of spectral intensity and a wavelength λSSL1-RM-max that provides the maximum value φSSL1-RM-max of spectral intensity in a range of 590 nm or more and 780 nm or less, and
λSSL1-RL-max that provides a longest wavelength local maximum value φSSL1-RL-max of a normalized spectral power distribution SSSL1(λ) which is derived from the spectral power distribution φSSL1(λ) in a range of 380 nm or more and 780 nm or less which is used in the definition of an index Acg (φSSL1(λ)) to be described later. This relationship is shown in
Therefore, for example, λCHIP-BM-dom generally differs from λSSL1-BM-max and λPHOS-RM-max also generally differs from λSSL1-RM-max. On the other hand, λSSL1-RL-max may sometimes assume a same value as λSSL1-RM-max.
<Index Acg(φSSL1(λ))>
The index Acg(φSSL1(λ) is defied as below, as disclosed as the index Acg in Japanese Patent No. 5252107 and Japanese Patent No. 5257538.
Let φref1(λ) and φSSL1(λ) respectively denote spectral power distributions of calculational reference light and test light which represent color stimuli that differ from one another when measuring light emitted in a main radiant direction from a light-emitting device of the first aspect of the first invention, x(λ), y(λ), and z(λ) denote a color-matching function, and (Xref1, Yref1, Zref1) and (XSSL1, YSSL1, ZSSL1) respectively denote tristimulus values corresponding to the calculational reference light and the test light. In this case, the following is satisfied regarding the calculational reference light and the test light, where k denotes a constant.
Y
ref1
=k∫φ
ref1(λ)·y(λ)dλ
Y
SSL1
=k∫φ
SSL1(λ)·y(λ)dλ
At this point, normalized spectral power distributions obtained by normalizing the spectral power distributions of the calculational reference light and the test light by their respective Y were defined as
S
ref1(λ)=φref1(λ)/Yref1and
S
SSL1(λ)=φSSL1(λ)/YSSL1and
and a difference between the normalized reference light spectral power distribution and the normalized test light spectral power distribution was represented by
ΔSSSL1(λ)=Sref1(λ)−SSSL1(λ).
Furthermore, at this point, the index Acg(φSSL1(λ)) was defined as follows.
A
cg(ϕSSL1(λ))=∫Λ1Λ2ΔSSSL1(λ)dλ+∫Λ2Λ3(−ΔSSSL1(λ))dλ+∫Λ3Λ4ΔSSSL1(λ)dλ [Expression 7]
Moreover, upper and lower limit wavelengths of the integrals were respectively set to
Λ1=380 nm,
Λ2=495 nm, and
Λ3=590 nm.
In addition, Λ4 is defined by dividing Λ4 into the two cases described below. First, if a wavelength that provides a longest wavelength local maximum value in a range of 380 nm or more and 780 nm or less in a normalized test light spectral power distribution SSSL1 (λ) is denoted by λSSL1-RL-max (nm) and a normalized spectral intensity thereof is denoted by SSSL1(λSSL1-RL-max), then a wavelength which is on a longer wavelength-side of λSSL1-RL-max and which has an intensity of SSSL1(λSSL1-RL-max)/2 is denoted as Λ4. If such a wavelength does not exist in a range up to 780 nm, then Λ4 is assumed to be 780 nm.
<Narrow-Band/Wide-Band>
A narrow-band light-emitting element according to the first aspect of the first invention shares the same definition as Japanese Patent No. 5252107 and Japanese Patent No. 5257538 and refers to a light-emitting element, the full-width at half-maximum of which is ⅔ or less with respect to 115 nm, 95 nm, and 190 nm which respectively represent region widths of a short wavelength region (380 nm to 495 nm), an intermediate wavelength region (495 nm to 590 nm), and a long wavelength region (590 nm to 780 nm).
Conversely, a wide-band light-emitting element according to the first aspect of the first invention refers to a light-emitting element the full-width at half-maximum of which is wider than ⅔ with respect to 115 nm, 95 nm, and 190 nm which respectively represent region widths of the short wavelength region (380 nm to 495 nm), the intermediate wavelength region (495 nm to 590 nm), and the long wavelength region (590 nm to 780 nm). In other words, generally, a light-emitting element with a full-width at half-maximum of approximately 77 nm or more in the short wavelength region, approximately 64 nm or more in the intermediate wavelength region, and approximately 127 nm or more in the long wavelength region is a wide-band light-emitting element.
<Notation of Chromaticity of Light Source>
Chromaticity points of the light-emitting device according to the first aspect of the first invention are explicitly indicated as follows. Chromaticity derived from a spectral power distribution of light emitted from the light-emitting device in the main radiant direction can be discussed using, for example, the CIE 1931 (x, y) chromaticity diagram or the CIE 1976 (u′, v′) chromaticity diagram. However, since a position on a chromaticity diagram can be described in an easily-understood manner using correlated color temperature CCT and deviation Duv, the (u′, (2/3)v′) chromaticity diagram (synonymous with the CIE 1960 (u, v) chromaticity diagram) is particularly used in the first aspect of the first invention.
Moreover, deviation Duv of the first aspect of the first invention is an amount defined by ANSI C78.377 and represents a distance of closest approach to a black-body radiation locus on a (u′, (2/3)v′) chromaticity diagram as an absolute value thereof. Furthermore, a positive sign means that a chromaticity point of a light-emitting device is above (on a side where v′ is greater than) the black-body radiation locus, and a negative sign means that the chromaticity point of the light-emitting device is below (on a side where v′ is smaller than) the black-body radiation locus.
<φSSL1-BG-min/φSSL1-BM-max and φSSL1-BG-min/φSSL1-BM-max>
φSSL1-BG-min mainly appears in a portion where a longer wavelength-side tail (a base portion where spectral radiant flux intensity decreases) of a spectral radiant flux due to emission of light by a blue semiconductor light-emitting element and a shorter wavelength side tail (a base portion where spectral radiant flux intensity decreases) of a spectral radiant flux due to emission of light by a light-emitting element responsible for the intermediate wavelength region overlap with each other. In other words, φSSL1-BG-min often occurs as a recess with a shape of φSSL1(λ) in a range of 465 nm or more and 525 nm or less which straddles the short wavelength region and the intermediate wavelength region.
In order to relatively uniformly improve saturation of color appearance of the 15 specific mathematically-derived Munsell renotation color samples to be described later, φSSL1-BG-min/φSSL1-BM-max obtained by normalizing φSSL1-BG-min with a maximum value of spectral intensity in a range of 430 nm to 495 nm and φSSL1-BG-min/φSSL1-RM-max obtained by normalizing φSSL1-BG-min with a maximum value of spectral intensity in a range of 590 nm to 780 nm must be controlled with care. In other words, in the light-emitting device according to the first aspect of the first invention, φSSL1-BG-min/φSSL1-BM-max and φSSL1-BG-min/φSSL1-RM-max have optimum ranges as will be described later.
<Reference Light, Experimental Reference Light, and Test Light>
In the first aspect of the first invention, reference light defined by CIE and used in calculations for predicting a mathematical color appearance is described as reference light, reference light for calculation, calculation reference light, and the like. On the other hand, reference light for experiments used in actual visual comparisons such as light of an incandescent bulb having a tungsten filament or the like is described as reference light, reference light for experiment, experimental reference light, and the like. In addition, light with high Ra and high Ri, the color appearance of which is predicted to approach that of reference light such as light from an LED light source including a purple semiconductor light-emitting element and a blue/green/red phosphor is also described as reference light, reference light for experiment, experimental reference light, and the like. Furthermore, light as an object of a mathematical or experimental consideration may sometimes be described as test light in comparison to reference light.
<Method for Quantifying Color Appearance of Illuminated Object>
In order to quantitatively evaluate the color appearance of an object illuminated by light based on the spectral power distribution of the light, a color sample with known mathematical spectral reflection characteristics is defined, a case where illumination by calculation reference light is assumed is compared with a case where illumination by test light is assumed, and a “difference in color appearances” of the color sample is used as an index.
Although test colors used in CRI may generally be considered as options, the color samples R1 to R8 used to derive average color rendition indexes are color samples with intermediate chroma and are therefore unsuitable for discussing saturation of colors with high chroma. In addition, while R9 to R12 are high-chroma color samples, there are not enough samples for a detailed discussion covering a range of all hue angles.
Therefore, it was decided that 15 color samples (one color sample per hue) be selected from color samples which have the highest chroma and which are positioned outermost in a Munsell color circle according to the Munsell renotation color system. Moreover, these are the same color samples used in CQS (Color Quality Scale) (versions 7.4 and 7.5) that is a new color rendition index proposed by NIST (National Institute of Standards and Technology), U.S.A. The 15 color samples used in the first aspect of the first invention will be listed below. In addition, a number assigned for convenience sake are provided before each color sample. Moreover, in the present specification, these numbers will sometimes be represented by n. For example, n=3 signifies “5PB 4/12”. n denotes a natural number from 1 to 15.
In the first aspect of the first invention, from the perspective of deriving various indices, an attempt was made to quantify in what way the color appearance of the 15 color samples listed above changes (or does not change) between a case where the colors are assumed to be illuminated by calculational reference light and a case where the colors are assumed to be illuminated by test light when a color appearance or an object appearance that is as natural, vivid, highly visible, and comfortable as though perceived in an outdoor high-illuminance environment is achieved even in an ordinary indoor illuminance environment, and to extract results of the quantification as a color rendering property that should be attained by a light-emitting device.
Moreover, selection of a color space and selection of a chromatic adaptation formula are also important when quantitatively evaluating color appearance that is mathematically derived from the spectral power distributions described above. In the first aspect of the first invention, CIE 1976 L*a*b* (CIELAB) that is a uniform color space currently recommended by the CIE was used. In addition, CMCCAT2000 (Colour Measurement Committee's Chromatic Adaptation Transform of 2000) was adopted for chromatic adaptation calculation.
Moreover, while the CIELAB color space is a three-dimensional color space, since the first aspect of the first invention mainly focuses chroma and hue, lightness has been omitted in the CIELAB color space according to the first aspect of the first invention and only the a* and b* axes are plotted two-dimensionally. In addition, in the CIELAB color space used when describing experimental examples, comparative experimental examples, and the like according to the first aspect of the first invention, points connected by dotted lines in the drawings represent results when assuming illumination by a calculation reference light and solid lines represent results when assuming illumination by respective test lights.
Furthermore, specifically, quantification related to color appearance is performed as follows. First, when the light-emitting device according to the first aspect of the first invention emits test light in the main radiant direction, the a* values and the b* values of the 15 color samples in the CIE 1976 L*a*b* color space of the test light (related to the light-emitting device according to the first aspect of the first invention) are to be respectively denoted by a*nssL1 and b*nSSL1 (where n is a natural number from 1 to 15), and hue angles of the 15 color samples are to be respectively denoted by θnSSL1 (degrees) (where n is a natural number from 1 to 15). In addition, when mathematically assuming illumination by a calculation reference light (black-body radiation light when lower than 5000 K and CIE daylight when equal to or higher than 5000 K) which is selected in accordance with the correlated color temperature TSSL1 of the test light described above, the a* values and the b* values of the 15 color samples in the CIE 1976 L*a*b* color space are to be respectively denoted by a*nref1 and b*nref1 (where n is a natural number from 1 to 15), and hue angles of the 15 color samples are to be respectively denoted by θnref1 (degrees) (where n is a natural number from 1 to 15). In this case, an absolute value |ΔhnSSL1| of each difference in hue angles ΔhnSSL1 (degrees) (where n is a natural number from 1 to 15) of each of the 15 Munsell renotation color samples when illuminated by the two types of light may be represented by
|ΔhnssL1|=|θnSSL1−θnref1|.
A mathematically-predicted each difference in hue angles related to the 15 Munsell renotation color samples particularly selected in the first aspect of the first invention are defined as described above because the present inventor considers each difference in hue angles to be an important index as means for comprehensively evaluating various objects and color appearances of the objects when conducting visual experiments using test light and experimental reference light or experimental pseudo-reference light and for realizing a natural, vivid, highly visible and comfortable appearance of colors and appearance of objects.
In addition, each saturation difference ΔCnSSL1 (where n is a natural number from 1 to 15) of the 15 Munsell renotation color samples when assuming illumination by the test light and the calculation reference light is represented by
ΔCnSSL1=√{(a*nSSL1)2+(b*nSSL1)2}−√{(a*nref1)2+(b*nref1)2}.
Furthermore, an average saturation difference of the 15 Munsell renotation color samples is represented by
(hereinafter, may be denoted as SATave(φSSL1(λ)). Moreover, when a maximum saturation difference value of the 15 Munsell renotation color samples is denoted by ΔCSSL-max1 and a minimum saturation difference value is denoted by ΔCSSL-min1, a difference between a maximum saturation difference and a minimum saturation difference (difference among differences between maximum and minimum degrees of saturation) is represented by
|ΔCSSL-max1−ΔCSSL-min1|.
Various characteristics related to mathematically-predicted saturation differences of the 15 Munsell renotation color samples particularly selected in the first aspect of the first invention are defined as described above because the present inventor considers these characteristics to be important indexes as means for comprehensively evaluating various objects and color appearances of the objects when conducting visual experiments using test light and experimental reference light or experimental pseudo-reference light and for realizing a natural, vivid, highly visible and comfortable appearance of colors and appearance of objects.
<Luminous Efficacy of Radiation KssL1 (Lm/W) and Luminous Efficacy of a Source ηssL1 (Lm/W)>
Furthermore, when evaluating the test light spectral power distribution φSSL1(λ) when measuring light emitted in a main radiant direction from a light-emitting device of the first aspect of the first invention, the widely-used definition below was adopted for luminous efficacy of radiation KSSL1 (lm/W).
K
SSL1
=Km×[∫380780{ϕSSL1(λ)×V(λ)}dλ]/[∫380780ϕSSL1(λ)dλ] [Expression 9]
In the equation above,
Km: maximum luminous efficacy(lm/W),
V(λ): spectral luminous efficiency, and
λ: wavelength (nm).
Therefore, a luminous efficacy of radiation KSSL1 (lm/W) of a test light spectral power distribution φSSL1 (λ) when measuring light in the main radiant direction emitted from the light-emitting device according to the first aspect of the first invention can be described as efficiency inherent in the shape of the spectral power distribution.
On the other hand, light source efficiency ηSSL1 (lm/W) is a quantity indicating how much of power supplied to the light-emitting device according to the first aspect of the first invention is converted into a luminous flux.
Furthermore, the luminous efficacy of radiation KSSL1 (lm/W) of a test light spectral power distribution φSSL1(λ) when measuring light in the main radiant direction emitted from the light-emitting device is efficiency inherent in the shape of the spectral power distribution itself and may be described as a quantity that equals light source efficiency ηSSL1 (lm/W) when assuming that characteristics of all materials constituting the light-emitting device (for example, internal quantum efficiency of semiconductor light-emitting elements, light extraction efficiency, internal quantum efficiency of phosphors, external quantum efficiency of phosphors, and efficiency related to light transmission characteristics of encapsulants) have 100% efficiency.
<Conception of Invention>
The present inventor mathematically and experimentally considered whether or not both favorable color appearance and high light source efficiency can be achieved when the index Acg (φSSL1(λ)) has a value outside a range of −360 or more and −10 or less and, particularly, a value larger than −10.
The index Acg (φSSL1(λ)) is an index used when a visible range related to radiation that acts as color stimuli is roughly divided into a short wavelength region (380 nm or more and less than 495 nm in a blue region including purple and the like), an intermediate wavelength region (495 nm or more and less than 590 nm in a green region including yellow and the like), and a long wavelength region (590 nm or more and 780 nm or less in a red region including orange and the like) to perform a comparison with mathematical normalized reference light spectral power distributions to determine whether or not irregularities in a spectral power distribution exist at an appropriate intensity at appropriate positions in the normalized reference light spectral power distributions. As illustrated in
As disclosed as the index Acg in Japanese Patent No. 5252107 and Japanese Patent No. 5257538, a requirement for realizing “a light-emitting device capable of realizing a natural, vivid, highly visible and comfortable appearance of colors and appearance of objects” is that the index Acg (φSSL1(λ)) is within a range of −360 or more and −10 or less. These can be understood as follows.
In the short wavelength range, a first term of Acg(φSSL1(λ)) (an integral of ΔSSSL1(λ)) is more likely to have a negative value when a distribution intensity of the normalized test light spectral power distribution is higher than that of the mathematically normalized reference light spectral power distribution.
In the intermediate wavelength range, conversely, a second term of Acg(φSSL1(λ)) (an integral of −ΔSSSL1(λ)) is more likely to have a negative value when a distribution intensity of the normalized test light spectral power distribution is lower than that of the normalized reference light spectral power distribution.
Furthermore, in the long wavelength range, a third term of Acg(φSSL1 (λ)) (an integral of ΔSSSL1(λ)) is more likely to have a negative value when a distribution intensity of the normalized test light spectral power distribution is higher than that of the normalized reference light spectral power distribution.
In other words, it can be understood that one of the requirements for realizing “a light-emitting device capable of realizing a natural, vivid, highly visible and comfortable appearance of colors and appearance of objects” is fulfilled when such a tendency exists.
Moreover, as described earlier, the calculation reference light changes depending on CCT of test light. In other words, black-body radiator is used as the calculational reference light when the CCT of the test light is lower than 5000 K, and defined CIE daylight is used as the calculational reference light when the CCT of the test light is equal to or higher than 5000 K. When deriving a value of Acg(φSSL1(λ)), mathematically defined black-body radiation light or CIE daylight is used for φref1(λ) and a simulated function or a value obtained by measuring light emitted in a main radiant direction by a prototype light-emitting device in an experiment is used as φSSL1(λ).
On the other hand, in order to improve light source efficiency of a light source, a substantially different shape from the spectral power distributions disclosed in Japanese Patent No. 5252107 and Japanese Patent No. 5257538 is required when also considering a shape of spectral luminous efficiency V(λ).
With respect to a first term (a wavelength integration of ΔSSSL1(λ) from 380 nm to 495 nm) and a third term (a wavelength integration of ΔSSSL1(λ) from 590 nm to Λ4 or 780 nm) of the index Acg(φSSL1(λ)), desirably, spectral intensity of the normalized test light spectral power distribution is not excessively stronger than that of the normalized reference light spectral power distribution or, in other words, the wavelength integration of ΔSSSL1(λ) does not assume an excessively negative value and is within an appropriate range. This is due to the fact that, since V(λ) in these regions has a relatively small value, a contribution of V(λ) towards improving luminous flux is small even if excessively strong radiation exists in these regions. In addition, in terms of improving light source efficiency, with respect to a second term (a wavelength integration of −ΔSSSL1(λ) from 495 nm to 590 nm) of the index Acg(φSSL1(λ)), spectrum intensity of the normalized test light spectral power distribution is not excessively weaker than that of the normalized reference light spectral power distribution or, in other words, the wavelength integration of −ΔSSSL1(λ) does not assume an excessively negative value and is within an appropriate range. This is due to the fact that, since V(λ) in this region has a relatively large value, the contribution of V(λ) towards improving luminous flux is reduced if excessively weak radiation exists in this region.
In consideration thereof, based on the ideas discussed above, the present inventor examined whether or not a light source with higher light source efficiency and superior color appearance of illuminated objects can be realized by a spectral power distribution that completely differs from the disclosed contents of Japanese Patent No. 5252107 and Japanese Patent No. 5257538, and arrived at the light-emitting device according to the first aspect of the first invention. A specific method used is as follows.
First, as a light-emitting element that emits light in the intermediate wavelength region, a wide-band light-emitting element which differs from the narrow-band light-emitting elements disclosed as preferable cases in Japanese Patent No. 5252107 and Japanese Patent No. 5257538 was selected. It was thought that making such a selection reduces “excessive irregularities in the normalized test light spectral power distribution as compared with the normalized reference light spectral power distribution” in the intermediate wavelength region and prevents the spectrum intensity of the normalized test light spectral power distribution from becoming excessively weaker than that of the normalized reference light spectral power distribution in the second term (a wavelength integration of −ΔSSSL1(λ) from 495 nm to 590 nm) of the index Acg(φSSL1(λ)).
In addition, the selection of a phosphor-exciting light source in an LED light-emitting device was also made with the intention of reducing “excessive irregularities in the normalized test light spectral power distribution as compared with the normalized reference light spectral power distribution” in the short wavelength region and preventing the first term (a wavelength integration of ΔSSSL1(λ) from 380 nm to 495 nm) of the index Acg(φSSL1(λ)) from taking an excessively negative value. In other words, in order to prevent the spectrum intensity of the normalized test light spectral power distribution from becoming excessively stronger than that of the normalized reference light spectral power distribution, an emission wavelength of the phosphor-exciting light source was arranged in a region where the spectral intensity of the normalized reference light spectral power distribution is relatively high. Specifically, a blue semiconductor light-emitting element was selected as the phosphor-exciting light source instead of a purple semiconductor light-emitting element.
<Method and Conclusion of Experiment>
An experiment for completing the light-emitting device according to the first aspect of the first invention was performed and concluded as follows.
As the light-emitting device, a packaged LED was prepared by including various semiconductor light-emitting elements, various phosphors, an encapsulant, and the like in a small square package measuring 3.5 mm×3.5 mm. A prototype of an LED lamp including the packaged LED was also made.
In order to ensure fair comparisons of the various prototype light-emitting devices, although the various semiconductor light-emitting elements, various phosphors, and compositions thereof were altered for each device, all of the light sources used the same small package material, mounting positions/methods of the semiconductor light-emitting elements, LED lamp shape/material, and the like. In addition, the LED lamps were mounted with lenses made of a material with flat transmission characteristics from 350 nm to around 800 nm in order to preserve the spectral radiation characteristics of the packaged LEDs included in the LED lamps to the greatest extent feasible.
Under such conditions, a radiometric property and a photometric property of each light-emitting device were measured. In addition, the color appearance of the 15 Munsell renotation color samples described above when assuming illumination by light having the spectral power distribution of each light-emitting device was compared with the color appearance of the 15 Munsell renotation color samples when assuming illumination by calculation reference light to mathematically derive how the color appearance changes (or does not change) from a colorimetric perspective, and the color appearance was quantitatively evaluated using the indexes described earlier.
Furthermore, in the experiment of the first aspect of the first invention, a comparative visual experiment was also conducted in which test subjects were asked to determine superiority or inferiority of color appearance. In the comparative visual experiment, an experimental reference light was prepared for each color temperature group shown in Table 1-1 by referring to ANSI C78.377, a same illuminated object was respectively independently illuminated by test light and the experimental reference light, and the test subjects were asked to classify which of the lights illuminated the illuminated object so as to produce a more superior color appearance into 11 categories including rank −5, rank −4, rank −3, rank −2, rank −1, rank 0, rank +1, rank +2, rank +3, rank +4, and rank +5.
In this case, as the experimental reference light, a light-emitting device having chromaticity coordinates as close to a black-body locus as possible was prepared. The light-emitting device for emitting experimental reference light was configured as shown in, for example, Comparative Experimental Example 101 using a purple semiconductor light-emitting element with an emission peak wavelength of 410 nm when emitting light by itself, an SBCA phosphor as a blue phosphor, a β-SiAlON phosphor with a peak wavelength of 545 nm and a full-width at half-maximum of 55 nm during light excitation as a narrow-band green phosphor, and a CASON phosphor with a peak wavelength of 645 nm and a full-width at half-maximum of 99 nm during light excitation as a red phosphor so as to prepare light with a high Ra and a high Ri which conceivably produces color appearance approaching a mathematical reference light. For example, spectral radiation characteristics shown in Comparative Experimental Example 101 are an example of the experimental reference light of group E when classified according to CCT during the comparative visual experiment. The calculated CCT was 4116 K, Duv was −0.0017, and Ra was 98.0. Moreover, for the other CCT groups, a light-emitting device which has chromaticity coordinates as close to a black-body locus as possible and which emits light with a high Ra and a high Ri that conceivably produces color appearance approaching a mathematical reference light when illuminating an illuminated object was similarly prepared.
When conducting the comparative visual experiment, in order to suppress changes in luminance due to switching light-emitting devices, distances between the illuminated objects and the light-emitting devices were adjusted, drive power supplies were changed to adjust an amount of current supplied to the LED lamps, and the like so that luminance at the positions of the illuminated objects was approximately the same. In addition, luminance during the comparative visual experiment was set to a range of approximately 100 lx to approximately 7000 lx.
In addition, the following illuminated objects and the like were prepared for the comparative visual experiment. Due consideration was given to preparing chromatic objects so that colors of all hues including purple, bluish purple, blue, greenish blue, green, yellowish green, yellow, reddish yellow, red, and reddish purple were represented. In addition, these objects were prepared in wide varieties and in large numbers including still objects, flowers, food, clothing, and printed material. Furthermore, the skins of the subjects (Japanese) themselves were also included in the experiment as observation objects. Moreover, the color names partially added to the object names listed below simply signify that such objects will appear in such colors in ordinary environments and are not accurate representations of the colors.
White ceramic plate, white asparagus, white mushroom, white preserved flower, white handkerchief, white dress shirt, white rice
Purple preserved flower
Bluish purple cloth handkerchief, blue jeans, blue preserved flower, greenish blue towel
Green bell pepper, lettuce, shredded cabbage, broccoli, green lime, green apple
Yellow banana, yellow bell pepper, greenish yellow lemon, yellow preserved flower, fried egg
Orange orange, orange bell pepper, carrot
Red tomato, red apple, red bell pepper, red sausage, red preserved flower
Black preserved flower
Pink necktie, pink preserved flower
Russet necktie, croquette, pork cutlet, burdock, cookie, chocolate, peanut, woodenware
Skin of subjects (Japanese)
Newspaper, color printed matter including black letters on white background (polychromatic), paperback, weekly magazine
Silver watch (white dial-plate)
Color checkers (Color checker classic manufactured by X-Rite; total of 24 color samples including 18 chromatic colors and six achromatic colors (one white, four grey, and one black)).
Moreover, names and Munsell notations of the respective color samples in the color checker are as follows.
Rankings obtained by the comparative visual experiment were statistically processed based on the results of classifications by the test subjects as follows. Cases where the result was the same as or comparable with the experimental reference light or when there was no perceptible change were classified as rank 0. In addition, when “a natural, vivid, highly visible and comfortable appearance of colors and appearance of objects were realized”, cases where the result was slightly favorable were classified as rank +1, cases where the result was favorable were classified as rank +2, cases where the result was more favorable were classified as rank +3, cases where the result was extremely favorable were classified as rank +4, and cases where the result was dramatically favorable were classified as rank +5. Conversely, when “a natural, vivid, highly visible and comfortable appearance of colors and appearance of objects were not realized”, depending on degrees of the results, cases where the result was slightly unfavorable were classified as rank −1, cases where the result was unfavorable were classified as rank −2, cases where the result was more unfavorable were classified as rank −3, cases where the result was extremely unfavorable were classified as rank −4, and cases where the result was dramatically unfavorable were classified as rank −5.
When determining the ranks, the test subjects were instructed to observe and comprehensively grade the illuminated objects from the following perspectives. Specifically, when the illuminated objects were illuminated by the respective light-emitting devices in comparison with being illuminated by the experimental reference light, A) whether or not “achromatic color appearances” such as black and white are favorably perceived, B) whether or not characters used on printed matter, newspapers, and the like including black letters on a white background are readily legible, C) whether or not “chromatic color appearances” having various hues including a test subject's own skin color are favorably perceived, D) whether or not colors of objects having similar hues (for example, two red bell peppers as different individual objects) are readily distinguishable, and E) whether or not increased brightness can be perceived (whether or not a sense of brightness increases) at the same luminance.
Moreover, among the various indexes organized in Tables 1-2 to 1-15 presented below, fields with the description “light-emitting element” indicate characteristics of single light-emitting elements as described above while fields with the description “light-emitting device” represent results of measurements as a packaged LED. Fields with the description “color appearance” represent results obtained by calculation from a spectral power distribution of the packaged LEDs and fields with the description “comparative visual experiment result” represent results of classification related to the color appearance of the illuminated objects during the comparative visual experiment using LED lamps containing the packaged LEDs.
Hereinafter, while the first invention of the present invention will be described in detail using the examples and the comparative examples, it is needless to say that the scope of the first invention of the present invention is not limited to the experimental examples and the like presented below.
<Overview>
First, an overview and effects of the first aspect of the first invention will be described using the four types of light-emitting devices shown in Table 1-2 as an example.
Comparative Experimental Example 101 used a light-emitting device which produced a color appearance approaching reference light when illuminating the illuminated objects, which emitted experimental reference light with an extremely high average color rendition index (Ra) and a high special color rendition index (Ri), and of which Acg (φSSL1(λ)) was +64.1. The light source was realized by using a purple semiconductor light-emitting element as a phosphor-exciting light source and a narrow-band β-SiAlON (with a wavelength providing maximum emission intensity when light is excited by a phosphor alone of 545 nm and a full-width at half-maximum of 55 nm) as a green phosphor.
Moreover, details of the SBCA phosphor, the β-SiAlON phosphor, and the CASON phosphor described in the present specification are the same as the materials disclosed in Japanese Patent No. 5252107 and Japanese Patent No. 5257538.
Comparative Experimental Example 102 used a light-emitting device which emitted the light disclosed in Japanese Patent No. 5252107 and Japanese Patent No. 5257538 and of which Acg(φSSL1(λ)) was −44.9. In a similar manner to Comparative Experimental Example 101, this light source was also realized by using a purple semiconductor light-emitting element as a phosphor-exciting light source and a narrow-band β-SiAlON (with a wavelength providing maximum emission intensity when light is excited by a phosphor alone of 545 nm and a full-width at half-maximum of 55 nm) as a green phosphor.
Reference Experimental Example 101 also used a light-emitting device which emitted light within the scopes of Japanese Patent No. 5252107 and Japanese Patent No. 5257538 and of which Acg(φSSL1(λ)) was −58.7. However, this light source was realized by using a blue semiconductor light-emitting element as a phosphor-exciting light source and a wide-band CSMS (with a wavelength providing maximum emission intensity when light is excited by a phosphor alone of 514 nm and a full-width at half-maximum of 106 nm) as a green phosphor.
Meanwhile, Experimental Example 101 used a novel light-emitting device which emitted light disclosed in neither Japanese Patent No. 5252107 nor Japanese Patent No. 5257538 and of which Acg(φSSL1(λ)) was +10.4. This light source was realized by using a blue semiconductor light-emitting element as a phosphor-exciting light source and a wide-band CSO (with a wavelength providing maximum emission intensity when light is excited by a phosphor alone of 520 nm and a full-width at half-maximum of 96 nm) as a green phosphor.
Moreover, for purposes of comparison, these four light-emitting devices were all given correlated color temperatures (approximately 3800 to 4200 K) that are close to one another. In addition, with the exception of the light-emitting device of Comparative Experimental Example 101 which was prepared as experimental reference light, Duv(φSSL1(λ)) also had values close to one another (approximately −0.0100 to −0.0125).
Furthermore, details of constituent materials and characteristics thereof of each light source and characteristics as light-emitting devices were as summarized in Table 1-2. Table 1-2 also shows mathematically-derived results of differences between cases where the 15 specific Munsell renotation color samples were illuminated by reference light and cases where the 15 specific Munsell renotation color samples were illuminated by respective test lights. Table 1-2 further shows a result of the comparative visual experiment conducted with the light-emitting device of Comparative Experimental Example 101 which was prepared as experimental reference light as a reference and using the remaining three light-emitting devices to assess actual color appearances.
Respective spectral radiant flux characteristics of the light-emitting device of Comparative Experimental Example 101, the light-emitting device of Comparative Experimental Example 102, the light-emitting device of the Reference Experimental Example 101, and the light-emitting device of the Experimental Example 101 are shown in
Table 1-2,
With the light-emitting device in Comparative Experimental Example 102, the index Acg(φSSL1(λ)) was −44.9 and light source efficiency ηSSL1 as a light-emitting device was 45.9 (lm/W). In addition, from a mathematical perspective,
Furthermore, with the light-emitting device in Reference Experimental Example 101, the index Acg(φSSL1(λ)) was −58.7 and light source efficiency ηSSL1 as a light-emitting device was 48.0 (lm/W). In addition, from a mathematical perspective,
In comparison, with the light-emitting device shown in Experimental Example 101, the index Acg(φSSL1(λ)) was +10.4. Light source efficiency ηSSL1 as a light-emitting device was 54.4 (lm/W), which was relatively higher than both light-emitting devices. In addition, from a mathematical perspective,
In other words, the result of the light-emitting device of Experimental Example 101 can be described as illustrating, in concrete terms, that even when outside of the scopes of the light-emitting devices according to Japanese Patent No. 5252107 and Japanese Patent No. 5257538 and, in particular, even when the index Acg (φSSL1 (λ)) has a larger value than −10, there may be cases where “a light-emitting device capable of realizing a natural, vivid, highly visible and comfortable appearance of colors and appearance of objects” can be realized. Furthermore, it is shown that, precisely in such cases, the light source efficiency ηSSL1 of the light-emitting device may be improved.
<Detailed Description 1>
Next, the first aspect of the first invention will be described in detail by further illustrating experimental examples/comparative experimental examples.
Tables 1-3 to 1-7 show experimental examples of the first aspect of the first invention. The tables represent, in the order of table numbers, results of light-emitting devices graded rank +1 to rank +5 by the comprehensive rank classification of the comparative visual experiment. In addition, light-emitting devices classified in one rank have been sorted in order from low TSSL1 to high TSSL1. Furthermore,
A detailed examination of the results of the experimental examples/comparative experimental examples reveals that, when the color appearance due to illumination by a light-emitting device was determined to be +1 or higher in the comparative visual experiment, the light-emitting device included the following light-emitting elements.
Meanwhile, it is revealed that, when the color appearance due to illumination by a light-emitting device was determined to be +1 or higher in the comparative visual experiment, the various indexes derived from the spectral power distribution φSSL1(λ) of the light-emitting device included all of the following characteristics.
Furthermore, it is revealed that the spectral power distribution φSSL1(λ) of a light-emitting device determined to have a rank of +1 or higher in the comparative visual experiment also had the following characteristics.
Moreover, it is revealed that luminous efficacy of radiation KSSL1 (lm/W) and correlated color temperature TSSL1 (K) derived from the spectral power distribution φSSL1 (λ) of a light-emitting device determined to have a rank of +1 or higher in the comparative visual experiment may have the following characteristics.
In addition, it is revealed that the spectral power distribution φSSL1(λ) of a light-emitting device determined to have a rank of +1 or higher in the comparative visual experiment characteristically does not have effective intensity derived from a light-emitting element in a range of 380 nm or more and 405 nm or less.
Furthermore, it is revealed that φSSL1(λ) of the light-emitting device determined to have a rank of +1 or higher in the comparative visual experiment characteristically does not include a narrow-band green phosphor and a yellow phosphor as light-emitting elements.
Meanwhile, it is revealed that, when the color appearance due to illumination by a light-emitting device was determined to be +1 or higher in the comparative visual experiment, the various indexes related to “color appearance” derived from the spectral power distribution φSSL1(λ) of the light-emitting device included all of the following characteristics, where n is a natural number from 1 to 15.
Results of calculating color appearance based on the spectral power distribution φSSL1(λ) of the light-emitting devices satisfying the above or, in other words,
To further specifically describe the effects of color appearance, it was confirmed that using the light-emitting device according to the first aspect of the first invention for illumination produced the effects of A) favorably perceiving “achromatic color appearances” such as black and white, B) perceiving characters used on printed matter, newspapers, and the like including black letters on a white background to be readily legible, C) favorably perceiving “chromatic color appearances” having various hues including a test subject's own skin color, D) perceiving colors of objects having similar hues to be readily distinguishable, and E) perceiving increased brightness even at the same luminance as compared to illumination by reference light.
Furthermore, the selection of a blue semiconductor light-emitting element described in Condition a is conceivably characterized as follows when considering the results classified into ranks +1 to +5.
A dominant wavelength λCHIP-BM-dom of the blue light-emitting element alone when pulse-driven can be selected from a range of 445 nm or more and 475 nm or less,
based on the results of all experimental examples, slightly favorably selected from a range of 447.5 nm or more and 470 nm or less,
based on the results of ranks +4 and +5, extremely favorably selected from a range of 452.5 nm or more and 470 nm or less, and
based on the result of rank +5, dramatically favorably selected from a vicinity of 457.5 nm.
In this case, a vicinity refers to ±2.5 nm.
Furthermore, the selection of a wide-band green phosphor described in Condition β is conceivably characterized as follows when considering the results classified into ranks +1 to +5.
A wavelength λPHOS-GM-max of the wide-band green phosphor that provides maximum emission intensity when light is excited by a phosphor alone is 511 nm or more and 543 nm or less and a full-width at half-maximum WPHOS-GM-fWhm thereof can be selected from a range of 90 nm or more and 110 nm or less,
based on the results of all experimental examples, slightly favorably, the wavelength λPHOS-GM-max that provides maximum emission intensity when light is excited by a phosphor alone is 514 nm or more and 540 nm or less and the full-width at half-maximum WPHOS-GM-fwhm thereof is selected from a range of 96 nm or more and 108 nm or less,
based on the results of ranks +2 to +5, favorably, the wavelength λPHOS-GM-max that provides maximum emission intensity when light is excited by a phosphor alone is 520 nm or more and 540 nm or less and the full-width at half-maximum WPHOS-GM-fwhm thereof is selected from a range of 96 nm or more and 108 nm or less, and
based on the result of rank +5, dramatically favorably, the wavelength λPHOS-GM-max that provides maximum emission intensity when light is excited by a phosphor alone is 520 nm or more and 530 nm or less and the full-width at half-maximum WPHOS-GM-fwhm thereof is selected from a range of 96 nm or more and 104 nm or less.
Furthermore, based on an overall trend, further dramatically favorably, the wavelength λPHOS-GM-max that provides maximum emission intensity when light is excited by the phosphor alone is 521 nm or more and 529 nm or less and the full-width at half-maximum WPHOS-GM-fwhm thereof is selected from a range of 97 nm or more and 103 nm or less.
These are trends that are conceivably required by the light-emitting device according to the first aspect of the first invention to have irregularities of appropriate sizes at appropriate positions of the spectral power distribution φSSL1(λ).
Moreover, specific phosphor materials are conceivably characterized as follows when considering the results classified into ranks +1 to +5.
While the green phosphor is not particularly limited as long as the green phosphor emits green light when light is excited by a phosphor alone and satisfies the optical characteristics described above, examples of the green phosphor include a LuAG phosphor, a CSO phosphor, a G-YAG phosphor, a CSMS phosphor, a BSS phosphor, and a BSON phosphor,
based on results of all experimental examples, a LuAG phosphor, a CSO phosphor, a G-YAG phosphor, or a CSMS phosphor is slightly favorably selected,
based on the results of ranks +2 to +5, a LuAG phosphor, a CSO phosphor, or a G-YAG phosphor is favorably selected, and
based on the result of rank +5, a LuAG phosphor or a CSO phosphor is dramatically favorably selected.
Furthermore, the selection of a red phosphor described in Condition γ is conceivably characterized as follows when considering the results classified into ranks +1 to +5.
A wavelength λPHOS-RM-max of the red phosphor that provides maximum emission intensity when light is excited by a phosphor alone is 622 nm or more and 633 nm or less and a full-width at half-maximum WPHOS-RM-fWhm thereof can be selected from a range of 80 nm or more and 105 nm or less,
based on the results of all experimental examples, slightly favorably, the wavelength λPHOS-RM-max that provides maximum emission intensity when light is excited by a phosphor alone is 625 nm or more and 660 nm or less and the full-width at half-maximum WPHOS-GM-fwhm thereof is selected from a range of 87 nm or more and 99 nm or less,
based on the results of ranks +4 to +5, extremely favorably, the wavelength λPHOS-RM-max that provides maximum emission intensity when light is excited by a phosphor alone is 645 nm or more and 660 nm or less and the full-width at half-maximum WPHOS-GM-fwhm thereof is selected from a range of 88 nm or more and 99 nm or less, and
based on the result of rank +5, dramatically favorably, the wavelength λPHOS-RM-max that provides maximum emission intensity when light is excited by a phosphor alone is 645 nm or more and 660 nm or less and the full-width at half-maximum WPHOS-RM-fwhm thereof is selected from a range of 88 nm or more and 89 nm or less.
In addition, based on an overall trend, conceivably favorably, the wavelength λPHOS-RM-max that provides maximum emission intensity when light is excited by the phosphor alone is 632 nm or more and 660 nm or less and the full-width at half-maximum WPHOS-RM-fwhm thereof is selected from a range of 88 nm or more and 99 nm or less.
Moreover, specific phosphor materials are conceivably characterized as follows when considering the results classified into ranks +1 to +5.
While the red phosphor is not particularly limited as long as the red phosphor emits red light when light is excited by a phosphor alone and satisfies the optical characteristics described above, examples of the red phosphor include a CASN phosphor, a CASON phosphor, and a SCASN phosphor,
based on results of all experimental examples, a CASN phosphor, a CASON phosphor, or a SCASN phosphor is slightly favorably selected,
based on the results of ranks +4 to +5, a CASN phosphor, or a CASON phosphor is extremely favorably selected, and
based on the result of rank +5, a CASN phosphor is dramatically favorably selected.
Furthermore, the selection of an index Acg (φSSL1(λ) described in Condition 1 is conceivably characterized as follows when considering the results classified into ranks +1 to +5.
An index Acg(φSSL1(λ) can be selected from a range of more than −10.0 and 120.0 or less,
based on the results of all experimental examples, slightly favorably, the index is −4.6 or more and 116.3 or less,
based on the results of ranks +3 to +5, more favorably, the index is −4.6 or more and 87.7 or less,
based on the results of ranks +4 to +5, extremely favorably, the index is −4.6 or more and 70.9 or less, and
based on the result of rank +5, dramatically favorably, the index is −1.5 or more and 26.0 or less.
Furthermore, the selection of a Duv(φSSL1(λ)) described in Condition 2 is conceivably characterized as follows when considering the results classified into ranks +1 to +5.
A distance D (φSSL1(λ)) can be selected from a range of −0.0220 or more and −0.0070 or less,
based on the results of all experimental examples, slightly favorably, the distance Duv (φSSL1(λ)) is −0.0212 or more and −0.0071 or less,
based on the results of ranks +3 to +5, more favorably, the distance Duv (φSSL1(λ)) is −0.0184 or more and −0.0084 or less,
based on the results of ranks +4 to +5, extremely favorably, the distance Duv(φSSL1(λ)) is −0.0161 or more and −0.0084 or less, and
based on the result of rank +5, dramatically favorably, the distance Duv(φSSL1(λ)) is −0.0145 or more and −0.0085 or less.
Moreover, based on an overall trend, Duv (φSSL1(λ)) is further dramatically favorably selected from a range of −0.0145 or more and −0.0090 or less, even more dramatically favorably selected from a range of −0.0140 or more and less than −0.0100, and still even more dramatically favorably selected from a range of −0.0135 or more and less than −0.0120.
Furthermore, the selection of a value of φSSL1-BG-min/φSSL1-BM-max described in Condition 3 is conceivably characterized as follows when considering the results classified into ranks +1 to +5.
A value of φSSL1-BG-min/φSSL1-BM-max can be selected from a range of 0.2250 or more and 0.7000 or less,
based on the results of all experimental examples, slightly favorably, the value of φSSL1-BG-min/φSSL1-BM-max is 0.2278 or more and 0.6602 or less,
based on the results of ranks +4 to +5, extremely favorably, the value of φSSL1-BG-min/φSSL1-BM-max is 0.2427 or more and 0.6225 or less, and
based on the result of rank +5, dramatically favorably, the value of φSSL1-BG-min/φSSL1-BM-max is 0.2427 or more and 0.5906 or less.
Furthermore, the selection of a wavelength λSSL1-RM-max described in Condition 4 is conceivably characterized as follows when considering the results classified into ranks +1 to +5.
A wavelength λSSL1-RM-max can be selected from a range of 605 nm or more and 653 nm or less,
based on the results of all experimental examples, slightly favorably, the wavelength λSSL1-RM-max is selected from a range of 606 nm or more and 652 nm or less,
based on the results of ranks +3 to +5, more favorably, the wavelength λSSL1-RM-max is 607 nm or more and 647 nm or less, and
based on the results of ranks +4 to +5, extremely favorably, the wavelength λSSL1-RM-max is 622 nm or more and 647 nm or less. In addition, based on the trends described so far, λSSL1-RM-max is conceivably extremely favorably selected from a range of 625 nm or more and 647 nm or less.
Furthermore, based on the result of rank +5, λSSL1-RM-max is dramatically favorably selected from a range of 630 nm or more and 647 nm or less.
Moreover, based on an overall trend, λSSL1-RM-max is conceivably further dramatically favorably selected from a range of 631 nm or more and 647 nm or less.
These are trends that are conceivably required by the light-emitting device according to the first aspect of the first invention to have irregularities of appropriate sizes at appropriate positions of the spectral power distribution φSSL1(λ).
Furthermore, the selection of a wavelength λSSL1-BM-max described in Condition 5 is conceivably characterized as follows when considering the results classified into ranks +1 to +5.
A wavelength λSSL1-BM-max can be selected from a range of 430 nm or more and 480 nm or less,
based on the results of all experimental examples, slightly favorably, the wavelength λSSL1-BM-max is selected from a range of 440 nm or more and 460 nm or less, based on the results of ranks +4 to +5, extremely favorably, the wavelength λSSL1-BM-max is 447 nm or more and 460 nm or less, and
based on the results of rank +5, dramatically favorably, the wavelength λSSL1-BM-max is 450 nm or more and 457 nm or less.
In addition, based on an overall trend, λSSL1-BM-max is conceivably further dramatically favorably selected from a range of 451 nm or more and 456 nm or less.
These are trends that are conceivably required by the light-emitting device according to the first aspect of the first invention to have irregularities of appropriate sizes at appropriate positions of the spectral power distribution φSSL1(λ).
Furthermore, the selection of a value of φSSL1-BG-min/φSSL1-RM-max described in Condition 6 is conceivably characterized as follows when considering the results classified into ranks +1 to +5.
A value of φSSL1-BG-min/φSSL1-RM-max can be selected from a range of 0.1800 or more and 0.8500 or less,
based on the results of all experimental examples, slightly favorably, the value of φSSL1-BG-min/φSSL1-RM-max is 0.1917 or more and 0.8326 or less,
based on the results of ranks +3 to +5, more favorably, the value of φSSL1-BG-min/φSSL1-RM-max is 0.1917 or more and 0.6207 or less, and
based on the results of ranks +4 to +5, extremely favorably, the value of φSSL1-BG-min/φSSL1-RM-max is 0.1917 or more and 0.6202 or less, and
based on the result of rank +5, dramatically favorably, the value of φSSL1-BG-min/φSSL1-RM-max is 0.1917 or more and 0.5840 or less.
Furthermore, based on an overall trend, φSSL1-BG-min/φSSL1-RM-max is conceivably favorably selected from a range of 0.1917 or more and 0.7300 or less.
These are trends that are conceivably required by the light-emitting device according to the first aspect of the first invention to have irregularities of appropriate sizes at appropriate positions of the spectral power distribution φSSL1(λ).
Furthermore, the selection of a luminous efficacy of radiation KSSL1 (lm/W) described in Condition 7 is conceivably characterized as follows when considering the results classified into ranks +1 to +5.
A luminous efficacy of radiation KSSL1 (lm/W) can be selected from a range of 210.0 (lm/W) or more and 290.0 (lm/W) or less,
based on the results of all experimental examples, slightly favorably, the luminous efficacy of radiation KSSL1 (lm/W) is selected from a range of 212.2 (lm/W) or more and 286.9 (lm/W) or less,
based on the results of ranks +2 to +5, favorably, the luminous efficacy of radiation KSSL1 (lm/W) is 212.2 (lm/W) or more and 282.3 (lm/W) or less,
based on the results of ranks +4 to +5, extremely favorably, the luminous efficacy of radiation KSSL1 (lm/W) is 212.2 (lm/W) or more and 261.1 (lm/W) or less, and
based on the results of rank +5, dramatically favorably, the luminous efficacy of radiation KSSL1 (lm/W) is 212.2 (lm/W) or more and 256.4 (lm/W) or less.
Furthermore, the selection of a correlated color temperature TSSL1 (K) described in Condition 8 is conceivably characterized as follows when considering the results classified into ranks +1 to +5.
A correlated color temperature TSSL1 (K) can be selected from a range of 2600 (K) or more and 7700 (K) or less, based on the results of all experimental examples, slightly favorably, the correlated color temperature TSSL1(K) is 2644 (K) or more and 7613 (K) or less, and
based on the results of ranks +4 to +5, extremely favorably, the correlated color temperature TSSL1 (K) is 2644 (K) or more and 6797 (K) or less.
Furthermore, the selection of each saturation difference ΔCnSSL1 described in Condition I is conceivably characterized as follows when considering the results classified into ranks +1 to +5.
Each saturation difference ΔCnSSL1 can be selected from a range of −4.00 or more and 8.00 or less,
based on the results of all experimental examples, slightly favorably, each saturation difference ΔCnSSL1 is −3.49 or more and 7.11 or less,
based on the results of ranks +2 to +5, favorably, each saturation difference ΔCnSSL1 is −3.33 or more and 7.11 or less,
based on the results of ranks +4 to +5, extremely favorably, each saturation difference ΔCnSSL1 is −1.73 or more and 6.74 or less, and
based on the result of rank +5, dramatically favorably, each saturation difference ΔCnSSL1 is −0.93 or more and 6.74 or less.
Furthermore, the selection of a value of SATave(φSSL1(λ)) described in Condition II is conceivably characterized as follows when considering the results classified into ranks +1 to +5.
A value of SATave (φSSL1 (λ)) can be selected from a range of 0.50 or more and 4.00 or less,
based on the results of all experimental examples, slightly favorably, the value of SATave (φSSL1(λ)) is 0.53 or more and 3.76 or less,
based on the results of ranks +2 to +5, favorably, the value of SATave (φSSL1(λ)) is 1.04 or more and 3.76 or less,
based on the results of ranks +3 to +5, more favorably, the value of SATave (φSSL1(λ)) is 1.11 or more and 3.76 or less,
based on the results of ranks +4 to +5, extremely favorably, the value of SATave (φSSL1(λ)) is 1.40 or more and 3.76 or less, and
based on the result of rank +5, dramatically favorably, the value of SATave (φSSL1(λ)) is 1.66 or more and 3.76 or less.
Furthermore, the selection of a difference |ΔCSSL-max1−ΔCSSL-min1| between the maximum saturation difference value and the minimum saturation difference value described in Condition III is conceivably characterized as follows when considering the results classified into ranks +1 to +5.
A difference |ΔCSSL-max1−ΔCSSL-min1| can be selected from a range of 2.00 or more and 10.00 or less,
based on the results of all experimental examples, slightly favorably, the difference |ΔCSSL-max1−ΔCSSL-min1| is 3.22 or more and 9.52 or less,
based on the results of ranks +4 to +5, extremely favorably, the difference |ΔCSSL-max1−ΔCSSL-min1| is 4.12 or more and 7.20 or less, and based on the result of rank +5, dramatically favorably, the index is 4.66 or more and 7.10 or less.
Furthermore, the selection of an absolute value of each difference in hue angles |ΔhnSSL1| described in Condition IV is conceivably characterized as follows when considering the results classified into ranks +1 to +5.
A absolute value of each difference in hue angles |ΔhnSSL1| can be selected from a range of 0.00 or more and 12.50 or less,
based on the results of all experimental examples, slightly favorably, the absolute value of each difference in hue angles |ΔhnSSL1| is 0.00 or more and 12.43 or less,
based on the results of ranks +2 to +5, favorably, the absolute value of each difference in hue angles |ΔhnSSL1| is 0.01 or more and 12.43 or less,
based on the results of ranks +3 to +5, more favorably, the absolute value of each difference in hue angles |ΔhnSSL1| is 0.02 or more and 12.43 or less, and
based on the results of ranks +4 to +5, extremely favorably, the absolute value of each difference in hue angles |ΔhnSSL1| is 0.02 or more and 9.25 or less.
Moreover, since an absolute value of each difference in hue angles |ΔhnSSL1| is conceivably desirably 0, by adjusting a lower limit of values thereof, ideally,
a range of 0.00 or more and 12.43 or less is more favorably selected,
a range of 0.00 or more and 9.25 or less is extremely favorably selected,
a range of 0.00 or more and 7.00 or less is more extremely favorably selected, and
a range of 0.00 or more and 5.00 or less is further extremely favorably selected.
With respect to color appearance, the examination conducted above also shows that the color appearance realized by a light-emitting device “capable of realizing a natural, vivid, highly visible and comfortable appearance of colors and appearance of objects” is quantified when Conditions I to IV are simultaneously satisfied.
<Detailed Description 2>
The comparative visual experiment confirmed that light emitted from the light-emitting devices described in Experimental Examples 101 to 152 are more superior in terms of color appearance than light-emitting devices respectively emitting experimental reference light. At the same time, a significant improvement in light source efficiency ηSSL1 was also confirmed as described below. Table 1-8 compiles values of Acg(φSSL1(λ)) and light source efficiency ηSSL1 of Comparative Experimental Example 102 and Reference Experimental Example 101 shown in Table 1-2.
Meanwhile, Table 1-9 extracts all light-emitting devices with TSSL1 in a range of 3800 K to 4200 K and Duv(φSSL1(λ)) in a range of −0.0125 or more and −0.0100 or less from the experimental examples shown in Tables 1-3 to 1-7 and presents the light-emitting devices in such a manner that a fair comparison with Comparative Experimental Example 102 and Reference Experimental Example 101 can be performed. Table 1-9 compiles values derived from 101, 102, 103, 119, 121, 123, 141, and 142. Although Table 1-8 shows that Acg (φSSL1(λ)) has an average value of −51.8 and ηSSL1 has an average value of 47.0 (lm/W), Table 1-9 shows that Acg (φSSL1(λ)) has an average value of +51.4 and ηSSL1 has an average value of 65.5 (lm/W). On average, a difference in color appearance of illuminated objects between the light-emitting device shown in Table 1-8 and the light-emitting device shown in Table 1-9 is not large. Nevertheless, this shows that, compared to the conventional light-emitting device shown in Table 1-8, light source efficiency of the light-emitting device according to the first aspect of the first invention shown in Table 1-9 has increased by approximately 39%.
<Detailed Description 3>
Tables 1-10 to 1-15 show respective comparative experimental examples (ranks −1 to −5) of the first aspect of the first invention from the following perspectives. In addition,
BM-max
BG-min/
RM-max
max(nm)
max(nm)
Table 1-10 illustrates “a case where Duv(φSSL1(λ)) is less and −0.0220 and Acg(φSSL1(λ)) is −10 or less” despite using an appropriate blue semiconductor light-emitting element, an appropriate wide-band green phosphor, and an appropriate red phosphor.
Table 1-11 illustrates “a case where φSSL1-BG-min/φSSL1-BM-max is less than 0.225 as a result of the use of a yellow phosphor as a light-emitting element in the intermediate wavelength region” despite using an appropriate blue semiconductor light-emitting element and an appropriate red phosphor and despite Acg(φSSL1(λ)) being within an appropriate range.
Table 1-12 illustrates “a case where φSSL1-BG-min/φSSL1-BM-max is less than 0.225 as a result of the use of a narrow-band green phosphor as a light-emitting element in the intermediate wavelength region” despite using an appropriate blue semiconductor light-emitting element and an appropriate red phosphor and despite both Duv(φSSL1(λ)) and Acg (φSSL1(λ)) being within appropriate ranges.
Table 1-13 illustrates “a case where any of Duv(φSSL1(λ)), φSSL1-BG-min/φSSL1-BM-max, and λSSL1-RM-max which characterize a spectral power distribution is not appropriate” despite using an appropriate blue semiconductor light-emitting element, an appropriate wide-band green phosphor, and an appropriate red phosphor and despite Acg (φSSL1(λ)) being within an appropriate range.
Table 1-14 illustrates “a case where Duv(φSSL1(λ)) is more than −0.007 and Acg(φSSL1(λ)) is more than +120” despite using an appropriate blue semiconductor light-emitting element, an appropriate wide-band green phosphor, and an appropriate red phosphor.
Table 1-15 illustrates “a case where φSSL1-BG-min/φSSL1-BM-max is more than 0.7000 and Duv(φSSL1(λ)) is more than −0.007” despite using an appropriate blue semiconductor light-emitting element, an appropriate wide-band green phosphor, and an appropriate red phosphor and despite Acg(φSSL1(λ)) being within an appropriate range.
These results show that a light-emitting device which achieves both “a natural, vivid, highly visible and comfortable appearance of colors and appearance of objects” and “an improvement in light source efficiency” cannot be realized unless the spectral power distribution φSSL1(λ) as a light-emitting device satisfies all of Condition 1, Condition 2, Condition 3, and Condition 4. It is also shown that a light-emitting device with a spectral power distribution φSSL1(λ) not satisfying at least one of Condition 1, Condition 2, Condition 3, and Condition 4 failed to satisfy at least one of Conditions I to IV related to color appearance and, at the same time, ended up being classified in any of ranks −1 to −5 in comparative visual experiments.
Furthermore, with respect to light-emitting elements constituting a light-emitting device, a light-emitting device which achieves both “a natural, vivid, highly visible and comfortable appearance of colors and appearance of objects” and “an improvement in light source efficiency” could not be realized when using a narrow-band green phosphor or a yellow phosphor. This is also apparent from the fact that at least one of Conditions I to IV related to color appearance was not satisfied and, at the same time, from the fact that the light-emitting device was classified into rank −4 in a comparative visual experiment.
Further detailed examination reveals the following.
Comparative Experimental Example 103 (refer to
In Comparative Experimental Example 104 (refer to
Meanwhile, with respect to “a case where φSSL1-BG-min/φSSL1-BM-max is less than 0.225 as a result of the use of a yellow phosphor as a light-emitting element in the intermediate wavelength region” presented in Table 1-11 and “a case where φSSL1-BG-min/φSSL1-BM-max is less than 0.225 as a result of the use of a narrow-band green phosphor as a light-emitting element in the intermediate wavelength region” presented in Table 1-12,
In comparative visual experiments thereof, “some colors appeared excessively gaudy while other colors appeared excessively dull, and such differences in impression created a sense of considerable discomfort with respect to color appearance”. These are trends consistent with the CIELAB plots shown in
Conversely, using a wide-band green phosphor as a light-emitting element is conceivably favorable because these problems can be readily solved.
In Comparative Experimental Example 106 (not illustrated, φSSL1-BG-min/φSSL1-BM-max=0.1033) presented in Table 1-11, Comparative Experimental Example 110 (
Moreover, the following measures are conceivable as means to avoid situations such as those described above where φSSL1-BG-min/φSSL1-BM-max is excessively small. First, as first means, a wide-band green phosphor can be used. The use of a wide-band green phosphor enables situations where φSSL1-BG-min/φSSL1-BM-max is excessively small as presented in Comparative Experimental Example 106 and Comparative Experimental Example 110 to be avoided.
In addition, as second means to avoid situations where φSSL1-BG-min/φSSL1-BM-max is excessively small, a blue semiconductor light-emitting element having an appropriate wavelength can conceivably be used in addition to using a wide-band green phosphor. In the first aspect of the first invention, based on experimental examples, a blue semiconductor light-emitting element having a dominant wavelength during pulse drive of 445.0 nm or more and 475.0 nm or less can be selected, a blue semiconductor light-emitting element having a dominant wavelength during pulse drive of 447.5 nm or more and 470.0 nm or less can be more favorably selected, and a blue semiconductor light-emitting element having a dominant wavelength during pulse drive of 457.5 nm±2.5 nm can be dramatically favorably selected.
Moreover, while one may reason that φSSL1-BG-min/φSSL1-BM-max is favorably prevented from becoming excessively small by setting λCHIP-BM-dom to a longer wavelength, this is incorrect. A favorable range of λCHIP-BM-dom is as described above. The reason for this follows.
First, while the blue semiconductor light-emitting element is an AlGaInN semiconductor light-emitting element epitaxially mainly grown on a sapphire substrate, a Si substrate, a SiC substrate, or a GaN substrate, internal quantum efficiency thereof is dependent on an In composition of a quantum well layer or, in other words, on λCHIP-BM-dom. For example, an InGaN quantum well layer will now be considered. Since concentration of an In composition in a quantum well layer having sufficient spectral intensity at 465 nm or more and 525 nm or less is high enough to weaken a condition that causes maximum internal quantum efficiency, such an In composition is not favorable from the perspective of satisfying “both color appearance and light source efficiency of a light-emitting device”.
In addition, when considering color appearance, setting λCHIP-BM-dom to an excessively long wavelength so that spectral intensity originating from a light-emitting element is no longer present in an appropriate portion of a short wavelength region of φSSL1 (λ) results in color appearances of the 15 specific mathematically-derived Munsell renotation color samples in which a part thereof demonstrates excessive saturation tendencies while other parts demonstrate excessive nonsaturation tendencies. Specifically, tendencies of saturation/nonsaturation occur in different color samples from cases where φSSL1-BG-min/φSSL1-BM-max is excessively small. Therefore, setting λCHIP-BM-dom to an excessively long wavelength is not favorable for the purpose of preventing φSSL1-BG-min/φSSL1-BM-max from becoming excessively small.
Furthermore, the following measure is conceivable as third means to avoid situations where φSSL1-BG-min/φSSL1-BM-max is excessively small. Specifically, when a first λCHIP-BM-dom is set using a blue semiconductor light-emitting element having a dominant wavelength during pulse drive of 445.0 nm or more and 475.0 nm or less and a yellow phosphor or a narrow-band green phosphor is used as a light-emitting element in the intermediate wavelength region, a light-emitting element can conceivably be added in a range of 465 nm or more and 525 nm or less which straddles the short wavelength region and the intermediate wavelength region. To this end, an AlGaInN blue semiconductor light-emitting element having a second λCHIP-BM-dom with a center of its spectral power distribution in a region of 465 nm or more and 525 nm or less, a yellow-green light-emitting element (with a peak wavelength of around 530 nm to 570 nm) due to GaP on a GaP substrate having a second λCHIP-BM-dom, or the like can be selected and added. Moreover, a wide-band green phosphor can also be used in addition to the above.
However, since improvement in light source efficiency is as important as the color appearance of an illuminated object with the light-emitting device according to the first aspect of the first invention, excessively increasing light-emitting elements may cause a decline in light source efficiency in the form of increased mutual absorption, increased Stokes loss, or the like and is therefore not necessarily favorable. From this perspective, using a yellow phosphor, a narrow-band green phosphor, or the like as a light-emitting element in the intermediate wavelength region and further adding another light-emitting element is not favorable. In other words, in the light-emitting device according to the first aspect of the first invention, while a yellow phosphor, a narrow-band green phosphor, or the like can be used, the use of such phosphors is not necessarily favorable and a wide-band green phosphor is favorably used as a light-emitting element in the intermediate wavelength region.
In comparative visual experiments of Comparative Experimental Example 115 (refer to
In Comparative Experimental Example 116 (refer to
In Comparative Experimental Example 119 (refer to
In Comparative Experimental Example 126 (refer to
Moreover, in a similar manner, φSSL1-BG-min/φSSL1-BM-max must also be sufficiently controlled. In general terms, the appropriate ranges of φSSL1-BG-min/φSSL1-BM-max and φSSL1-BG-min/φSSL1-BM-max indicate that, in order to realize the effect of the first aspect of the first invention, it is essential that irregularities with appropriate sizes are present at appropriate positions in the spectral power distribution φSSL1(λ) of the light-emitting device.
While a favorable embodiment for implementing the light-emitting device according to the first aspect of the first invention will be described below, it is to be understood that modes for implementing the light-emitting device according to the first aspect of the first invention is not limited to those used in the following description.
With the light-emitting device according to the first aspect of the first invention, no restrictions are placed on configurations, materials, and the like of the light-emitting device as long as a radiometric property and a photometric property of test light which is irradiated from the light-emitting device in a main radiant direction and which becomes a color stimulus with respect to an illuminated object are in appropriate ranges.
A light-emitting device for implementing the light-emitting device according to the first aspect of the first invention such as an illumination light source, a lighting fixture including the illumination light source, or a lighting system including the illumination light source or the lighting fixture includes blue semiconductor light-emitting element.
Moreover, when the various conditions described above are satisfied and the effect of the first aspect of the first invention is obtained, illuminating light sources including semiconductor light-emitting elements may include, in addition to a blue semiconductor light-emitting element, for example, a plurality of semiconductor light-emitting elements of different types such as green and red in a single illuminating light source or a single illuminating light source may include a blue semiconductor light-emitting element, another single illuminating light source may include a green semiconductor light-emitting element, yet another single illuminating light source may include a red semiconductor light-emitting element, and the illuminating light sources may be integrated together with a lens, a reflecting mirror, a drive circuit, and the like in a lighting fixture to be provided in an illuminating system. Furthermore, in a case where one illumination light source is included in one lighting fixture and an individual semiconductor light-emitting element is incorporated in the illumination light source, even if the light-emitting device according to the first aspect of the first invention cannot be implemented as an individual illumination light source or an individual lighting fixture, a lighting system may be configured such that light radiated as the lighting system satisfies desired characteristics at a position of an illuminated object due to additive color mixing with light from a different lighting fixture that exists in the lighting system or the lighting system may be configured such that light in a main radiant direction among light radiated as the lighting system satisfies desired characteristics. In any mode, light as a color stimulus which is ultimately irradiated on an illuminated object or light in a main radiant direction among light emitted from the light-emitting device need only satisfy appropriate conditions according to the first aspect of the first invention.
Hereinafter, a light-emitting device according to the first aspect of the first invention will be described on the basis of satisfying the appropriate conditions described above.
The light-emitting device according to the first aspect of the first invention favorably includes a light-emitting element (light-emitting material) which has a peak within a short wavelength range from Λ1 (380 nm) to Λ2 (495 nm), another light-emitting element (light-emitting material) which has a peak within an intermediate wavelength range from Λ2 (495 nm) to Λ3 (590 nm), and yet another light-emitting element (light-emitting material) which has a peak within a long wavelength range from Λ3 (590 nm) to 780 nm. This is because favorable color appearance can be readily achieved if intensity of each of the light-emitting elements can be individually set or controlled.
Therefore, a light-emitting device according to the first aspect of the first invention at least includes one light-emitting element (light-emitting material) having a light emission peak in each of the three wavelength regions described above.
Moreover, when the various conditions described above are satisfied and the effect of the first aspect of the first invention is obtained, two regions among the three wavelength regions may respectively include one light-emitting element (light-emitting material) while the other region may include a plurality of light-emitting elements (light-emitting materials), one region among the three wavelength regions may include one light-emitting element (light-emitting material) while the other two regions may include a plurality of light-emitting elements (light-emitting materials), or all three wavelength regions may include a plurality of light-emitting elements.
In the first aspect of the first invention, while semiconductor light-emitting elements and phosphors can be freely mixed and mounted, at least a blue light-emitting element and two types of (green and red) phosphors are mounted in one light source. Moreover, when the various conditions described above are satisfied and the effect of the first aspect of the first invention is obtained, a blue light-emitting element and three types of (green, red 1, and red 2) phosphors may be mounted in one light source or one light source may include a portion mounted with a blue light-emitting element and two types of (green and red) phosphors and a portion mounted with a purple light-emitting element and three types of (blue, green, and red) phosphors.
In a light-emitting device according to the first aspect of the first invention, as light-emitting elements (light-emitting materials) in the three respective wavelength regions, the following light-emitting materials, phosphor materials, and semiconductor light-emitting elements are favorably included in the light-emitting device as light-emitting elements from the perspective of controlling intensity of peak portions or intensity of valleys between peaks or, in other words, from the perspective of forming appropriate irregularities in a spectral power distribution.
First, in the short wavelength range from Λ1 (380 nm) to Λ2 (495 nm) among the three wavelength ranges, light emitted from all light sources can be included, such as thermal emission light from a hot filament or the like, electric discharge emission light from a fluorescent tube, a high-pressure sodium lamp, or the like, stimulated emission light from a laser or the like, spontaneous emission light from a semiconductor light-emitting element, and spontaneous emission light from a phosphor. Among the above, emission of light from a semiconductor light-emitting element is favorable due to its small sizes and high energy efficiency.
Specifically, the following is favorable.
Favorable examples of a semiconductor light-emitting element include a blue light-emitting element in which an In(Al)GaN material formed on a sapphire substrate or a GaN substrate is included in an active layer structure.
Furthermore, a blue light-emitting element in which a Zn(Cd) (S)Se material formed on a GaAs substrate is included in an active layer structure is also favorable (Favorable peak wavelengths are as described earlier).
Moreover, a spectral power distribution or a peak wavelength of a radiant flux produced by a light-emitting element (light-emitting material) such as a semiconductor light-emitting element or a phosphor normally fluctuates slightly depending on ambient temperature, a heat dissipation environment of the light-emitting device including a package and a fixture, injected current, circuit architecture and, in some cases, deterioration or the like. The same applies to a spectral power distribution or a peak wavelength of a radiant flux produced by light-emitting elements (light-emitting materials) such as the semiconductor light-emitting elements and phosphors described below.
The active layer structure may be any of a multiple quantum well structure in which a quantum well layer and a barrier layer are laminated, a single or a double heterostructure including a relatively thick active layer and a barrier layer (or a clad layer), and a homo junction constituted by a single pn junction.
In addition, when the various conditions described above are satisfied and the effect of the first aspect of the first invention is obtained, a semiconductor laser such as a blue semiconductor laser may be used as a light-emitting element.
A semiconductor light-emitting element in the short wavelength region which is used in a light-emitting device according to the first aspect of the first invention favorably has an emission spectrum with a relatively wide full-width at half-maximum. From this perspective, a full-width at half-maximum of a blue semiconductor light-emitting element used in the short wavelength region is favorably 5 nm or more, more favorably 10 nm or more, extremely favorably 15 nm or more, and dramatically favorably 20 nm or more. However, having a significantly wide emission spectrum also makes it difficult to control φSSL1-BG-min/φSSL1-BM-max, φSSL1-BG-min/φSSL1-BM-max, and the like and prevents irregularities with appropriate sizes from being formed at appropriate positions in the spectral power distribution φSSL1(λ). Therefore, a full-width at half-maximum is favorably 45 nm or less, more favorably 40 nm or less, extremely favorably 35 nm or less, and dramatically favorably 30 nm or less.
Since a blue semiconductor light-emitting element in the short wavelength range that is used in the light-emitting device according to the first aspect of the first invention favorably includes an In(Al)GaN material in an active layer structure, the semiconductor light-emitting element is favorably a light-emitting element formed on a sapphire substrate or a GaN substrate.
In addition, as far as substrate thickness is concerned, the substrate is favorably either thick or completely separated from the blue semiconductor light-emitting element. In particular, when creating a blue semiconductor light-emitting element in the short wavelength range on a GaN substrate, in order to facilitate light extraction from side walls of the GaN substrate, the substrate is favorably thick and is 100 μm or more, more favorably 200 μm or more, extremely favorably 400 μm or more, and dramatically favorably 600 μm or more. On the other hand, for convenience of creating elements, the substrate thickness is favorably 2 mm or less, more favorably 1.8 mm or less, extremely favorably 1.6 mm or less, and dramatically favorably 1.4 mm or less.
Meanwhile, when creating a light-emitting element on a sapphire substrate or the like, the substrate is favorably separated using a method such as laser lift-off. Accordingly, internal reflection that occurs at an optical interface between an In(Al)GaN epitaxial layer and a sapphire substrate can be eliminated and light extraction efficiency can be improved. As a result, fabricating a light-emitting device according to the first aspect of the first invention using such a light-emitting element results in an improvement in light source efficiency and is therefore favorable.
In addition, when the various conditions described above are satisfied and the effect of the first aspect of the first invention is obtained, a light-emitting device according to the first aspect of the first invention may include a phosphor material in a short wavelength region.
Moreover, in the first aspect of the first invention, φSSL1(λ) described above favorably does not have effective intensity derived from a light-emitting element in a range of 380 nm or more and 405 nm or less. “Does not have effective intensity derived from a light-emitting element” refers to cases where the various conditions described above are satisfied and the effect of the first aspect of the first invention is produced even when φSSL1 (λ) has intensity derived from a light-emitting element at a wavelength λf in this range. More specifically, this refers to cases where intensity φSSL1(λf) derived from a light-emitting element in the wavelength range described above having been normalized by a maximum spectral intensity of φSSL1(λ) is favorably 10% or less, more favorably 5% or less, extremely favorably 3% or less, and dramatically favorably 1% or less as relative intensity at an arbitrary wavelength λf of 380 nm or more and 405 nm or less.
Therefore, in the first aspect of the first invention which uses a light-emitting element that emits blue light such as a blue light-emitting element (for example, a blue semiconductor laser with an oscillation wavelength of around 445 nm to 485 nm), intensity may be included as noise derived from a light-emitting element when intensity derived from the light-emitting element in a range of 380 nm or more and 405 nm or less is within the range of relative intensity described above.
Next, in the intermediate wavelength range from Λ2 (495 nm) to Λ3 (590 nm) among the three wavelength ranges, light emitted from all light sources can be included, such as thermal emission light from a hot filament or the like, electric discharge emission light from a fluorescent tube, a high-pressure sodium lamp, or the like, stimulated emission light from a laser or the like including second-order harmonic generation (SHG) using a non-linear optical effect or the like, spontaneous emission light from a semiconductor light-emitting element, and spontaneous emission light from a phosphor. Among the above, emission of light from a photoexcited phosphor is favorable.
Furthermore, when the various conditions described above are satisfied and the effect of the first aspect of the first invention is obtained, light emission from a semiconductor light-emitting element and light emission from a semiconductor laser or an SHG laser may be included, in which case these components are favorable due to their small sizes and high energy efficiency.
Examples of semiconductor light-emitting elements include a blue-green light-emitting element (with a peak wavelength of around 495 nm to 500 nm), a green light-emitting element (with a peak wavelength of around 500 nm to 530 nm), a yellow-green light-emitting element (with a peak wavelength of around 530 nm to 570 nm), and a yellow light-emitting element (with a peak wavelength of around 570 nm to 580 nm) which include an In(Al)GaN material on a sapphire substrate or a GaN substrate in an active layer structure. In addition, examples of semiconductor light-emitting elements include a yellowish green light-emitting element (with a peak wavelength of around 530 nm to 570 nm) due to GaP on a GaP substrate or a yellow light-emitting element (with a peak wavelength of around 570 nm to 580 nm) due to GaAsP on a GaP substrate. Furthermore, example of semiconductor light-emitting elements includes a yellow light-emitting element (with a peak wavelength of around 570 nm to 580 nm) due to AlInGaP on a GaAs substrate.
Specific examples of a green phosphor material in the intermediate wavelength region to be used in a light-emitting device according to the first aspect of the first invention include green phosphors which use, as a base material, Ce3+ activated aluminate, Ce3+ activated yttrium-aluminum oxide, Eu2+ activated alkaline-earth silicate crystals, or Eu2+ activated alkaline-earth nitride silicate. These green phosphors can normally be excited using a semiconductor light-emitting element ranging from ultraviolet to blue.
Specific examples of the Ce3+ activated aluminate phosphor include a green phosphor represented by the following general formula (4),
Ya(Ce,Tb,Lu)b(Ga,Sc)cAldOe (4)
(In the general formula (4), a, b, c, d and e satisfy a +b=3, 0≤b≤0.2, 4.5≤c+d≤5.5, 0.1≤c≤2.6, and 10.8≤e≤13.4.) (Ce3+ activated aluminate phosphor represented by the general formula (4) is referred to as a G-YAG phosphor).
In the G-YAG phosphor in particular, the composition range that satisfies the general formula (4) can be suitably selected. In the first aspect of the first invention, the wavelength λPHOS-GM-max and the full-width at half-maximum WPHOS-GM-fwhm that implement the maximum emission intensity when light is excited with the phosphor alone are preferably in the following ranges.
Specific examples of Ce3+ activated yttrium-aluminum oxide phosphor include a green phosphor represented by the following general formula (5).
Lua(Ce,Tb,Lu)b(Ga,Sc)cAldOe (5)
(In the general formula (5), a, b, c, d and e satisfy a+b=3, 0≤b≤0.2, 4.5≤c+d≤5.5, 0≤c≤2.6, and 10.8≤e≤13.4.) (the Ce3+ activated yttrium-aluminum oxide phosphor represented by the general formula (5) is called “LuAG phosphor”.)
In the LuAG phosphor, in particular, the composition range that satisfies the general formula (5) can be suitably selected. In the first aspect of the first invention, the wavelength λPHOS-GM-max and the full-width at half-maximum WPHOS-GM-fwhm that implement the maximum emission intensity when light is excited with the phosphor alone are preferably in the following ranges.
Other examples include green phosphors represented by the following general formula (6) and a phosphor represented by the following general formula (7).
M1aM2bM3cOd (6)
(In the general formula (6), M1 indicates a bivalent metallic element, M2 indicates a trivalent metallic element, and M3 indicates a tetravalent metallic element, and a, b, c and d satisfy 2.7≤a≤3.3, 1.8≤b≤2.2, 2.7≤c≤3.3 and 11.0≤d≤13.0.) (The phosphor represented by the general formula (6) is referred to as a CSMS phosphor).
In the above general formula (6), M1 is a bivalent metallic element, and is preferably at least one type selected from the group consisting of Mg, Ca, Zn, Sr, Cd and Ba, further preferably Mg, Ca or Zn, and particularly preferably Ca. In this case, Ca may be a single system or may be a composite system with Mg. M2 may include other bivalent metallic elements.
M2 is a trivalent metallic element, and is preferably at least one type selected from the group consisting of Al, Sc, Ga, Y, In, La, Gd and Lu, further preferably Al, Sc, Y or Lu, and particularly preferably Sc. In this case, Sc may be a single system or may be a composite system with Y or Lu. M2 must include Ce and may include other trivalent metallic elements.
M3 is a tetravalent metallic element, and preferably includes at least Si. An example of a tetravalent metallic element M3, other than Si, is preferably at least one type selected from the group consisting of Ti, Ge, Zr, Sn and Hf, more preferably at least one type selected from the group consisting of Ti, Zr, Sn and Hf, and particularly preferably Sn. Particularly it is preferable that M3 is Si. M3 may include other tetravalent metallic elements.
In the CSMS phosphor in particular, the composition range that satisfies the general formula (6) can be suitably selected. For the wavelength λPHOS-GM-max and the full-width at half-maximum WPHOS-GM-fwhm that implement the maximum emission intensity when light is excited with the phosphor alone to be in a preferable range in the first aspect of the first invention, the lower limit of the ratio of Ce included in M2 to the entire M2 is preferably 0.01 or more, and more preferably 0.02 or more. Further, the upper limit of the ratio of Ce included in M2 to the entire M2 is preferably 0.10 or less, and more preferably 0.06 or less. Further, the lower limit of the ratio of Mg included in M1 to the entire M1 is preferably 0.01 or more, and more preferably 0.03 or more. On the other hand, the upper limit is preferably 0.30 or less, and more preferably 0.10 or less.
Furthermore, examples include represented by the following general formula (7).
M1aM2bM3cOd (7)
(In the general formula (7), M1 indicates an activator element including at least Ce, M2 is a bivalent metallic element, and M3 is a trivalent metallic element, and a, b, c and d satisfy 0.0001≤a≤0.2, 0.8≤b≤1.2, 1.6≤c≤2.4 and 3.2≤d≤4.8.) (A phosphor represented by the general formula (7) is called “CSO phosphor”.)
In the above general formula (7), M1 is an activator element contained in a host crystal, and includes at least Ce. M1 can contain at least one type of bivalent to tetravalent element selected from the group consisting of Cr, Mn, Fe, Co, Ni, Cu, Ce, Pr, Nd, Sm, Eu, Tb, Dy, Ho, Er, Tm and Yb.
M2 is a bivalent metallic element, and is preferably at least one type selected from the group consisting of Mg, Ca, Zn, Sr, Cd and Ba, further preferably Mg, Ca or Sr, and is particularly preferably that Ca is 50 mol % or more of the elements of M2.
M3 is a trivalent metallic element, and is preferably at least one type selected from the group consisting of Al, Sc, Ga, Y, In, La, Gd, Yb and Lu, and further preferably Al, Sc, Yb or Lu, more further preferably Sc, or Sc and Al, or Sc and Lu, and is particularly preferably that Sc is 50 mol % or more of the elements of M3.
M2 and M3 are a bivalent metallic element and trivalent metallic element respectively, and a small part of M2 and/or M3 may be a metallic element of which valence is any one of 1, 4 and 5, and a very small amount of anions, such as a halogen element (F, Cl, Br, I), nitrogen, sulfur selenium or the like may be contained in the compound.
In a CSO phosphor in particular, a composition range that satisfies the general formula (7) can be suitably selected. In the first aspect of the first invention, the wavelength λPHOS-GM-max and the full-width at half-maximum WPHOS-GM-fwhm that implement the maximum emission intensity when light is excited with phosphor alone are preferably in the following ranges.
Furtheremore, specific examples of green phosphors using an alkaline-earth silicate crystal as a host and Eu2+ as an activator include a phosphor represented by the following general formula (8).
(BaaCabSrcMgdEux)SiO4 (8)
(In the general formula (8), a, b, c, d, and x satisfy a +b+c+d+x=2, 1.0≤a≤2.0, 0≤b<0.2, 0.2≤c≤1.0, 0≤d<0.2, and 0<x≤0.5.) (Alkaline-earth silicate represented by the general formula (8) is referred to as a BSS phosphor).
In the BSS phosphor, a composition range that satisfies the general formula (8) can be suitable selected. In the first aspect of the first invention, the wavelength λPHOS-GM-max and the full-width at half-maximum WPHOS-GM-fwhm that implement the maximum emission intensity when light is excited with the phosphor alone are preferably in the following ranges.
Furthermore,
Furtheremore, specific examples of green phosphors using an alkaline-earth nitride silicate as a host and Eu2+ as an activator include a phosphor represented by the following general formula (9).
(Ba,Ca,Sr,Mg,Zn,Eu)3Si6O12N2 (9)
(This phosphor is referred to as a BSON phosphor).
In the BSON phosphor, a composition range that satisfies the general formula (9) can be suitable selected. In the first aspect of the first invention, the wavelength λPHOS-GM-max and the full-width at half-maximum WPHOS-GM-fwhm that implement the maximum emission intensity when light is excited with the phosphor alone are preferably in the following ranges.
In the general formula (9), a combination of Ba, Sr and Eu is preferably among the selectable bivalent metallic elements (Ba, Ca, Sr, Mg, Zn, Eu), and the ratio of Sr to Ba is more preferably 10 to 30%.
In addition, when the various conditions described above are satisfied and the effect of the first aspect of the first invention is obtained, a yellow phosphor may be additionally included such as a yttrium-aluminum-garnet-based phosphor (referred to as a YAG phosphor) which is represented by (Y1-uGdu)3(Al1-vGav)5O12:Ce, Eu (where u and v respectively satisfy 0≤u≤0.3 and 0≤v≤0.5) or a lanthanum silicon nitride phosphor (referred to as an LSN phosphor) which is represented by Ca1.5xLa3-xSi6N11:Ce (where x satisfies 0≤x≤1). Furthermore, a narrow-band green phosphor represented by Si6-zAlzOzN8-z:Eu (where 0<z<4.2) having an Eu2+ activated SiAlON crystal as a base material (this phosphor is referred to as a β-SiAlON phosphor) may be included. However, it is difficult to realize a desired color appearance of an illuminated object when configuring a light-emitting device using only these narrow-band green phosphors or yellow phosphors as a light-emitting element in the intermediate wavelength region. Therefore, in the light-emitting device according to the first aspect of the first invention, while a yellow phosphor or a narrow-band green phosphor can be used in combination with other semiconductor light-emitting elements, wide-band phosphors, or the like, such combined use is not necessarily favorable. Favorably, a wide-band green phosphor is used as a light-emitting element in the intermediate wavelength region.
Therefore, a light-emitting device according to the first aspect of the first invention favorably does not substantially include a yellow phosphor. “Does not substantially include a yellow phosphor” refers to cases where the various conditions described above are satisfied and the effect produced by the first aspect of the first invention is obtained even when a yellow phosphor is included and specifically refers to cases where a weight of a yellow phosphor with respect to a weight of all phosphors is favorably 7% or less, more favorably 5% or less, extremely favorably 3% or less, and dramatically favorably 1% or less.
Next, in the long wavelength range from Λ3 (590 nm) to 780 nm among the three wavelength ranges, light emitted from all light sources can be included, such as thermal emission light from a hot filament or the like, electric discharge emission light from a fluorescent tube, a high-pressure sodium lamp, or the like, stimulated emission light from a laser or the like, spontaneous emission light from a semiconductor light-emitting element, and spontaneous emission light from a phosphor. Among the above, emission of light from a photoexcited phosphoris is favorable.
Furthermore, when the various conditions described above are satisfied and the effect of the first aspect of the first invention is obtained, light emission from a semiconductor light-emitting element and light emission from a semiconductor laser or an SHG laser may be included, in which case these components are favorable due to their small sizes and high energy efficiency.
Examples of the semiconductor light-emitting element include an orange light-emitting element (with a peak wavelength of around 590 nm to 600 nm) or a red light-emitting element (from 600 nm to 780 nm) in which an AlGaAs material formed on a GaAs substrate or an (Al)InGaP material formed on a GaAs substrate is included in an active layer structure. In addition, examples of the semiconductor light-emitting element include of a red light-emitting element (from 600 nm to 780 nm) in which an GaAsP material formed on a GaP substrate is included in an active layer structure.
In addition, specific examples of the light-emitting device according to the first aspect of the first invention include phosphors using Eu2+ as an activator and a crystal constituted by alkaline-earth silicon-nitride, a SiAlON, or alkaline-earth silicate as a host. A red phosphor of this type can normally be excited using a semiconductor light-emitting element ranging from ultraviolet to blue.
Specific examples of phosphors using an alkaline-earth silicon-nitride crystal as a host include a phosphor represented by CaAlSiN3:Eu (this phosphor is referred to as a CASN phosphor), (Ca,Sr,Ba,Mg)AlSiN3:Eu and/or (Ca,Sr,Ba)AlSiN3:Eu (this phosphor is referred to as a SCASN phosphor), a phosphor represented by (CaAlSiN3)1-x(Si2N2O)x:Eu (where x satisfies 0<x<0.5) (this phosphor is referred to as a CASON phosphor), a phosphor represented by (Sr, Ca, Ba)2AlxSi5-xOxN8-x:Eu (where 0≤x≤2), and a phosphor represented by Euy (Sr, Ca, Ba)1-y:Al1+xSi4-xOXN7-x (where 0≤x<4, 0≤y<0.2).
Other examples include a Mn4+-activated fluoride complex phosphor. A Mn4+-activated fluoride complex phosphor is a phosphor which uses Mn4+ as an activator and a fluoride complex salt of an alkali metal, amine, or an alkaline-earth metal as a host crystal. Fluoride complex salts which form the host crystal include those whose coordination center is a trivalent metal (B, Al, Ga, In, Y, Sc, or a lanthanoid), a tetravalent metal (Si, Ge, Sn, Ti, Zr, Re, or Hf), and a pentavalent metal (V, P, Nb, or Ta), and the number of fluorine atoms coordinated around the center ranges from 5 to 7.
Specific examples of a Mn4+-activated fluoride complex phosphor include A2+xMyMnzFn (where A is Na and/or K; M is Si and Al; −1≤x≤1 and 0.9≤y+z≤1.1 and 0.001≤z≤0.4 and 5≤n≤7) having a hexafluoro complex salt of an alkaline metal as a base crystal. Phosphors represented by A2+xMyMnzFn include those where A denotes one or more elements selected from K (potassium) and Na (sodium) and M denotes Si (silicon) or Ti (titanium) such as K2SiF6:Mn (referred to as a KSF phosphor) or K2Si1-xNaxAlxF6:Mn,K2TiF6:Mn (referred to as a KSNAF phosphor) which is obtained by replacing a part (favorably, 10 mol % or less) of the constituent elements of K2SiF6:Mn with Al and Na.
Other examples include a phosphor represented by the following general formula (10) and a phosphor represented by the following general formula (11).
(La1-x-yEuxLny)2O2S (10)
(In the general formula (10), x and y denote numbers respectively satisfying 0.02≤x≤0.50 and 0≤y≤0.50, and Ln denotes at least one trivalent rare-earth element among Y, Gd, Lu, Sc, Sm, and Er). (A lanthanum oxysulfide phosphor represented by the general formula (10) is referred to as an LOS phosphor).
(k−x)MgO·xAF2·GeO2:yMn4+ (11)
(In the general formula (11), k, x, and y denote numbers respectively satisfying 2.8≤k≤5, 0.1≤x≤0.7, and 0.005≤y≤0.015, and A is any of calcium (Ca), strontium (Sr), barium (Ba), zinc (Zn), and a mixture consisted of these elements). (A germanate phosphor represented by the general formula (11) is referred to as an MGOF phosphor).
In the first aspect of the first invention, a configuration in which only one of a CASN phosphor, a CASON phosphor, and a SCASN phosphor is included in a light-emitting device is favorable for improving light source efficiency. Meanwhile, although a KSF phosphor, a KSNAF phosphor, a LOS phosphor, and a MGOF phosphor have extremely narrow half-value widths of around 6 nm, around 6 nm, around 4 nm, and around 16 nm, respectively, using these phosphors in combination with a CASN phosphor, a CASON phosphor, a SCASN phosphor, or the like may result in forming irregularities in an appropriate range in the spectral power distribution φSSL1(λ) of the light-emitting device and is therefore favorable.
With the combinations of light-emitting elements described above, peak wavelength positions, full-widths at half-maximum, and the like of the respective light-emitting elements are extremely advantageous in realizing a color appearance or an object appearance perceived as favorable by the subjects in the visual experiments.
In the light-emitting device according to the first aspect of the first invention, it is favorable to use the light-emitting elements (light-emitting materials) heretofore described because the index Acg(φSSL1(λ)), the distance Duv(φSSL1(λ)), φSSL1-BG-min/φSSL1-BM-max, the wavelength wavelength λSSL1-RM-max and the like can be more readily set to desired values. Using the light-emitting elements described above is also favorable because ΔCnSSL1, SATaveφSSL1(λ)), |ΔCSSL-maX1−ΔCSSL-min1|, and |ΔhnSSL1| which are related, when light is treated as a color stimulus, to a difference between color appearances of the 15 color samples when illumination by the light-emitting device is assumed and color appearances when illumination by calculational reference light is assumed can also be more readily set to desired values.
A second aspect of the first invention of the present invention is a method for designing a light-emitting device. With a method for designing according to the second aspect of the first invention of the present invention, design guidelines for “a light-emitting device capable of realizing a natural, vivid, highly visible and comfortable appearance of colors or an appearance of objects” can be provided. In other words, by designing a light-emitting device according to the description of the second aspect of the first invention of the present invention, “a light-emitting device capable of realizing a natural, vivid, highly visible and comfortable appearance of colors or an appearance of objects” can be provided. That is, the description on the first aspect of the first invention may be entirely applied to the second aspect of the first invention of the present invention.
<2. Second Invention>
The second invention of the present invention includes an aspect related to the light-emitting device (a first aspect of the second invention) as well as an aspect related to a method for designing the light-emitting device (a second aspect of the second invention), an aspect related to a method for driving the light-emitting device (a third aspect of the second invention), and an aspect related to an illumination method (a fourth aspect of the second invention).
In order to solve the problems described in the section titled “Technical Problem” presented earlier, the present inventor has arrived with a light-emitting device having improved light source efficiency and a design guideline for the light-emitting device in Japanese Patent Application No. 2014-159784.
The light sources described above that satisfy the requirements which the present inventor has already discovered can implement “a natural, vivid, highly visible, and comfortable appearance of colors and an appearance of objects” and, at the same time, improve light source efficiency of such light sources.
However, the concept of an optimum illumination slightly differs depending on age, gender, country and the like, and also differs depending on the space and purpose of the illumination. Furthermore, taste in illumination which an individual feels to be optimum may differ greatly depending on the living environment where the individual grew up and the culture thereof.
It is an object of the second invention of the present invention to provide a light-emitting device that can implement a natural, vivid, highly visible and comfortable appearance of colors and appearance of objects as if the objects are seen outdoors, and to provide a light-emitting device with improved light source efficiency that can change the appearance of colors of illuminated objects so as to satisfy the requirements for various illuminations, and a method for designing thereof. Furthermore, it is an object of the second invention of the present invention to provide a method for driving the light-emitting device and an illumination method with a device.
In order to achieve the objects described above, the first aspect of the second invention of the present invention relates to the following a light-emitting device. [1] A light-emitting device which includes M number of light-emitting areas (where M is a natural number equal to or greater than 2), and has a blue semiconductor light-emitting element, a green phosphor, and a red phosphor as light-emitting elements in at least one of the light-emitting areas, wherein
when φSSL2N(λ) (where N ranges from 1 to M) denotes a spectral power distribution of light emitted from each light-emitting area in a main radiant direction of the light-emitting device, and φSSL2(λ) denoting a spectral power distribution of all light emitted from the light-emitting device in the radiant direction satisfies
the light-emitting device includes a light-emitting area where φSSL2(λ) satisfies Conditions 1 to 4 below.
light emitted from the light-emitting device includes, in the main radiant direction thereof, light whose distance DuvφSSL2(λ)) from a black-body radiation locus as defined by ANSI C78.377 satisfies
−0.0220≤Duv(φSSL2(λ))≤−0.0070.
φSSL2(λ) denotes a spectral power distribution of light emitted from the light-emitting device in the radiant direction,
φref2(λ) denotes a spectral power distribution of reference light which is selected in accordance with a correlated color temperature TSSL2 of the light emitted from the light-emitting device in the radiant direction,
(XSSL2, YSSL2, ZSSL2) denote tristimulus values of the light emitted from the light-emitting device in the radiant direction, and
(Xref2, Yref2, Zref2) denote tristimulus values of the reference light which is selected in accordance with the correlated color temperature TSSL2 of the light emitted from the light-emitting device in the main radiant direction, and
a normalized spectral power distribution SSSL2(λ) of the light emitted from the light-emitting device in the radiant direction,
a normalized spectral power distribution Sref2(λ) of the reference light which is selected in accordance with the correlated color temperature TSSL2 (K) of the light emitted from the light-emitting device in the radiant direction, and
a difference ΔSSSL2(λ) of between normalized spectral power distributions are respectively defined as
S
SSL2(λ)=φSSL2(λ)/YSSL2
S
ref2(λ)=φref2(λ)/Yref2and
ΔSSSL2(λ)=Sref2(λ)−SSSL2(λ) and
in a case where λSSL2-RL-max (nm) represents a wavelength that provides a longest wavelength local maximum value of SSSL2(λ) in a wavelength range of 380 nm or more and 780 nm or less, and when a wavelength Λ4 that is represented by SSSL2 (λSSL2-RL-max)/2 exists on a longer wavelength-side of λSSL2-RL-max,
an index Acg(φSSL2(λ)) represented by the following formula (2-1) satisfies
−10.0<Acg(φSSL2(λ))≤120.0,
but
in a case where λSSL2-RL-max (nm) represents a wavelength that provides the longest wavelength local maximum value of SSSL2(λ) in a wavelength range of 380 nm or more and 780 nm or less, and when the wavelength Λ4 that is represented by SSSL2(λSSL2-RL-max)/2 does not exist on the longer wavelength-side of λSSL2-RL-max,
an index Acg(φSSL2(λ)) represented by the following formula (2-2) satisfies
−10.0<Acg(φSSL2(λ))≤120.0,
[Expression 11]
A
cg(ϕSSL2(λ))=∫380495ΔSSSL2(λ)dλ+∫495590(−ΔSSSL2(λ))dλ+∫590Λ4ΔSSSL2(λ)dλ (2- 1)
[Expression 12]
A
cg(ϕSSL2(λ))=∫380495ΔSSSL2(λ)dλ+∫495590(−ΔSSSL2(λ))dλ+∫590780ΔSSSL2(λ)dλ (2-2)
when a maximum value of spectral intensity in a range of 430 nm or more and 495 nm or less is defined as φSSL2-BM-max and a minimum value of spectral intensity in a range of 465 nm or more and 525 nm or less is defined as φSSL2-BG-max, the spectral power distribution φSSL2(λ) of light satisfies
0.2250≤φSSL2-BG-min/φSSL2-BM-max≤0.7000; and
in the spectral power distribution φSSL2(λ) of light, when a maximum value of spectral intensity in a range of 590 nm or more and 780 nm or less is defined as φSSL2-RM-max, a wavelength λSSL2-RM-max that provides λSSL2-RM-max satisfies
605(nm)≤λSSL2-RM-max≤653(nm).
[2] The light-emitting device according to [1], wherein all of φSSL2N(λ) (N is 1 to M) satisfies the Conditions 1 to 4. [3] The light-emitting device according to [1] or [2], wherein at least one light-emitting area of the M number of light-emitting areas has wiring that allows the light-emitting area to be electrically driven independently from other light-emitting areas.
[4] The light-emitting device according to [3], wherein all the M numbers of light-emitting areas each have wiring that allows the light-emitting area to be electrically driven independently from other light-emitting areas.
[5] The light-emitting device according to any one of [1] to [4], wherein the light-emitting device satisfies Condition 5 below.
In the spectral power distribution φSSL2(λ) of light described above, a wavelength λSSL2-BM-max that provides φSSL2-BM-max satisfies
430(nm)≤λSSL2-RM-max≤480(nm).
[6] The light-emitting device according to any one of [1] to [5], wherein the light-emitting device satisfies Condition 6 below.
0.1800≤φSSL2-BG-min/φSSL2-BM-max≤0.8500. Condition 6
[7] The light-emitting device according to any one of [1] to [6], wherein a luminous efficacy of radiation KSSL2 (lm/W) in a wavelength range of 380 nm or more and 780 nm or less, which is derived from φSSL2(λ), satisfies Condition 7 below.
210.0lm/W≤KSSL2≤290.0lm/W. Condition 7
[8] The light-emitting device according to any one of [1] to [7], wherein at least one selected from the group consisting of the index Acg(φSSL2(λ)) represented by the formula (2-1) or (2-2), the correlated color temperature TSSL2(K) and the distance DuvφSSL2(λ)) from the black-body radiation locus can be changed.
[9] The light-emitting device according to [8], wherein a luminous flux and/or a radiant flux emitted from the light-emitting device in the main radiant direction can be independently controlled when at least one selected from the group consisting of the index Acg(φSSL2(λ)) represented by the formula (2-1) or (2-2), the correlated color temperature TSSL2 (K) and the distance DuvφSSL2(λ)) from the black-body radiation locus is changed.
[10] The light-emitting device according to any one of [1] to [9], wherein a maximum distance L between two arbitrary points on a virtual outer periphery enveloping the entire light-emitting areas closest to each other, is 0.4 mm or more and 200 mm or less.
[11] The light-emitting device according to any one of [1] to [10], including the light-emitting areas that allow φSSL2(λ) to further satisfy the following Conditions I to IV by changing a luminous flux amount and/or a radiant flux amount emitted from the light-emitting areas:
when a*nssL2 and b*nssL2 (where n is a natural number from 1 to 15) respectively denote the a* value and b* value in the CIE 1976 L*a*b* color space of the following 15 Munsell renotation color samples of #01 to #15 based on a mathematical assumption that illumination is performed by the light emitted in the radiant direction, and
when a*nref2 and b*nref2 (where n is a natural number from 1 to 15) respectively denote the a* value and b* value in the CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples based on a mathematical assumption that illumination is performed by reference light which is selected in accordance with the correlated color temperature TSSL2 (K) of the light emitted in the radiant direction, each saturation difference ΔCnSSL2 satisfies
−4.00≤αCnSSL2≤8.00 (where n is a natural number from 1 to 15),
an average saturation difference SATave (φSSL2(λ)) represented by the following formula (2-3) satisfies 0.50≤SATave(φSSL1(λ))≤4.00,
when a maximum saturation difference value is denoted by ΔCSSL-max2 and a minimum saturation difference value is denoted by ΔCSSL-min2, a difference |ΔCSSL-max2−ΔCSSL-min2| between the maximum saturation difference value and the minimum saturation difference value satisfies
2.00≤|ΔCmax−ΔCmin|≤10.00,
where ΔCnSSL2=√{(a*nSSL2)2+(b*nSSL2)2}−√{(a*nref2)2+(b*nref2)2}
with the 15 Munsell renotation color samples being:
when θnSSL2 (degrees) (where n is a natural number from 1 to 15) denotes a hue angle in the CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples based on a mathematical assumption that illumination is performed by the light emitted in the radiant direction, and
when θnref2 (degrees) (where n is a natural number from 1 to 15) denotes a hue angle in the CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples based on a mathematical assumption that illumination is performed by reference light which is selected in accordance with the correlated color temperature TSSL2 of the light emitted in the radiant direction, an absolute value of each difference in hue angles |ΔhnSSL2| satisfies
0.00 degree≤|ΔhnSSL2|≤9.0 degree(where n is a natural number from1to15),
where Δhn=θnSSL2−θnref2.
[12] The light-emitting device according to any one of [1] to [11], wherein a correlated color temperature TSSL2 (K) of light emitted from the light-emitting device in the radiant direction satisfies
2600K≤TSSL2≤7700K.
[13] The light-emitting device according to any one of [1] to [12], including light-emitting areas so that the φSSL2(λ) can satisfy the Conditions 1 to 4 by changing a luminous flux amount and/or a radiant flux amount emitted from the light-emitting areas.
[14] A method for designing a light-emitting device which includes M number of light-emitting areas (M is 2 or greater natural number), and has a blue semiconductor light-emitting element, a green phosphor, and a red phosphor as light-emitting elements in at least one of the light-emitting areas,
the method comprising designing the light-emitting areas such that, when φSSL2(λ) (N is 1 to M) is a spectral power distribution of a light emitted from each light-emitting area in a main radiant direction of the light-emitting device, and φSSL2(λ), which is a spectral power distribution of all the lights emitted from the light-emitting device in the radiant direction, is represented by
φSSL2(λ) satisfies the following Conditions 1 to 4: Condition 1:
a distance DuvφSSL2(λ)) of the spectral power distribution φSSL2(λ) of light from a black-body radiation locus defined by ANSI C78.377 satisfies
−0.0220≤Duv(φSSL2(λ))≤−0.0070;
φSSL2(λ) denotes a spectral power distribution of light emitted from the light-emitting device in the radiant direction,
φref2(λ) denotes a spectral power distribution of reference light which is selected in accordance with a correlated color temperature TSSL2 of the light emitted from the light-emitting device in the radiant direction,
(XSSL2, YSSL2, ZSSL2) denote tristimulus values of the light emitted from the light-emitting device in the radiant direction, and
(Xref2, Yref2, Zref2) denote tristimulus values of the reference light which is selected in accordance with the correlated color temperature TSSL2 (K) of the light emitted from the light-emitting device in the radiant direction, and
a normalized spectral power distribution SSSL2(λ) of the light emitted from the light-emitting device in the radiant direction,
a normalized spectral power distribution Sref2(λ) of the reference light which is selected in accordance with the correlated color temperature TSSL2 (K) of the light emitted from the light-emitting device in the radiant direction, and
a difference ΔSSSL2(λ) of between normalized spectral power distributions are respectively defined as
S
SSL2(λ)=φSSL2(λ)/YSSL2
S
ref2(λ)=φref2(λ)/Yref2and
ΔSSSL2(λ)=Sref2(λ)−SSSL2(λ) and
in a case where λSSL2-RL-max (nm) represents a wavelength that provides a longest wavelength local maximum value of SSSL2(λ) in a wavelength range of 380 nm or more and 780 nm or less, and when a wavelength Λ4 that is represented by SSSL2(λSSL2-RL-max)/2 exists on a longer wavelength-side of λSSL2-RL-max,
an index Acg(φSSL2(λ)) represented by the following formula (2-1) satisfies
−10.0<Acg(φSSL2(λ))≤120.0,
but
in a case where λSSL2-RL-max (nm) represents a wavelength that provides the longest wavelength local maximum value of SSSL2(λ) in a wavelength range of 380 nm or more and 780 nm or less, and when the wavelength Λ4 that is represented by SSSL2 (λSSL2-RL-max)/2 does not exist on the longer wavelength-side of λSSL2-RL-max,
an index Acg(φSSL2(λ)) represented by the following formula (2-2) satisfies
−10.0<Acg(φSSL2(λ))≤120.0,
[Expression 15]
A
cg(ϕSSL2(λ))=∫380495ΔSSSL2(λ)dλ+∫495590(−ΔSSSL2(λ))dλ+∫590Λ4ΔSSSL2(λ)dλ (2- 1)
[Expression 16]
A
cg(ϕSSL2(λ))=∫380495ΔSSSL2(λ)dλ+∫495590(−ΔSSSL2(λ))dλ+∫590780ΔSSSL2(λ)dλ (2-2)
when a maximum value of spectral intensity in a range of 430 nm or more and 495 nm or less is defined as φSSL2-BM-max and a minimum value of spectral intensity in a range of 465 nm or more and 525 nm or less is defined as φSSL2-BG-max, the spectral power distribution φSSL2(λ) of light satisfies
0.2250≤φSSL2-BG-min/φSSL2-BM-max≤0.7000; and
in the spectral power distribution φSSL2(λ) of light, when a maximum value of spectral intensity in a range of 590 nm or more and 780 nm or less is defined as φSSL2-RM-max, a wavelength λSSL2-RM-max that provides φSSL2-RM-max, satisfies
605(nm)≤λSSL2-RM-max≤653(nm).
[15] The method for designing a light-emitting device according to [14], wherein all of φSSL2N(λ) (N is 1 to M) satisfies the Conditions 1 to 4.
[16] The method for designing a light-emitting device according to [14] or [15], wherein at least one light-emitting area of the M number of light-emitting areas has wiring that allows the light-emitting area to be electrically driven independently from other light-emitting areas.
[17] The method for designing a light-emitting device according to [16], wherein all the M numbers of light-emitting areas each have wiring that allows the light-emitting area to be electrically driven independently from other light-emitting areas.
[18] The method for designing a light-emitting device according to any one of [14] to [18], wherein the method satisfies Condition 5 below.
In the spectral power distribution φSSL2(λ) of light described above, a wavelength λSSL2-BM-max that provides φSSL2-BM-max satisfies
430(nm)≤λSSL2-RM-max≤480(nm).
[19] The method for designing a light-emitting device according to any one of [14] to [18], wherein the method satisfies Condition 6 below.
0.1800≤φSSL2-BG-min/φSSL2-RM-max≤0.8500. Condition 6
[20] The method for designing a light-emitting device according to any one of [14] to [19], wherein a luminous efficacy of radiation KSSL2(lm/W) in a wavelength range of 380 nm or more and 780 nm or less, which is derived from φSSL2(λ), satisfies Condition 7 below.
210.0lm/W≤KSSL2≤290.0lm/W. Condition 7
[21] The method for designing a light-emitting device according to any one of [14] to [20], wherein at least one selected from the group consisting of the index Acg(φSSL2(λ)) represented by the formula (2-1) or (2-2), the correlated color temperature TSSL2(K) and the distance DuvφSSL2(λ)) from the black-body radiation locus can be changed.
[22] The method for designing a light-emitting device according to [21], wherein a luminous flux and/or a radiant flux emitted from the light-emitting device in the main radiant direction can be independently controlled when at least one selected from the group consisting of the index Acg(φSSL2(λ)) represented by the formula (2-1) or (2-2), the correlated color temperature TSSL2(K) and the distance DuvφSSL2(λ)) from the black-body radiation locus is changed.
[23] The method for designing a light-emitting device according to any one of [14] to [22], wherein a maximum distance L between two arbitrary points on a virtual outer periphery enveloping the entire light-emitting areas closest to each other, is 0.4 mm or more and 200 mm or less.
[24] The method for designing a light-emitting device according to any one of [14] to [23], further comprising allowing φSSL2(λ) to further satisfy the following Conditions I to IV by changing a luminous flux amount and/or a radiant flux amount emitted from the light-emitting areas:
when a*nssL2 and b*nssL2 (where n is a natural number from 1 to 15) respectively denote the a* value and b* value in the CIE 1976 L*a*b* color space of the following 15 Munsell renotation color samples of #01 to #15 based on a mathematical assumption that illumination is performed by the light emitted in the radiant direction, and
when a*nref2 and b*nref2 (where n is a natural number from 1 to 15) respectively denote the a* value and b* value in the CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples based on a mathematical assumption that illumination is performed by reference light which is selected in accordance with the correlated color temperature T (K) of the light emitted in the radiant direction, each saturation difference ΔCnSSL2 satisfies
−4.00≤ΔCnSSL2≤8.00(where n is a natural number from1to15),
an average saturation difference SATave(φSSL2(λ)) represented by formula (2-3) satisfies 0.50≤SATave(φSSL2(λ))≤4.00,
when a maximum saturation difference value is denoted by ΔCSSL-max2 and a minimum saturation difference value is denoted by ΔCSSL-min2, a difference |ΔCSSL-max2−ΔCSSL-min1| between the maximum saturation difference value and the minimum saturation difference value satisfies
2.00≤|ΔCSSL-max2−ΔCSSL-min2|≤10.00,
where ΔCnSSL2=√{(a*nSSL2)2+(b*nSSL2)2}−√{(a*nref2)2+(b*nref2)2}
with the 15 Munsell renotation color samples being:
when θnSSL2 (degrees) (where n is a natural number from 1 to 15) denotes a hue angle in the CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples based on a mathematical assumption that illumination is performed by the light emitted in the radiant direction, and
when θnref2 (degrees) (where n is a natural number from 1 to 15) denotes a hue angle in the CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples based on a mathematical assumption that illumination is performed by reference light which is selected in accordance with the correlated color temperature TSSL2 (K) of the light emitted in the radiant direction, an absolute value of each difference in hue angles |ΔhnSSL2| satisfies
0.00 degree≤|ΔhnSSL2|≤12.50 degrees (where n is a natural number from 1 to 15),
where ΔhnSSL2=θnSSL2−θnref2.
[25] The method for designing a light-emitting device according to any one of [14] to [24], wherein the correlated color temperature TSSL2 (K) of light emitted from the light-emitting device in the radiant direction satisfies
2600K≤TSSL2≤7700K.
[26] The method for designing a light-emitting device according to any one of [14] to [25], wherein
the method comprises designing the light-emitting areas so that φSSL2(λ) satisfies the Conditions 1 to 4 described earlier by changing an amount of luminous flux and/or an amount of radiant flux emitted from the light-emitting areas.
[27] A method for driving a light-emitting device which includes M number of light-emitting areas (M is 2 or greater natural number), and has a blue semiconductor light-emitting element, a green phosphor, and a red phosphor as light-emitting elements in at least one of the light-emitting areas,
the method comprising supplying power to each light-emitting area such that, when φSSL2(λ) (N is 1 to M) is a spectral power distribution of a light emitted from each light-emitting area in a main radiant direction of the light-emitting device, and φSSL2(λ), which is a spectral power distribution of all the lights emitted from the light-emitting device in the radiant direction, is represented by
φSSL2(λ) satisfies the following Conditions 1 to 4:
a distance DuvφSSL2(λ)) of the spectral power distribution φSSL2(λ) of light from a black-body radiation locus defined by ANSI C78.377 satisfies
−0.0220≤Duv(φSSL2(λ))≤−0.0070;
φSSL2(λ) denotes a spectral power distribution of light emitted from the light-emitting device in the radiant direction,
φref2(λ) denotes a spectral power distribution of reference light which is selected in accordance with a correlated color temperature TSSL2 (K) of the light emitted from the light-emitting device in the radiant direction,
(XSSL2, YSSL2, ZSSL2) denote tristimulus values of the light emitted from the light-emitting device in the radiant direction, and
(Xref2, Yref2, Zref2) denote tristimulus values of the reference light which is selected in accordance with the correlated color temperature TSSL2 (K) of the light emitted from the light-emitting device in the radiant direction, and
a normalized spectral power distribution SSSL2(λ) of the light emitted from the light-emitting device in the radiant direction,
a normalized spectral power distribution Sref2(λ) of the reference light which is selected in accordance with the correlated color temperature TSSL2 (K) of the light emitted from the light-emitting device in the radiant direction, and
a difference ΔSSSL2(λ) of between normalized spectral power distributions are respectively defined as
S
SSL2(λ)=φSSL2(λ)/YSSL2,
S
ref2(λ)=φref2(λ)/Yref2and
ΔSSSL2(λ)=Sref2(λ)−SSSL2(λ) and
in a case where λSSL2-RL-max (nm) represents a wavelength that provides a longest wavelength local maximum value of SSSL2(λ) in a wavelength range of 380 nm or more and 780 nm or less, and when a wavelength Λ4 that is represented by SSSL2(λSSL2-RL-max)/2 exists on a longer wavelength-side of λSSL2-RL-max,
an index Acg(φSSL2(λ)) represented by the following formula (2-1) satisfies
−10.0<Acg(φSSL2(λ))≤120.0,
but
in a case where λSSL2-RL-max (nm) represents a wavelength that provides the longest wavelength local maximum value of SSSL2(λ) in a wavelength range of 380 nm or more and 780 nm or less, and when the wavelength Λ4 that is represented by SSSL2(λSSL2-RL-max)/2 does not exist on the longer wavelength-side of λSSL2-RL-max,
an index Acg(φSSL2(λ)) represented by the following formula (2-2) satisfies
−10.0<Acg(φSSL2(λ))≤120.0,
[Expression 19]
A
cg(ϕSSL2(λ))=∫380495ΔSSSL2(λ)dλ+∫495590(−ΔSSSL2(λ))dλ+∫590Λ4ΔSSSL2(λ)dλ (2- 1)
[Expression 20]
A
cg(ϕSSL2(λ))=∫380495ΔSSSL2(λ)dλ+∫495590(−ΔSSSL2(λ))dλ+∫590780ΔSSSL2(λ)dλ (2-2)
when a maximum value of spectral intensity in a range of 430 nm or more and 495 nm or less is defined as φSSL2-BM-max and a minimum value of spectral intensity in a range of 465 nm or more and 525 nm or less is defined as φSSL2-BG-min, the spectral power distribution φSSL2(λ) of light satisfies
0.2250≤φSSL2-BG-min/φSSL2-BM-max≤0.7000; and
in the spectral power distribution φSSL2(λ) of light, when a maximum value of spectral intensity in a range of 590 nm or more and 780 nm or less is defined as φSSL2-RM-max, a wavelength λSSL2-RM-max that provides φSSL2-RM-max satisfies
605(nm)≤λSSL2-RM-max≤653(nm).
[28] The method for driving a light-emitting device according to [27], wherein power is supplied to the light-emitting areas so that all of φSSL2N(λ) (N is 1 to M) satisfies the Conditions 1 to 4.
[29] The method for driving a light-emitting device according to [27] or [28], wherein at least one light-emitting area of the M number of light-emitting areas is electrically driven independently from other light-emitting areas.
[30] The method for driving a light-emitting device according to any one of [27] to [29], wherein all the M number of light-emitting areas are electrically driven independently from other light-emitting areas.
[31] The method for driving a light-emitting device according to any one of [27] to [30], wherein the method satisfies Condition 5 below.
Condition 5:
In the spectral power distribution φSSL2(λ) of light described above, a wavelength λSSL2-BM-max that provides φSSL2-BM-max satisfies
430(nm)≤λSSL2-RM-max≤480(nm).
[32] The method for driving a light-emitting device according to any one of [27] to [31], wherein the method satisfies Condition 6 below.
0.1800≤φSSL2-BG-min/φSSL2-RM-max≤0.8500. Condition 6
[33] The method for driving a light-emitting device according to any one of [27] to [32], wherein a luminous efficacy of radiation KSSL2(lm/W) in a wavelength range of 380 nm or more and 780 nm or less, which is derived from φSSL2(λ), satisfies Condition 7 below.
210.0lm/W≤KSSL2≤290.0lm/W. Condition 7
[34] The method for driving a light-emitting device according to any one of [27] to [33], wherein at least one selected from the group consisting of the index Acg(φSSL2(λ)) represented by the formula (2-1) or (2-2), the correlated color temperature TSSL2 (K) and the distance DuvφSSL2(λ)) from the black-body radiation locus is changed.
[35] The method for driving a light-emitting device according to [34], wherein a luminous flux and/or a radiant flux emitted from the light-emitting device in the main radiant direction is unchanged when at least one selected from the group consisting of the index Acg(φSSL2(λ)) represented by the formula (2-1) or (2-2), the correlated color temperature TSSL2 (K) and the distance DuvφSSL2(λ)) from the black-body radiation locus is changed.
[36] The method for driving a light-emitting device according to [34], wherein a luminous flux and/or a radiant flux emitted from the light-emitting device in the main radiant direction is decreased when the index Acg(φSSL2(λ)) represented by the formula (2-1) or (2-2) is decreased.
[37] The method for driving a light-emitting device according to [34], wherein a luminous flux and/or a radiant flux emitted from the light-emitting device in the main radiant direction is increased when the correlated color temperature TSSL2 (K) is increased.
[38] The method for driving a light-emitting device according to [34], wherein a luminous flux and/or a radiant flux emitted from the light-emitting device in the main radiant direction is decreased when the distance DuvφSSL2(λ)) from the black-body radiation locus is decreased.
[39] The method for driving a light-emitting device according to any one of [27] to [38],
further comprising supplying power such that φSSL2(λ) further satisfies the following Conditions I to IV:
when a*nssL2 and b*nssL2 (where n is a natural number from 1 to 15) respectively denote the a* value and b* value in the CIE 1976 L*a*b* color space of the following 15 Munsell renotation color samples of #01 to #15 based on a mathematical assumption that illumination is performed by the light emitted in the radiant direction, and
when a*nref2 and b*nref2 (where n is a natural number from 1 to 15) respectively denote the a* value and b* value in the CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples based on a mathematical assumption that illumination is performed by reference light which is selected in accordance with the correlated color temperature TSSL2 (K) of the light emitted in the radiant direction, each saturation difference ΔCnSSL2 satisfies
−4.00≤ΔCnSSL2≤8.00(where n is a natural number from1to15),
an average saturation difference SATave(φSSL2(λ)) represented by formula (2-3) satisfies 0.50≤SATave(φSSL2(λ))≤4.00,
when a maximum saturation difference value is denoted by ΔCSSL-max2 and a minimum saturation difference value is denoted by ΔCSSL-min2, a difference |ΔCSSL-max2−ΔCSSL-min1| between the maximum saturation difference value and the minimum saturation difference value satisfies
2.00≤|ΔCSSL-max2−ΔCSSL-min2|≤10.00,
where ΔCnSSL2=√{(a*nSSL2)2+(b*nSSL2)2}−√{(a*nref2)2+(b*nref2)2}
with the 15 Munsell renotation color samples being:
when θnSSL2 (degrees) (where n is a natural number from 1 to 15) denotes a hue angle in the CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples based on a mathematical assumption that illumination is performed by the light emitted in the radiant direction, and
when θnref2 (degrees) (where n is a natural number from 1 to 15) denotes a hue angle in the CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples based on a mathematical assumption that illumination is performed by reference light which is selected in accordance with the correlated color temperature TSSL2 (K) of the light emitted in the radiant direction, an absolute value of each difference in hue angles |ΔhnSSL2| satisfies
0.00 degree≤|ΔhnSSL2|≤12.50 degrees (where n is a natural number from 1 to 15),
where ΔhnSSL2=θnSSL2−θnref2.
[40] An illumination method comprising:
illuminated objects preparation step of preparing illuminated objects; and
an illumination step of illuminating the objects by light emitted from a light-emitting devices which includes M number of light-emitting areas (M is 2 or greater natural number), and has a blue semiconductor light-emitting element, a green phosphor, and a red phosphor as light-emitting elements in at least one of the light-emitting areas,
in the illumination step, when light emitted from the light-emitting devices illuminate the objects, the objects are illuminated so that the light measured at a position of the objects satisfies Condition 1 and Conditions I to IV below:
a distance DuvφSSL2(λ)) from a black-body radiation locus as defined by ANSI C78.377 of the light measured at the position of the objects satisfies
−0.0220≤Duv(φSSL2(λ))≤−0.0070;
if an a* value and a b* value in CIE 1976 L*a*b* color space of 15 Munsell renotation color samples from #01 to #15 listed below when mathematically assuming illumination by the light measured at the position of the objects are respectively denoted by a*nssL2 and b*nssL2 (where n is a natural number from 1 to 15), and
if an a* value and a b* value in CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples when mathematically assuming illumination by a reference light that is selected according to a correlated color temperature TSSL2 (K) of the light measured at the position of the objects are respectively denoted by a*nref2 and b*nref2 (where n is a natural number from 1 to 15), then each saturation difference ΔCnSSL2 satisfies
−4.00≤ΔCnSSL2≤8.00(where n is a natural number from1to15);
an average saturation difference SATave(φSSL2(λ)) represented by formula (2-3) satisfies 0.50≤SATave(φSSL2(λ))≤4.00,
when a maximum saturation difference value is denoted by ΔCSSL-max2 and a minimum saturation difference value is denoted by ΔCSSL-min2, a difference |ΔCSSL-max2−ΔCSSL-min2| between the maximum saturation difference value and the minimum saturation difference value satisfies
2.00≤|ΔCSSL-max2−ΔCSSL-min2|≤10.00,
where ΔCnSSL2=√{(a*nSSL2)2+(b*nSSL2)2}−√{(a*nref2)2+(b*nref2)2}
with the 15 Munsell renotation color samples being:
if hue angles in CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples when mathematically assuming illumination by the light measured at the position of the objects are denoted by θnSSL2 (degrees) (where n is a natural number from 1 to 15), and
if hue angles in CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples when mathematically assuming illumination by a reference light that is selected according to the correlated color temperature TSSL2 (K) of the light measured at the position of the objects are denoted by θnref2 (degrees) (where n is a natural number from 1 to 15), then an absolute value of each difference in hue angles |ΔhnSSL2| satisfies
0.00 degree≤|ΔhnSSL2|≤12.50 degrees (where n is a natural number from 1 to 15),
here ΔhnSSL2=θnSSL2−θnref2.
[41] The illumination method according to [40], wherein when φSSL2N(λ) (N is 1 to M) is a spectral power distribution of a light which has been emitted from each light-emitting element and has reached the position of the objects, and φSSL2(λ) is a spectral power distribution of the light measured at the position of the objects is represented by
all the φSSL2N(λ) (N is 1 to M) can satisfy the Condition 1 and the Conditions I to IV.
[42] The illumination method according to [40] or [41], wherein at least one light-emitting area of the M number of light-emitting areas is electrically driven independently from other light-emitting areas for performing the illumination.
[43] The illumination method according to [42], wherein all the M number of light-emitting areas are electrically driven independently from other light-emitting areas.
[44] The illumination method according to any one of [40] to [43], wherein at least one selected from the group consisting of an average saturation difference SATave(φSSL2(λ)) represented by the formula (2-3), the correlated color temperature TSSL2(K), and the distance DuvφSSL2(λ)) from the black-body radiation locus is changed.
[45] The illumination method according to [44], wherein the luminance in the object is independently controlled when at least one selected from the group of an average saturation difference SATave(φSSL2(λ)) represented by the formula (2-3), the correlated color temperature TSSL2(K), and the distance DuvφSSL2(λ)) from the black-body radiation locus is changed.
[46] The illumination method according to [45], wherein the luminance in the object is unchangeable when at least one selected from the group of an average saturation difference SATave(φSSL2(λ)) represented by the formula (2-3), the correlated color temperature TSSL2 (K), and the distance DuvφSSL2(λ)) from the black-body radiation locus is changed.
[47] The illumination method according to [45], wherein the luminance in the object is decreased when the average saturation difference SATave(φSSL2(λ)) represented by the formula (2-3) is increased.
[48] The illumination method according to [45], wherein the illuminance in the object is increased when the correlated color temperature TSSL2(K) is increased.
[49] The illumination method according to [45], wherein the luminance in the object is decreased when the distance Duv (φSSL2 (λ)) from the black-body radiation locus is decreased. [50] The illumination method according to any one of [40] to [49], wherein
if a maximum distance between two arbitrary points on a virtual outer periphery enveloping the entire light-emitting areas closest to each other is denoted by L, and a distance between the light-emitting device and the illumination object is denoted by H,
5×L≤H≤500×L.
According to the second invention of the present invention, both favorable color appearance and high light source efficiency can be achieved in “a light-emitting device capable of realizing a natural, vivid, highly visible and comfortable appearance of colors or an appearance of objects”.
The conveniences implemented by the second invention of the present invention follow.
In other words, optimum illumination differs depending on age, gender, country and the like, or depending on the space and the purpose of illumination, but if the light-emitting device according to the second invention of the present invention, or the method for driving the light-emitting device according to the second invention of the present invention is used, more suitable illumination conditions can be easily selected from a variable range.
Hereinafter, while the second invention of the present invention will be described in detail, the following description presents differences from the description of the second invention of the present invention. For descriptions common to the first invention and the second invention of the present invention, the description of the first invention of the present invention provided earlier will apply.
While the second invention of the present invention will be described in detail hereinafter, it is to be understood that the second invention of the present invention is not limited to the embodiments described below and that various modifications can be made without departing from the spirit and scope of the invention.
Moreover, in a light-emitting device according to the first to third aspects of the second invention of the present invention specify the invention based on light in a “main radiant direction” among light emitted from a light-emitting device. Therefore, light-emitting devices capable of radiating light including light in a “main radiant direction” which meets requirements of the second invention of the present invention are to be included in the spirit and scope of the second invention of the present invention.
In addition, an illumination method according to the fourth aspect of the second invention of the present invention specifies the invention based on light at a position where an object is illuminated in a case where light emitted from a light-emitting device used in the illumination method illuminates the object. Therefore, illumination methods used by light-emitting devices capable of emitting light at a “position where an object is illuminated” which meets requirements of the second invention of the present invention are to be included in the spirit and scope of the second invention of the present invention.
The spectral power distribution of light emitted from a light-emitting device in the main radiant direction according to the second invention of the present invention is preferably measured at a distance where luminance at a measurement point is practical luminance (as will be described later, 150 lx or higher and 5000 lx or lower).
The light-emitting device according to the first aspect of the second invention of the present invention includes M number of light-emitting areas (M is 2 or greater natural number). In this description, light-emitting areas that emit light in an equivalent spectral power distribution (allowing a general dispersion generated in the manufacturing steps) are called the “same type of light-emitting areas”. In other words, even if the light-emitting areas are physically separated and disposed with a distance, these light-emitting areas are of a same type if they emit lights in an equivalent spectral power distribution (allowing a general dispersion generated in the manufacturing steps). This means that the light-emitting device, according to the first aspect of the second invention of the present invention, includes two or more types of light-emitting areas from which lights in mutually different spectral power distributions are emitted.
At least one light-emitting area of the plurality of types of light-emitting areas includes a blue semiconductor light-emitting element, a green phosphor, and a red phosphor as the light-emitting element. Only if at least one light-emitting area includes a blue semiconductor light-emitting element, a green phosphor, and a red phosphor as the light-emitting element, the light-emitting elements included in each light-emitting area are not limited. The light-emitting elements, other than the semiconductor light-emitting element and the phosphors, can be any light-emitting element if various supplied energies can be converted into electromagnetic radiation energy, and the electromagnetic radiation energy includes visible light in a range from 380 nm to 780 nm. For example, a hot filament, a fluorescent tube, a high pressure sodium lamp, a laser, and a secondary harmonic generation (SHG) source that can convert electric energy can be used.
The configuration of the light-emitting device according to the first aspect of the second invention of the present invention is not especially limited, only if a plurality of light-emitting areas, including a light-emitting area which has a blue semiconductor light-emitting element, a green phosphor, and a red phosphor as the light-emitting element, exists therein. An individual semiconductor light-emitting element to which a lead or the like as a conducting mechanism is added or a packaged LED to which a heat dissipating mechanism is further added and integrated with a phosphor or the like may be adopted as the light-emitting area.
In addition, the light-emitting device can be an LED module in which a robust heat dissipating mechanism is added to one or more packaged LEDs and which is generally mounted with a plurality of packaged LEDs may be adopted as the light-emitting device. Furthermore, an LED lighting fixture in which a lens, a reflecting mechanism, and the like are added to a packaged LED may be adopted. Moreover, a lighting system which supports a large number of LED lighting fixtures or the like and which is configured to be capable of illuminating an object may be adopted. The light-emitting device according to the first aspect of the second invention of the present invention encompasses all of the above.
In the light-emitting device according to the first aspect of the second invention of the present invention, when φSSL2N(λ) (N is in the 1 to M range) is the spectral power distribution of the light emitted from each light-emitting area, φSSL2(λ), which is the spectral power distribution of all the lights emitted from the light-emitting device in the radiant direction, is represented by
This will be described with reference to
The light-emitting device 200 in
When φSSL21(λ) is the spectral power distribution of the light emitted from the light-emitting area 201, φSSL22(λ) is the spectral power distribution of the light emitted from the light-emitting area 202, φSSL23(λ) is the spectral power distribution of the light emitted from the light-emitting area 203, φSSL24(λ) is the spectral power distribution of the light emitted from the light-emitting area 204, and φSSL25(λ) is the spectral power distribution of the light emitted from the light-emitting area 205, then the spectral power distribution φSSL2(λ) of all the lights emitted from the light-emitting device in the radiant direction is represented by
In other words, when N is 1 to M, φSSL2(λ) can be represented by
According to the second invention of the present invention, light source efficiency is improved and color appearance can be made variable while realizing a natural, vivid, highly visible and comfortable appearance of colors and appearance of objects as if the objects are seen outdoors. In concrete terms, the light-emitting device, including light-emitting areas that can satisfy predetermined conditions by changing the luminous flux amount and/or radiant flux amount emitted from each light-emitting area, is provided.
Hereinafter, the second invention of the present invention will be described in detail.
The present inventor has discovered a radiometric property or a photometric property common to spectra or spectral power distributions capable of realizing a color appearance or an object appearance which is as natural, vivid, highly visible, and comfortable as though perceived outdoors in a high-illuminance environment even in an ordinary indoor illuminance environment. The present inventor further ascertained, from a colorimetric perspective, in what way the color appearance of the color samples having specific spectral reflectance characteristics when assuming that the color is illuminated by light having the aforementioned spectrum or spectral power distribution changes (or does not change) when the object described above is achieved in comparison with a case where illumination by calculational reference light is assumed, and collectively reached the present invention. In addition, the invention described above was improved from the perspective of light source efficiency to arrive at a light-emitting device having high light source efficiency. In addition, the present inventor discovered that the appearance of colors can be variable if a plurality of light-emitting areas is included.
<Emission by Single Light-Emitting Element and Emission by Light-Emitting Device>
A light-emitting device according to a first aspect of the second invention of the present invention includes a plurality of light-emitting areas and may be, for example, a packaged LED including a semiconductor light-emitting element and a phosphor, an LED light bulb including a packaged LED, or a light-emitting module, a light-emitting system, or the like which integrates such light-emitting devices. Hereinafter, a member/material which constitutes a light-emitting device according to the first aspect of the second invention of the present invention and which is capable of emitting light either spontaneously or as a result of being excited by another member/material will be described as a light-emitting element. Therefore, in the first aspect of the second invention of the present invention, a semiconductor light-emitting element, a phosphor, and the like may be light-emitting elements.
On the other hand, a spectral power distribution φSSL2(λ) of the light-emitting device itself according to the first aspect of the second invention of the present invention is based on characteristics when power is being continuously supplied thereto and is characterized by the following indexes.
Specifically, the spectral power distribution φSSL2(λ) of the light-emitting device is characterized by a maximum value φSSL2-BM-max of spectral intensity and a wavelength λSSL2-BM-max that provides the maximum value φSSL2-BM-max of spectral intensity in a range of 430 nm or more and 495 nm or less,
a minimum value φSSL2-BG-max of spectral intensity and a wavelength λSSL2-BG-max that provides the minimum value φSSL2-BG-max of spectral intensity in a range of 465 nm or more and 525 nm or less,
a maximum value λSSL2-RM-max of spectral intensity and a wavelength λSSL2-RM-max that provides the maximum value λSSL2-RM-max of spectral intensity in a range of 590 nm or more and 780 nm or less, and
λSSL2-RL-max that provides a longest wavelength local maximum value φSSL2-RL-max of a normalized spectral power distribution SSSL2(λ) which is derived from the spectral power distribution φSSL2(λ) in a range of 380 nm or more and 780 nm or less which is used in the definition of an index Acg(φSSL2(λ)) to be described later.
Therefore, for example, λCHIP-BM-dom generally differs from λSSL2-BM-max and λPHOS-RM-max also generally differs from λSSL2-RM-max On the other hand, λSSL2-RL-max may sometimes assume a same value as λSSL2-RM-max.
<Index Acg(φSSL2(λ))>
The index Acg(φSSL2(λ) is defied as below, as disclosed as the index Acg in Japanese Patent No. 5252107 and Japanese Patent No. 5257538.
Let φref2(λ) and φSSL2(λ) respectively denote spectral power distributions of calculational reference light and test light which represent color stimuli that differ from one another when measuring light emitted in a main radiant direction from a light-emitting device of the first aspect of the second invention of the present invention, x(λ), y(λ), and z(λ) denote a color-matching function, and (Xref2, Yref2, Zref2) and (XSSL1, YSSL2, ZSSL2) respectively denote tristimulus values corresponding to the calculational reference light and the test light. In this case, the following is satisfied regarding the calculational reference light and the test light, where k denotes a constant.
Y
ref2
=k∫φ
ref2(λ)·y(λ)dλ
Y
SSL2
=k∫φ
SSL2(λ)·y(λ)dλ
At this point, normalized spectral power distributions obtained by normalizing the spectral power distributions of the calculational reference light and the test light by their respective Y were defined as
S
ref2(λ)=φref2(λ)/Yref2and
S
SSL2(λ)=φSSL2(λ)/YSSL2,
and a difference between the normalized reference light spectral power distribution and the normalized test light spectral power distribution was represented by
ΔSSSL2(λ)=Sref2(λ)−SSSL2(λ).
Furthermore, at this point, the index Acg(φSSL2(λ)) was defined as follows.
A
cg(ϕSSL2(λ))=∫Λ1Λ2ΔSSSL2(λ)dλ+∫Λ2Λ3(−ΔSSSL2(λ))dλ+∫Λ3Λ4ΔSSSL2(λ)dλ [Expression 27]
Moreover, upper and lower limit wavelengths of the integrals were respectively set to
Λ1=380 nm,
Λ2=495 nm, and
Λ3=590 nm.
In addition, Λ4 is defined by dividing Λ4 into the two cases described below. First, if a wavelength that provides a longest wavelength local maximum value in a range of 380 nm or more and 780 nm or less in a normalized test light spectral power distribution SSSL2(λ) is denoted by λSSL2-RL-max (nm) and a normalized spectral intensity thereof is denoted by SSSL2 (λSSL2-RL-max), then a wavelength which is on a longer wavelength-side of λSSL2-RL-max and which has an intensity of SSSL2 (λSSL2-RL-max)/2 is denoted as Λ4. If such a wavelength does not exist in a range up to 780 nm, then Λ4 is assumed to be 780 nm.
<φSSL2-BG-min/φSSL2-BM-max and φSSL2-BG-min/φSSL2-RM-max>
φSSL2-BG-min mainly appears in a portion where a longer wavelength-side tail (a base portion where spectral radiant flux intensity decreases) of a spectral radiant flux due to emission of light by a blue semiconductor light-emitting element and a shorter wavelength side tail (a base portion where spectral radiant flux intensity decreases) of a spectral radiant flux due to emission of light by a light-emitting element responsible for the intermediate wavelength region overlap with each other. In other words, φSSL2-BG-min often occurs as a recess with a shape of φSSL2(λ) in a range of 465 nm or more and 525 nm or less which straddles the short wavelength region and the intermediate wavelength region.
In order to relatively uniformly improve saturation of color appearance of the 15 specific mathematically-derived Munsell renotation color samples to be described later, φSSL2-BG-min/φSSL2-BM-max obtained by normalizing φSSL2-BG-min with a maximum value of spectral intensity in a range of 430 nm to 495 nm and φSSL2-BG-min/φSSL2-RM-max obtained by normalizing φSSL2-BG-min with a maximum value of spectral intensity in a range of 590 nm to 780 nm must be controlled with care. In other words, in the light-emitting device according to the first aspect of the second invention, φSSL2-BG-min/φSSL2-BM-max and φSSL2-BG-min/φSSL2-RM-max have optimum ranges as will be described later.
When the light-emitting device according to the first aspect of the second invention of the present invention emits test light in the main radiant direction, the a* values and the b* values of the 15 color samples in the CIE 1976 L*a*b* color space of the test light (related to the light-emitting device according to the first aspect of the second invention of the present invention) are to be respectively denoted by a*nSSL2 and b*nssL2 (where n is a natural number from 1 to 15), and hue angles of the 15 color samples are to be respectively denoted by θnSSL2 (degrees) (where n is a natural number from 1 to 15). In addition, when mathematically assuming illumination by a calculation reference light (black-body radiation light when lower than 5000 K and CIE daylight when equal to or higher than 5000 K) which is selected in accordance with the correlated color temperature TSSL2 of the test light described above, the a* values and the b* values of the 15 color samples in the CIE 1976 L*a*b* color space are to be respectively denoted by a*nref2 and b*nref2 (where n is a natural number from 1 to 15), and hue angles of the 15 color samples are to be respectively denoted by θnref2 (degrees) (where n is a natural number from 1 to 15). In this case, an absolute value |ΔhnSSL2| of each difference in hue angles ΔhnSSL2 (degrees) (where n is a natural number from 1 to 15) of each of the 15 Munsell renotation color samples when illuminated by the two types of light may be represented by
|ΔhnSSL2|=|θnSSL2−θnref2|.
In addition, each saturation difference ΔCnSSL2 (where n is a natural number from 1 to 15) of the 15 Munsell renotation color samples when assuming illumination by the test light and the calculation reference light is represented by
ΔCnSSL2=√{(a*nSSL2)2+(b*nSSL2)2}−√{(a*nref2)2+(b*nref2)2}.
Furthermore, an average saturation difference SATave(φSSL2(λ)) of the 15 Munsell renotation color samples is represented by the following formula (2-3)
Moreover, when a maximum saturation difference value of the 15 Munsell renotation color samples is denoted by ΔCSSL-max2 and a minimum saturation difference value is denoted by ΔCSSL-min2, a difference between a maximum saturation difference and a minimum saturation difference (difference among differences between maximum and minimum degrees of saturation) is represented by
|ΔCSSL-max2−ΔCSSL-min2|.
<Luminous Efficacy of Radiation KssL2 (Lm/W) and Luminous Efficacy of a Source ηssL2 (Lm/W)>
Furthermore, when evaluating the test light spectral power distribution φSSL2(λ) when measuring light emitted in a main radiant direction from a light-emitting device of the first aspect of the second invention of the present invention, the widely-used definition below was adopted for luminous efficacy of radiation KSSL2 (lm/W).
K
SSL2
=Km×[∫380780{ϕSSL2(λ)×V(λ)}dλ]/[∫380780ϕSSL2(λ)dλ] [Expression 29]
In the equation above,
Therefore, a luminous efficacy of radiation KSSL2 (lm/W) of a test light spectral power distribution φSSL2(λ) when measuring light in the main radiant direction emitted from the light-emitting device according to the first aspect of the second invention of the present invention can be described as efficiency inherent in the shape of the spectral power distribution.
On the other hand, light source efficiency ηSSL2 (lm/W) is a quantity indicating how much of power supplied to the light-emitting device according to the first aspect of the second invention of the present invention is converted into a luminous flux.
Furthermore, the luminous efficacy of radiation KSSL2 (lm/W) of a test light spectral power distribution φSSL2(λ) when measuring light in the main radiant direction emitted from the light-emitting device is efficiency inherent in the shape of the spectral power distribution itself and may be described as a quantity that equals light source efficiency ηSSL2 (lm/W) when assuming that characteristics of all materials constituting the light-emitting device (for example, internal quantum efficiency of semiconductor light-emitting elements, light extraction efficiency, internal quantum efficiency of phosphors, external quantum efficiency, and efficiency related to light transmission characteristics of encapsulants) have 100% efficiency.
<Conception of Invention Related to Light Source Efficiency>
The present inventor mathematically and experimentally evaluated whether or not both preferable color appearance and high light source efficiency can be achieved when the index Acg(φSSL2(λ)) has a value outside a range of −360 or more and −10 or less and particularly a value larger than −10. The description of the first invention of the present invention will be applied to this evaluation.
[Examination with Light-Emitting Device Including a Plurality of Light-Emitting Areas]
Hereinafter, the second invention of the present invention will be described in further detail with reference to experimental examples and the like.
In the experimental examples, the inventor assumed that the light-emitting device included a plurality of light-emitting areas, and examined how the appearance of colors of the light-emitting device change by adjusting the radiant flux amount (luminous flux amount) of each light-emitting area. In other words, the characteristics of numeric values, such as the index Acg(φSSL2(λ)), CCT (K), DuvφSSL2(λ)), the luminous efficacy of radiation KSSL2 (lm/W), λSSL2-BM-max, φSSL2-BG-min/φSSL2-BM-max, λSSL2-RM-max, and φSSL2-BG-min/φSSL2-RM-max of the light emitted from each light-emitting area and the light-emitting device in the main radiant direction, were extracted. At the same time, differences between color appearances of the 15 color samples when assuming illumination by calculational reference lights and color appearances of the 15 color samples when assuming a test light spectral power distribution actually measured were also compiled using |ΔhnSSL2|, SATave(φSSL2(λ)), ΔCnSSL2, and |ΔCSSL-max2−ΔCSSL-min2| as indices. Moreover, while values of |ΔhnSSL2| and ΔCnSSL2 vary when n is selected, in this case, maximum and minimum values are shown. These values are also described in Tables 2-16 to 2-22.
In concrete terms, the inventor experimented on how φSSL2(λ), which is the sum of the spectral power distribution of the light emitted from each light-emitting area in the main radiant direction, will change by changing the luminous flux amount and/or radiant flux amount emitted from each light-emitting area in the main radiant direction.
Experimental Example 201
A 5 mm diameter resin package 10 in which two light-emitting units exist, as shown in
Next, if the current value of the current supplied to each light-emitting area of the packaged LED 210, which includes the light-emitting area 211 and the light-emitting area 212, is appropriately adjusted, then five types of spectral power distributions shown in
The spectral power distributions in
At drive points A to E and in intervals between the drive points, both a natural, vivid, highly visible and comfortable appearance of colors and appearance of objects as if the objects are seen outdoors and high light source efficiency can conceivably be achieved. For example, between the drive point A and the drive point E, the correlated color temperature of the packaged LED can be variable in a 3207 K to 4204 K range, and Duv(φSSL2(λ)) can also be variable in the −0.0072 to −0.0155 range. Further, the average saturation difference of the 15 Munsell renotation color samples can also be variable in a 1.95 to 2.32 range while implementing such an appearance of colors. Accordingly, in an area where both a preferable appearance of colors and high light source efficiency can be achieved, illumination conditions that are conceivably more optimal can be readily selected from a variable range in accordance with the age, the gender or the like of a user of the light-emitting device or in accordance with a space, a purpose, or the like of the illumination.
In this case, the following drive control is also possible.
First, when at least one of the index Acg(φSSL2(λ)), correlated color temperature TSSL2 (K), and distance Duv(φSSL2(λ)) from the black-body radiation locus, is changed, the luminous flux and/or radiant flux emitted from the light-emitting device in the main radiant direction can be unchangeable. If this control is performed, a difference of appearance of colors, caused by a change of the shape of the spectral power distribution, can be easily checked without depending on the luminance of the illumination object, which is preferable.
Second, when the index Acg(φSSL2(λ)) is decreased in an appropriate range, the luminous flux and/or radiant flux of the light-emitting device can be decreased, so as to decrease the luminance of the illumination object.
Third, when Duv(φSSL2(λ)) is decreased in an appropriate range as well, the luminous flux and/or radiant flux of the light-emitting device can be decreased, so as to decrease the luminance of the illumination object. In the second and third cases, brightness is normally increased, hence energy consumption can be suppressed by decreasing luminance, which is preferable.
Fourth, when the correlated color temperature is increased, the luminous flux and/or radiant flux of the light-emitting device can be increased, so as to increase the luminance of the illumination object. Under a general illumination environment, a relatively low luminance environment is often felt to be comfortable when the color temperature is in a low range, and a relatively high luminance environment is often felt to be comfortable when the color temperature is in a high range. This psychological effect is known as the Kruithof Effect, and performing control integrating this effect is also possible, and when the correlated color temperature is increased, it is preferable to increase the luminance of the illumination object by increasing the luminous flux and/or radiant flux of the light-emitting device.
Experimental Example 202
A ceramic package, in which a 7 mm diameter light-emitting unit is divided into six sub-light-emitting units, as shown in
Next, if the current value of current injected into each light-emitting area of the packaged LED having the light-emitting area 221, the light-emitting area 222 and the light-emitting area 223 is appropriately adjusted, and four types of spectral power distributions shown in
The spectral power distribution in
At drive points A to C, both a natural, vivid, highly visible and comfortable appearance of colors and appearance of objects as if the objects are seen outdoors and high light source efficiency can conceivably be achieved. In addition, even at a drive point D which exists in a range enclosed by the drive points A to C, both a natural, vivid, highly visible and comfortable appearance of colors and appearance of objects as if the objects are seen outdoors and high light source efficiency can conceivably be achieved. Therefore, for example, in an area enclosed by the drive point A, the drive point B, and the drive point C as well as in a vicinity of the area, a correlated color temperature of the package LED is variable from 2934 K to 3926 K and Duv(φSSL2(λ)) is also variable from −0.0104 to −0.0073 while achieving the appearance of colors described above. Further, the average saturation difference of the 15 Munsell renotation color samples can also be variable in a 0.94 to 1.91 range. Accordingly, in an area where both a preferable appearance of colors and high light source efficiency can be achieved, illumination conditions that are conceivably more optimal can be readily selected from a variable range in accordance with the age, the gender or the like of a user of the light-emitting device or in accordance with a space, a purpose, or the like of the illumination.
This experimental example is especially preferable since one light-emitting device includes three types of light-emitting areas for which colors are adjusted differently, and the variable ranges can be wider compared with the case when one light-emitting device includes two types of light-emitting areas for which colors are adjusted differently.
In this case, the following drive control is also possible.
First, when at least one of the index Acg(φSSL2(λ)), correlated color temperature TSSL2 (K), and distance Duv(φSSL2(λ)) from the black-body radiation locus, is changed, the luminous flux and/or the radiant flux emitted from the light-emitting device in the main radiant direction can be unchangeable. If this control is performed, a difference of appearance of colors, caused by a change of the shape of the spectral power distribution, can be easily checked without depending on the luminance of the illumination object, which is preferable.
Second, when the index Acg(φSSL2(λ)) is decreased in an appropriate range, the luminous flux and/or radiant flux of the light-emitting device can be decreased, so as to decrease the luminance of the illumination object.
Third, when Duv(φSSL2(λ)) is decreased in an appropriate range as well, the luminous flux and/or radiant flux of the light-emitting device can be decreased, so as to decrease the luminance of the illumination object. In the second and third cases, brightness is normally increased, hence energy consumption can be suppressed by decreasing luminance, which is preferable.
Fourth, when the correlated color temperature is increased, the luminous flux and/or radiant flux of the light-emitting device can be increased, so as to increase the luminance of the illumination object. Under a general illumination environment, a relatively low luminance environment is often felt to be comfortable when the color temperature is in a low range, and a relatively high luminance environment is often felt to be comfortable when the color temperature is in a high range. This psychological effect is known as the Kruithof Effect, and performing control integrating this effect is also possible, and when the correlated color temperature is increased, it is preferable to increase the luminance of the illumination object by increasing the luminous flux and/or radiant flux of the light-emitting device.
Experimental Example 203
As shown in
Next, if the radiant fluxes of the LED light bulbs constituting the light-emitting area 231 and the light-emitting area 232 are appropriately adjusted using dimming controllers connected to the independent power supplies respectively, five types of spectral power distributions shown in
The CIELAB plot in each drawing indicates the a* values and the b* values which are plotted respectively: when 15 Munsell renotation color samples #01 to #15 are mathematically assumed as the illumination objects and these illumination objects are illuminated using this illumination system; and when these illumination objects are illuminated by a reference light derived from the correlated color temperature of the light-emitting device of this illumination system. Here the drive point names A to E are assigned to the radiant flux of the illumination system (light-emitting device) in descending order of contribution of the radiant flux of the LED light bulb constituting the light-emitting area 231.
The spectral power distributions in
Although at least one of φSSL2-BG-min/φSSL2-BM-max and φSSL2-RM-min is not within an appropriate range according to the second invention of the present invention at the drive points A and B, both a natural, vivid, highly visible and comfortable appearance of colors and appearance of objects as if the objects are seen outdoors and high light source efficiency can conceivably be achieved at the drive point C, the drive point D, and the drive point E as well as in intervals therebetween and in a vicinity thereof. For example, between the drive point C and the drive point E, the correlated color temperature of the illumination system can be variable in a 3146 K to 3544 K range, and Duv(φSSL2(λ)) can also be variable in a −0.0121 to −0.0116 range, while implementing the above mentioned appearance of colors. Further, the average saturation difference of the 15 Munsell renotation color samples can also be variable in a 1.65 to 2.17 range. Accordingly, in an area where both a preferable appearance of colors and high light source efficiency can be achieved, illumination conditions that are conceivably more optimal can be readily selected from a variable range in accordance with the age, the gender or the like of a user of the light-emitting device or in accordance with a space, a purpose, or the like of the illumination.
In this case, the following drive control is also possible.
First, when at least one of the index Acg(φSSL2(λ)), correlated color temperature TSSL2 (K), and distance Duv(φSSL2(λ)) from the black-body radiation locus, is changed, the luminous flux and/or the radiant flux emitted from the light-emitting device in the main radiant direction can be unchangeable. If this control is performed, a difference of appearance of colors, caused by a change of the shape of the spectral power distribution, can be easily checked without depending on the luminance of the illumination object, which is preferable.
Second, when the index Acg(φSSL2(λ)) is decreased in an appropriate range, the luminous flux and/or radiant flux of the light-emitting device can be decreased, so as to decrease the luminance of the illumination object.
Third, when Duv(φSSL2(λ)) is decreased in an appropriate range as well, the luminous flux and/or radiant flux of the light-emitting device can be decreased, so as to decrease the luminance of the illumination object. In the second and third cases, brightness is normally increased, hence energy consumption can be suppressed by decreasing luminance, which is preferable.
Fourth, when the correlated color temperature is increased, the luminous flux and/or radiant flux of the light-emitting device can be increased, so as to increase the luminance of the illumination object. Under a general illumination environment, a relatively low luminance environment is often felt to be comfortable when the color temperature is in a low range, and a relatively high luminance environment is often felt to be comfortable when the color temperature is in a high range. This psychological effect is known as the Kruithof Effect, and performing control integrating this effect is also possible, and when the correlated color temperature is increased, it is preferable to increase the luminance of the illumination object by increasing the luminous flux and/or radiant flux of the light-emitting device.
Experimental Example 204
As the same as the case of the Experimental Example 203, as shown in
Next, if the radiant fluxes of the LED light bulbs constituting the light-emitting area 231 and the light-emitting area 232 are appropriately adjusted using dimming controllers connected to the independent power supplies respectively, five types of spectral power distributions shown in
The CIELAB plot in each drawing indicates the a* values and the b* values which are plotted respectively: when 15 Munsell renotation color samples #01 to #15 are mathematically assumed as the illumination objects and these illumination objects are illuminated using this illumination system; and when these illumination objects are illuminated by a reference light derived from the correlated color temperature of the light-emitting device of this illumination system. Here the drive point names A to E are assigned to the radiant flux of the illumination system (light-emitting device) in descending order of contribution of the radiant flux of the LED light bulb constituting the light-emitting area 231.
The spectral power distributions in
At the drive point A, the drive point B, the drive point D, and the drive point E, at least one from Duv(φSSL2(λ)), Acg(φSSL2(λ)), φSSL2-BG-min/φSSL2-BM-max and λSSL2-RM-max are not in an appropriate range of the second invention of the present invention, but at the drive point C and areas between and near the drive point, a natural, vivid, highly visible and comfortable appearance of colors and appearance of objects, as of the objects are seen outdoors, and high light source efficiency can be implemented. Moreover, at the drive point D and the drive point E, in an interval therebetween, and in a vicinity thereof, conceivably, while preferable color appearance is realized, relatively high light source efficiency cannot be realized due to relatively low luminous efficacy of radiation.
Experimental Example 205
A ceramic package LED 240, in which two 5 mm×5 mm ceramic packages, including one light-emitting area respectively, are disposed close to each other, is prepared as shown in
Next, if the current value of the current injected into each light-emitting area of the pair of packaged LEDs 240, which are the light-emitting area 241 and the light-emitting area 242, is appropriately adjusted, five types of spectral power distributions shown in
The CIELAB plot in each drawing indicates the a* values and the b* values which are plotted respectively: when 15 Munsell renotation color samples #01 to #15 are mathematically assumed as the illumination objects, and these illumination objects are illuminated by the pair of packaged LEDs; and when these illumination objects are illuminated by a reference light derived from the correlated color temperature of the pair of packaged LEDs. Here the drive point names A to E are assigned to the radiant flux of the light-emitting device in descending order of contribution of the radiant flux of the light-emitting area 241.
The spectral power distributions in
At the drive point C, the drive point D, and the drive point E, while Acg(φSSL2(λ)) is not in an appropriate range according to the second invention of the present invention, at the drive point A and the drive point B, in an interval therebetween, and in a vicinity thereof, conceivably, light source efficiency is improved compared to other drive points due to relatively high luminous efficacy of radiation and, at the same time, a natural, vivid, highly visible and comfortable appearance of colors and appearance of objects as if the objects are seen outdoors can be achieved. For example, between the drive point A and the drive point B, the correlated color temperature as the packaged LED can be variable in a 3168 K to 3365 K, and Duv(φSSL2(λ)) can also be variable in a −0.0123 to −0.0122 range, while implementing the above mentioned appearance of colors. Further, the average saturation difference of the 15 Munsell renotation color samples can also be variable in a 1.95 to 1.99 range.
Accordingly, in an area where both a preferable appearance of colors and high light source efficiency can be achieved, illumination conditions that are conceivably more optimal can be readily selected from a variable range in accordance with the age, the gender or the like of a user of the light-emitting device or in accordance with a space, a purpose, or the like of the illumination. Moreover, at the drive point C, the drive point D, and the drive point E, in an interval therebetween, and in a vicinity thereof, conceivably, while preferable color appearance is realized, relatively high light source efficiency cannot be realized due to relatively low luminous efficacy of radiation.
In this case, the following drive control is also possible.
First, when at least one of the index Acg(φSSL2(λ)) correlated color temperature TSSL2 (K), and distance Duv(φSSL2(λ)) from the black-body radiation locus, is changed, the luminous flux and/or radiant flux emitted from the light-emitting device in the main radiant direction can be unchangeable. If this control is performed, a difference of appearance of colors, caused by a change of the shape of the spectral power distribution, can be easily checked without depending on the luminance of the illumination object, which is preferable.
Second, when the index Acg(φSSL2(λ)) is decreased in an appropriate range, the luminous flux and/or radiant flux of the light-emitting device can be decreased, so as to decrease the luminance of the illumination object.
Third, when Duv(φSSL2(λ)) is decreased in an appropriate range as well, the luminous flux and/or radiant flux of the light-emitting device can be decreased, so as to decrease the luminance of the illumination object. In the second and third cases, brightness is normally increased, hence energy consumption can be suppressed by decreasing luminance, which is preferable.
Fourth, when the correlated color temperature is increased, the luminous flux and/or radiant flux of the light-emitting device can be increased, so as to increase the luminance of the illumination object. Under a general illumination environment, a relatively low luminance environment is often felt to be comfortable when the color temperature is in a low range, and a relatively high luminance environment is often felt to be comfortable when the color temperature is in a high range. This psychological effect is known as the Kruithof Effect, and performing control integrating this effect is also possible, and when the correlated color temperature is increased, it is preferable to increase the luminance of the illumination object by increasing the luminous flux and/or radiant flux of the light-emitting device.
Experimental Example 206
A 6 mm×9 mm ceramic package 50, which includes a total of sixteen light-emitting units, as shown in
Next, if the current value of current injected into each light-emitting area of the packaged LED having the light-emitting area 251 and the light-emitting are 252 is appropriately adjusted, five types of spectral power distributions shown in
The CIELAB plot in each drawing indicates the a* values and the b* values which are plotted respectively: when 15 Munsell renotation color samples #01 to #15 are mathematically assumed as the illumination objects and these illumination objects are illuminated by the packaged LED; and when these illumination objects are illuminated by a reference light derived from the correlated color template of the packaged LED. Here the drive point names A to E are assigned to the radiant flux of the light-emitting device in descending order of contribution of the radiant flux of the light-emitting area 251.
The spectral power distribution in
At the drive point A, the drive point D, and the drive point E, while at least any one of Duv(φSSL2(λ)), Acg(φSSL2(λ)), φSSL2-BG-min/φSSL2-BM-max, and λSSL2-RM-max is not in an appropriate range according to the second invention of the present invention, at the drive point B and the drive point C, in an interval therebetween, and in a vicinity thereof, conceivably, both a natural, vivid, highly visible and comfortable appearance of colors and appearance of objects as if the objects are seen outdoors and high light source efficiency can be achieved. Therefore, for example, in an interval between the drive point B and the drive point C and in a vicinity thereof, a correlated color temperature of the package LED is variable from 3968 K to 4164 K and Duv(φSSL2(λ)) is also variable from −0.0112 to −0.0116 while realizing preferable appearance of colors. Further, the average saturation difference of the 15 Munsell renotation color samples can also be variable in a 0.89 to 1.11 range. Accordingly, in an area where both a preferable appearance of colors and high light source efficiency can be achieved, illumination conditions that are conceivably more optimal can be readily selected from a variable range in accordance with the age, the gender or the like of a user of the light-emitting device or in accordance with a space, a purpose, or the like of the illumination.
In this case, the following drive control is also possible.
First, when at least one of the index Acg(φSSL2(λ)), correlated color temperature TSSL2 (K), and distance Duv(φSSL2(λ)) from the black-body radiation locus, is changed, the luminous flux and/or the radiant flux emitted from the light-emitting device in the main radiant direction can be unchangeable. If this control is performed, a difference of appearance of colors, caused by a change of the shape of the spectral power distribution, can be easily checked without depending on the luminance of the illumination object, which is preferable.
Second, when the index Acg(φSSL2(λ)) is decreased in an appropriate range, the luminous flux and/or radiant flux of the light-emitting device can be decreased, so as to decrease the luminance of the illumination object.
Third, when Duv(φSSL2(λ)) is decreased in an appropriate range as well, the luminous flux and/or radiant flux of the light-emitting device can be decreased, so as to decrease the luminance of the illumination object. In the second and third cases, brightness is normally increased, hence energy consumption can be suppressed by decreasing luminance, which is preferable.
Fourth, when the correlated color temperature is increased, the luminous flux and/or radiant flux of the light-emitting device can be increased, so as to increase the luminance of the illumination object. Under a general illumination environment, a relatively low luminance environment is often felt to be comfortable when the color temperature is in a low range, and a relatively high luminance environment is often felt to be comfortable when the color temperature is in a high range. This psychological effect is known as the Kruithof Effect, and performing control integrating this effect is also possible, and when the correlated color temperature is increased, it is preferable to increase the luminance of the illumination object by increasing the luminous flux and/or radiant flux of the light-emitting device.
Comparative Experimental Example 201
A resin packaged LED similar to Experimental Example 201 is prepared except for the following difference.
In the light-emitting area 211, a blue semiconductor light-emitting element (dominant wavelength: 438 nm), a green phosphor (β-SiAlON, peak wavelength: 545 nm, full-width at half-maximum: 55 nm) and a red phosphor (CASON, peak wavelength: 645 nm, full-width at half-maximum: 99 nm) are mounted and encapsulated.
In the light-emitting area 212, a blue semiconductor light-emitting element (dominant wavelength: 448 nm), a green phosphor (LSN, peak wavelength: 535 nm, full-width at half-maximum: 107 nm) and a red phosphor (CASN, peak wavelength: 660 nm, full-width at half-maximum: 88 nm) are mounted and encapsulated.
Next, if the current value of current injected into each light-emitting area of the packaged LED having the light-emitting area 211 and the light-emitting are 212 is appropriately adjusted, five types of spectral power distributions shown in
The spectral power distributions in
At all of the drive points from A to E, at least any one of Duv(φSSL2(λ)), Acg(φSSL2(λ)), φSSL2-BG-min/φSSL2-BM-max, and λSSL2-RM-max is not in an appropriate range according to the second invention of the present invention. Therefore, there is no drive point in the variable range as a packaged LED at which both a natural, vivid, highly visible and comfortable appearance of colors and appearance of objects as if the objects are seen outdoors and high light source efficiency can be achieved.
[Examination]
The following invention issues can be derived from the above experimental examples.
In other words, the effect of the second invention of the present invention can be implemented if the light-emitting area allows φSSL2(λ) to satisfy the following conditions by changing the luminous flux amount and/or radiant flux amount emitted from the light-emitting area, where φSSL2N(λ) (N is 1 to M) is a spectral power distribution of a light emitted from each light-emitting area in a main radiant direction of the light-emitting device, and φSSL2(λ) is a spectral power distribution of all the lights emitted from the light-emitting device in the radiant direction and satisfies
The following conditions can be applied in the same manner to the method for designing the light-emitting device according to the second aspect of the second invention of the present invention, and the method for driving the light-emitting device according to the third aspect of the second invention of the present invention.
light emitted from the light-emitting device includes, in the main radiant direction thereof, light whose distance Duv(φSSL2(λ)) from a black-body radiation locus as defined by ANSI C78.377 satisfies
−0.0220≤Duv(φSSL2(λ))≤−0.0070,
φSSL2(λ) denotes a spectral power distribution of light emitted from the light-emitting device in the radiant direction,
φref2(λ) denotes a spectral power distribution of reference light which is selected in accordance with a correlated color temperature TSSL2 (K) of the light emitted from the light-emitting device in the radiant direction,
(XSSL2, YSSL2, ZSSL2) denote tristimulus values of the light emitted from the light-emitting device in the radiant direction, and
(Xref2, Yref2, Zref2) denote tristimulus values of the reference light which is selected in accordance with the correlated color temperature TSSL2 (K) of the light emitted from the light-emitting device in the radiant direction, and
a normalized spectral power distribution SSSL2(λ) of the light emitted from the light-emitting device in the radiant direction,
a normalized spectral power distribution Sref2(λ) of the reference light which is selected in accordance with the correlated color temperature TSSL2 (K) of the light emitted from the light-emitting device in the radiant direction, and
a difference ΔSSSL2(λ) of between normalized spectral power distributions are respectively defined as
S
SSL2(λ)=φSSL2(λ)/YSSL2,
S
ref2(λ)=φref2(λ)/Yref2 and
ΔSSSL2(λ)=Sref2(λ)−SSSL2(λ) and
in a case where λSSL2-RL-max (nm) represents a wavelength that provides a longest wavelength local maximum value of SSSL2(λ) in a wavelength range of 380 nm or more and 780 nm or less, and when a wavelength Λ4 that is represented by SSSL2(λSSL2-RL-max)/2 exists on a longer wavelength-side of λSSL2-RL-max,
an index Acg(φSSL2(λ)) represented by the following formula (2-1) satisfies
−10.0<Acg(φSSL2(λ))≤120.0,
but
in a case where λSSL2-RL-max (nm) represents a wavelength that provides the longest wavelength local maximum value of SSSL2(λ) in a wavelength range of 380 nm or more and 780 nm or less, and when the wavelength Λ4 that is represented by SSSL2 (λSSL2-RL-max)/2 does not exist on the longer wavelength-side of λSSL2-RL-max,
an index Acg(φSSL2(λ)) represented by the following formula (2-2) satisfies
−10.0<Acg(φSSL2(λ))≤120.0;
[Expression 31]
A
cg(ϕSSL2(λ))=∫380495ΔSSSL2(λ)dλ+∫495590(−ΔSSSL2(λ))dλ+∫590Λ4ΔSSSL2(λ)dλ (2- 1)
[Expression 32]
A
cg(ϕSSL2(λ))=∫380495ΔSSSL2(λ)dλ+∫495590(−ΔSSSL2(λ))dλ+∫590780ΔSSSL2(λ)dλ (2-2)
when a maximum value of spectral intensity in a range of 430 nm or more and 495 nm or less is defined as φSSL2-BM-max and a minimum value of spectral intensity in a range of 465 nm or more and 525 nm or less is defined as φSSL2-BG-min, the spectral power distribution φSSL2(λ) of light satisfies
0.2250≤φSSL2-BG-min/φSSL2-BM-max≤0.7000; and
in the spectral power distribution φSSL2(λ) of light, when a maximum value of spectral intensity in a range of 590 nm or more and 780 nm or less is defined as φSSL2-RM-max, a wavelength λSSL2-RM-max that provides φSSL2-RM-max satisfies
605(nm)≤λSSL2-RM-max≤653(nm).
In the experimental examples, the light-emitting device includes two types or three types of light-emitting areas, but a number of types of the light-emitting area is not limited to two or three.
If there are two types of light-emitting areas, control of the light-emitting device is easy, which is preferable.
If there are three types of light-emitting areas, the control area becomes not a line but a plane on the chromaticity coordinates, and the appearance of colors can be adjusted in a wide range, which is preferable.
If there are four types or more of light-emitting areas, not only does the control area become a plane on the chromaticity coordinates, as mentioned above, but also the correlated color temperature, Duv(φSSL2(λ)) and the appearance of colors can be independently controlled, which is preferable. Furthermore, the appearance of colors can be adjusted without changing chromaticity, which is preferable.
If there are too many light-emitting areas, on the other hand, control in the actual light-emitting device becomes complicated, therefore a number of light-emitting areas is preferably ten or less, and even more preferable is eight or less.
In the light-emitting device which includes a plurality of types of light-emitting areas according to the second invention of the present invention, a following method can be used to change the luminous flux amount or radiant flux amount of each type of the light-emitting areas. One method is changing the power to supply each light-emitting area. For this, a method of changing current is preferable because it is easy to do. Another method is changing the luminous flux amount and/or radiant flux amount emitted from the light-emitting areas by allowing an optical ND filter to be disposed in each light-emitting area and exchanging the filter physically, or by electrically changing the transmittance of the polarizing filter or the like.
It is preferable to satisfy the following Condition 5 and/or Condition 6.
In the spectral power distribution φSSL2(λ) of light described above, a wavelength λSSL2-BM-max that provides φSSL2-BM-max satisfies
430(nm)≤λSSL2-RM-max≤480(nm).
0.1800≤φSSL2-BG-min/φSSL2-RM-max≤0.8500. Condition 6
To improve the appearance of colors, it is preferable to satisfy the following Conditions I to IV.
when a*nssL2 and b*nssL2 (where n is a natural number from 1 to 15) respectively denote the a* value and b* value in the CIE 1976 L*a*b* color space of the following 15 Munsell renotation color samples of #01 to #15 based on a mathematical assumption that illumination is performed by the light emitted in the radiant direction, and
when a*nref2 and b*nref2 (where n is a natural number from 1 to 15) respectively denote the a* value and b* value in the CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples based on a mathematical assumption that illumination is performed by reference light which is selected in accordance with the correlated color temperature TSSL2 (K) of the light emitted in the radiant direction, each saturation difference ΔCnSSL2 satisfies
−4.00≤ΔCnSSL2≤8.00(where n is a natural number from1to15),
an average saturation difference SATave(φSSL2(λ)) represented by the formula (2-3) satisfies 0.50≤SATave(φSSL2(λ))≤4.00 and
when a maximum saturation difference value is denoted by ΔCSSL-max2 and a minimum saturation difference value is denoted by ΔCSSL-min2, a difference |ΔCSSL-maX2−ΔCSSL-min2| between the maximum saturation difference value and the minimum saturation difference value satisfies
2.00≤|ΔCSSL-max2−ΔCSSL-min2|≤10.00,
where ΔCnSSL2=√{(a*nSSL2)2+(b*nSSL2)2}−√{(a*nref2)2+(b*nref2)2}
when θnSSL2 (degrees) (where n is a natural number from 1 to 15) denotes a hue angle in the CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples based on a mathematical assumption that illumination is performed by the light emitted in the radiant direction, and
when θnref2 (degrees) (where n is a natural number from 1 to 15) denotes a hue angle in the CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples based on a mathematical assumption that illumination is performed by reference light which is selected in accordance with the correlated color temperature TSSL2 (K) of the light emitted in the radiant direction, an absolute value of each difference in hue angles |ΔhnSSL2| satisfies
0.00 degree≤|ΔhnSSL2|≤12.50 degrees (where n is a natural number from 1 to 15),
where ΔhnSSL2=θnSSL2−θnref2.
It is also preferable that all the φSSL2N(λ) (N is 1 to M) of the light-emitting device satisfies Conditions 1 to 4 as shown in the Experimental Example 201 and the Experimental Example 202. In the case of this mode, both a natural, vivid, highly visible and comfortable appearance of colors and appearance of objects as if the objects are seen outdoors and high light source efficiency can be realized regardless of a ratio at which light emitted from the light-emitting areas are supplied. To determine whether φSSL2N(λ) (N is 1 to M) satisfies Conditions 1 to 4, it is assumed that only this φSSL2N(λ) is emitted from the light-emitting device.
On the other hand, as demonstrated by Experimental example 204 and Experimental example 206, with only light emitted from a single light-emitting area, there may be cases where both a natural, vivid, highly visible and comfortable appearance of colors and appearance of objects as if the objects are seen outdoors and high light source efficiency cannot be realized. Even in such cases, both preferable color appearance and high light source efficiency may be realized by appropriately adjusting a ratio of light emitted from each light-emitting area. Needless to say, this type of light-emitting device still is within the scope of the second invention of the present invention.
One of the features of the second invention of the present invention is that, for example, as demonstrated by Experimental Example 204 and Experimental Example 206, “both preferable color appearance and high light source efficiency can be realized” even when combining “light sources incapable of achieving both preferable color appearance and high light source efficiency”. Another feature is that, as demonstrated by Experimental Example 203 and Experimental Example 205, “both preferable color appearance and high light source efficiency can be realized” even if combining “a light-emitting area incapable of achieving both preferable color appearance and high light source efficiency” and “a light-emitting area capable of achieving both preferable color appearance and high light source efficiency”.
Presented below are guidelines for implementing a light-emitting device according to the second invention of the present invention so as to realize a light-emitting device “capable of achieving both a natural, vivid, highly visible and comfortable appearance of colors and appearance of objects as if the objects are seen outdoors and high light source efficiency” in “cases of combinations including light-emitting areas incapable of achieving both preferable color appearance and high light source efficiency” and, in particular, a case of a combination that is “solely constituted by light-emitting areas incapable of achieving both preferable color appearance and high light source efficiency”.
In order to realize “a light-emitting device achieving both preferable color appearance and high light source efficiency” with “a combination solely constituted by light-emitting areas incapable of achieving both preferable color appearance and high light source efficiency”, all of Duv(φSSL2(λ)) represented in Condition 1, Acg(φSSL2(λ)) represented in Condition 2, φSSL2-BG-min/φSSL2-BM-max represented in Condition 3, and λSSL2-RM-max represented in Condition 4 must be set within appropriate numerical value ranges as a result of the combination. In addition, favorably, λSSL2-BM-max represented in Condition 5 and φSSL2-BG-min/φSSL2-RM-max represented in Condition 6 are also set within appropriate numerical value ranges as a result of the combination. This is conceivably accomplished using methods such as those described below.
First, Duv(φSSL2(λ)) may be adjusted as follows.
When distances Duv(φSSL2(λ)) from a black-body radiation locus of light emitted from the respective light-emitting areas are all outside of proper ranges, for example, (a), (b), and (c) below are effective.
The reason for this follows.
For example, in a case where there are two light-emitting areas, Duv(φSSL2(λ)) of light emitted from one of the light-emitting areas is larger than a proper range (−0.0220 or more and −0.0070 or less), and Duv(φSSL2(λ)) of light emitted from the other light-emitting area has a value that is smaller than the proper range (−0.0220 or more and −0.0070 or less), it is readily understood that a drive point combining light from both light sources at a specific ratio may assume a numerical value that achieves both preferable color appearance and high light source efficiency.
However, even in a case where there are two light-emitting areas and values of Duv(φSSL2(λ)) of light emitted from the light-emitting areas are both larger than the proper range (−0.0220 or more and −0.0070 or less), since a black-body radiation locus is curved on a CIE 1976 u′v′ chromaticity diagram, a drive point combining light from both light sources at a specific ratio may assume a numerical value that achieves both preferable color appearance and high light source efficiency. This is also why, for example, in
Second, Acg(φSSL2(λ)) may be adjusted as follows.
When Acg(φSSL2(λ)) of light emitted from the respective light-emitting areas are all outside of proper ranges, (a), (b), and (c) below are effective in a similar manner to Duv(φSSL2(λ)).
The reason for this follows.
For example, in a case where there are two light-emitting areas, Acg(φSSL2(λ)) of light emitted from one of the light-emitting areas is larger than a proper range (more than −10 and 120 or less), and Acg(φSSL2(λ)) of light emitted from the other light-emitting area has a value that is smaller than the proper range (more than −10 and 120 or less), it is readily understood that a drive point combining light from both light sources at a specific ratio may assume a numerical value that achieves both preferable color appearance and high light source efficiency.
However, even in a case where there are two light-emitting areas and values of Acg(φSSL2(λ)) of light emitted from the light-emitting areas are both larger than the proper range (more than −10 and 120 or less), since a change with respect to color temperature of a spectral power distribution of reference light is nonlinear, a drive point combining light from both light sources at a specific ratio may assume a numerical value that achieves both preferable color appearance and high light source efficiency. This is also why, for example, in
Third, φSSL2-BG-min/φSSL2-BM-max and φSSL2-BG-min/φSSL2-RM-max may be adjusted as follows.
Since these parameters assume values obtained by weighting a characteristic of light emitted from a light-emitting area constituting a light-emitting device by a radiant flux proportion thereof and averaging the weighted values, for example, in a case where there are two light-emitting areas and the parameters of light emitted from one of the light-emitting areas are larger than proper ranges, a drive point combining light from both light sources at a specific ratio may assume a numerical value that achieves both preferable color appearance and high light source efficiency when parameters of light emitted from the other light-emitting area have values that are smaller than the proper ranges. For this reason, a combination of light sources such as that described below is effective.
(a′): a light-emitting device combining light-emitting areas which emit light with different irregularity positions in a spectral power distribution
For example,
Fourth, λSSL2-RM-max and λSSL2-BM-max may be adjusted as follows. While these indexes are provided by a shape of a spectral radiant flux distribution obtained by weighting characteristics of light emitted from light-emitting areas constituting a light-emitting device by a radiant flux proportion thereof and averaging the weighted characteristics, values of the indexes may change continuously or, depending on the shape of the spectral radiant flux distribution, the values may change discontinuously. The former corresponds to cases where distributions of spectral radiant flux emitted from all light-emitting areas are relatively gradual and the latter corresponds to cases where at least one spectral radiant flux distribution has a steep peak. Therefore, favorably, a combination of light-emitting areas is appropriately selected and the respective indexes are set in proper ranges in accordance with a distribution of spectral radiant flux emitted by each light-emitting area constituting the light-emitting device.
Concerning Condition (b), the correlated color temperature difference between two light-emitting areas, of which correlated color temperatures are most different among the plurality of light-emitting areas constituting the light-emitting device, is favorably 2000 K or more, more favorably 2500 K or more, extremely favorably 3000 K or more, dramatically favorably 3500 K or more, and most favorably 4000 K or more. Concerning Condition (c), the absolute value of the Duv difference between two light-emitting areas, of which correlated color temperatures are most different among the plurality of light-emitting areas constituting the light-emitting device, is favorably 0.005 or more, more favorably 0.010 or more, extremely favorably 0.015 or more, and dramatically favorably 0.020 or more.
Presented below are additional guidelines for implementing a light-emitting device according to the second invention of the present invention so as to realize a light-emitting device “capable of achieving both a natural, vivid, highly visible and comfortable appearance of colors and appearance of objects as if the objects are seen outdoors and high light source efficiency” in “cases of combinations including light-emitting areas incapable of achieving both a natural, vivid, highly visible and comfortable appearance of colors and appearance of objects as if the objects are seen outdoors and high light source efficiency” and, in particular, a case of a combination that is “solely constituted by light-emitting areas incapable of achieving both a natural, vivid, highly visible and comfortable appearance of colors and appearance of objects as if the objects are seen outdoors and high light source efficiency”.
In (d), (e) and (f) as well, it is preferable that the respective range disclosed in the second invention of the present invention and the range of each parameter that can be implemented by the combination of the light-emitting area overlap at least partially, and it is more preferable that these ranges overlap on a plane of the chromaticity diagram by using three or more light-emitting areas.
Furthermore, using four or more light-emitting areas enables all of the items (a) (or (a′)) to (f) to be adjusted to ranges disclosed in the second invention of the present invention relatively easily even when the light-emitting areas are “all light-emitting areas incapable of achieving both a natural, vivid, highly visible and comfortable appearance of colors and appearance of objects as if the objects are seen outdoors and high light source efficiency” and is therefore preferable.
In the second invention of the present invention, it is preferable that at least one of the light-emitting areas is a light-emitting area having wiring that can be electrically driven independently from the other light-emitting areas, and it is more preferable that all the light-emitting areas have wiring that can be electrically driven independently from the other light-emitting areas. It is also preferable to drive the light-emitting device in this way. In this mode, power to be supplied to each light-emitting area can be easily controlled, and the appearance of colors suitable to the taste of the user can be implemented.
In the second invention of the present invention, one light-emitting area may be driven so as to be electrically subordinate to another light-emitting area. For example, when current is injected into two light-emitting areas, one light-emitting area may be electrically subordinate to the other, such that when current to be injected into one light-emitting area is increased, current to be injected into the other light-emitting area is decreased. This circuit is easily implemented by a configuration using a variable resistor or the like, for example, and does not require a plurality of power supplies, which is preferable.
In the light-emitting device, it is preferable that at least one selected from the group consisting of: the index Acg(φSSL2(λ)), the correlated color temperature TSSL2 (K), and the distance Duv(φSSL2(λ)) from the black-body radiation locus, can be changed, and it is also preferable that the luminous flux and/or radiant flux emitted from the light-emitting device in the main radiant direction can be independently controlled when at least one selected from the group consisting of: the index Acg(φSSL2(λ)), the correlated color temperature TSSL2 (K) and the distance Duv(φSSL2(λ)) from the black-body radiation locus is changed. It is preferable to drive the light-emitting device in this way. In this mode, parameters to implement appearance of colors are variable, and an appearance of colors suitable to the taste of the user can be easily implemented.
It is preferable that the maximum distance L between two arbitrary points on a virtual outer periphery enveloping the entire light-emitting areas closest to each other is 0.4 mm or more and 200 mm or less. In this mode, the color separation of the lights emitted from a plurality of light-emitting areas is not visually recognized clearly, and the strange feeling of seeing an image generated by the light-emitting device can be reduced. Further, the spatial additive color mixing in the illumination light functions sufficiently, and when this light is irradiated onto the illumination object, color unevenness in the illuminated area can be reduced, which is preferable.
The maximum distance L between two arbitrary points on a virtual outer periphery enveloping the entire light-emitting areas will be described with reference to drawings.
This is the same for the illumination system 230 (details not shown) used for Experimental Example 202 and Experimental Example 203 in
The maximum distance L between two arbitrary points on a virtual outer periphery enveloping the entire light-emitting areas closest to each other is favorably 0.4 mm or more, more favorably 2 mm or more, extremely favorably 5 mm or more, and dramatically favorably 10 mm or more. This is because the higher radiant flux (and/or higher luminous flux) can be emitted as the virtual outer periphery enveloping one light-emitting area is larger. The maximum distance L between two arbitrary points on the virtual outer periphery enveloping the entire light-emitting areas closest to each other is favorably 200 mm or less, more favorably 150 mm or less, extremely favorably 100 mm or less, and dramatically favorably 50 mm or less. This is critical in terms of suppressing the generation of spatial color unevenness in the illuminated area.
On the other hand, in the driving method according to the second invention of the present invention, when φSSL2-BG-min/φSSL2-BM-max of Condition 3 and λSSL2-RL-max of Condition 4 are within proper ranges, a luminous flux and/or a radiant flux emitted from the light-emitting device in a main radiant direction can be made invariable when changing at least one of Acg(φSSL2(λ)) of Condition 2 in a proper range, a correlated color temperature TSSL2 (K), and a distance Duv(φSSL2(λ)) from a black-body radiation locus of Condition 1 in a proper range. If this control is performed, the difference of appearance of colors caused by the change of the shape of the spectral power distribution can be easily checked without depending on the luminance of the illumination object, which is preferable.
In addition, as the method for driving the light-emitting device, when φSSL2-BG-min/φSSL2-BM-max of Condition 3 and λSSL2-RL-max of Condition 4 are within proper ranges, favorable driving methods include a driving method of reducing a luminous flux and/or a radiant flux emitted from the light-emitting device in a main radiant direction when reducing the index Acg(φSSL2(λ)) of Condition 2 in a proper range by an appropriate range, a driving method of increasing a luminous flux and/or a radiant flux emitted from the light-emitting device in a main radiant direction when increasing the correlated color temperature TSSL2 (K), and a driving method of reducing a luminous flux and/or a radiant flux emitted from the light-emitting device in a main radiant direction when reducing Duv(φSSL2(λ)) of Condition 1 in a proper range by an appropriate range. This also means that favorable driving methods include a driving method of increasing a luminous flux and/or a radiant flux emitted from the light-emitting device in a main radiant direction when increasing the index Acg(φSSL2(λ)) of Condition 2 in a proper range, a driving method of reducing a luminous flux and/or a radiant flux emitted from the light-emitting device in a main radiant direction when reducing the correlated color temperature TSSL2(K), and a driving method of increasing a luminous flux and/or a radiant flux emitted from the light-emitting device in a main radiant direction when increasing Duv(φSSL2(λ)) of Condition 1 in a proper range by an appropriate range.
Reducing the index Acg(φSSL2(λ)) of Condition 2 in a proper range by an appropriate range when Duv(φSSL2(λ)) of Condition 1, φSSL2-BG-min/φSSL2-BM-max of Condition 3, and λSSL2-RL-max of Condition 4 are in proper ranges enables a light-emitting device which achieves both a natural, vivid, highly visible and comfortable appearance of colors and appearance of objects as if the objects are seen outdoors and high light source efficiency and which further emphasizes color appearance to be realized. Various visual experiments show that, since a sense of brightness is improved when reducing the index Acg(φSSL2(λ)) in this manner, an illuminated object can maintain a preferable color appearance even when reducing a luminous flux and/or a radiant flux or luminance to be measured, and reducing the index Acg(φSSL2(λ)) in this manner favorably enables energy consumption of the light-emitting device to be further suppressed. In a similar manner, since a light-emitting device which further emphasizes efficiency is realized when the index Acg(φSSL2(λ)) is increased by an appropriate range, an increase in a luminous flux and/or a radiant flux or luminance to be measured can be readily realized.
In addition, in a case of increasing the correlated color temperature TSSL2 (K) when Duv(φSSL2(λ)) of Condition 1, Acg(φSSL2(λ)) of Condition 2, φSSL2-BG-min/φSSL2-BM-max of Condition 3, and λSSL2-RL-max of Condition 4 are in proper ranges, comfortable illumination can be realized due to the Kruithof Effect by performing driving so as to increase a luminous flux and/or a radiant flux. Furthermore, conversely, when lowering the color temperature, control can be performed to reduce luminance of an illuminated object by reducing a luminous flux and/or a radiant flux of the light-emitting device. These controls incorporate the Kruithof Effect and are therefore favorable.
Reducing Duv(φSSL2(λ)) of Condition 1 in a proper range by an appropriate range when the index Acg(φSSL2(λ)) of Condition 2, φSSL2-BG-min/φSSL2-BM-max of Condition 3, and λSSL2-RL-max of Condition 4 are in proper ranges enables a light-emitting device which achieves both a natural, vivid, highly visible and comfortable appearance of colors and appearance of objects as if the objects are seen outdoors and high light source efficiency and which further emphasizes color appearance to be realized. Various visual experiments show that, since a sense of brightness is improved when reducing the distance Duv(φSSL2(λ)) from a black-body radiation locus by an appropriate range, an illuminated object can maintain a preferable color appearance even when reducing a luminous flux and/or a radiant flux or luminance to be measured, and reducing the distance Duv(φSSL2(λ)) in this manner favorably enables energy consumption of the light-emitting device to be suppressed. In a similar manner, since a light-emitting device which further emphasizes efficiency is realized when the index Duv(φSSL2(λ)) is increased by an appropriate range, an increase in a luminous flux and/or a radiant flux or luminance to be measured can be readily realized.
In the second invention of the present invention, it is also possible to perform the opposite of the above mentioned control, and needless to say, that the control method can be appropriately selected depending on the illumination object, the illumination environment, the purpose or the like.
On the other hand, the following invention issues can be derived from the experiment results.
In other words, the effect of the second invention of the present invention can be implemented by using an illumination method comprising:
illuminated objects preparation step of preparing illuminated objects; and
an illumination step of illuminating the objects by light emitted from a light-emitting devices which includes M number of light-emitting areas (M is 2 or greater natural number), and has a blue semiconductor light-emitting element, a green phosphor, and a red phosphor as light-emitting elements in at least one of the light-emitting areas,
in the illumination step, when light emitted from the light-emitting devices illuminate the objects, the objects are illuminated so that the light measured at a position of the objects satisfies Condition 1 and Conditions I to IV below:
a distance Duv(φSSL2(λ)) from a black-body radiation locus as defined by ANSI C78.377 of the light measured at the position of the objects satisfies
−0.0220≤Duv(φSSL2(λ))≤−0.0070;
if an a* value and a b* value in CIE 1976 L*a*b* color space of 15 Munsell renotation color samples from #01 to #15 listed below when mathematically assuming illumination by the light measured at the position of the objects are respectively denoted by a*nssL2 and b*nssL2 (where n is a natural number from 1 to 15), and
if an a* value and a b* value in CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples when mathematically assuming illumination by a reference light that is selected according to a correlated color temperature TSSL2 (K) of the light measured at the position of the objects are respectively denoted by a*nref2 and b*nref2 (where n is a natural number from 1 to 15), then each saturation difference ΔCnSSL2 satisfies
−4.00≤ΔCnSSL2≤8.00(where n is a natural number from1to15);
an average saturation difference SATave(φSSL2(λ)) represented by formula (2-3) above satisfies 0.50≤SATave(φSSL2(λ))≤4.00,
when a maximum saturation difference value is denoted by ΔCSSL-max2 and a minimum saturation difference value is denoted by ΔCSSL-min2, a difference |ΔCSSL-max2-ΔCSSL-min2| between the maximum saturation difference value and the minimum saturation difference value satisfies
2.00≤|ΔCSSL-max2−ΔCSSL-min2|≤10.00,
where ΔCnSSL2=√{(a*nSSL2)2+(b*nSSL2)2}−√{(a*nref2)2+(b*nref2)2}
with the 15 Munsell renotation color samples being:
if hue angles in CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples when mathematically assuming illumination by the light measured at the position of the objects are denoted by θnSSL2 (degrees) (where n is a natural number from 1 to 15), and
if hue angles in CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples when mathematically assuming illumination by a reference light that is selected according to the correlated color temperature TSSL2 (K) of the light measured at the position of the objects are denoted by θnref2 (degrees) (where n is a natural number from 1 to 15), then an absolute value of each difference in hue angles |ΔhnSSL2| satisfies
0.00 degree≤|ΔhnSSL2|≤12.50 degrees (where n is a natural number from 1 to 15),
here ΔhnSSL2=θnSSL2−θnref2.
It is preferable that when φSSL2N(λ) (N is 1 to M) is a spectral power distribution of a light which was emitted from each light-emitting element and reached the position of the object, and φSSL2(λ) is a spectral power distribution of the light measured at the position of the object is represented by
all of φSSL2N(λ) can satisfy the above mentioned Condition 1 and Conditions I to IV.
In the illumination method, it is preferable that at least one light-emitting area of the M number of light-emitting areas is electrically driven independently from the other light-emitting areas for performing the illumination, and it is more preferable that all of the light-emitting areas of the M number of light-emitting areas are electrically driven independently from the other light-emitting areas.
In the illumination method, it is preferable that at least one of: the index SATave(φSSL2(λ)), the correlated color temperature TSSL2 (K), and the distance Duv(φSSL2(λ)) from the black-body radiation locus is changed, or it is preferable that when at least one of the indexes is changed, the luminance in the object is independently controlled, or it is preferable that when at least one of the indexes is changed, the luminance in the object is made to be unchangeable.
Making the luminance unchangeable means that the luminance is not substantially changed, and the change of the luminance is favorably ±20% or less, more favorably ±15% or less, further favorably ±10% or less, particlarly favorably ±% or less, and most favorably ±3% or less. If this method is used, the difference of appearance of colors caused by the change of the shape of the spectral power distribution can be easily checked without depending on the luminance of the illumination object, and optimum spectral power distribution depending on the illumination environment, the object, the purpose or the like can be easily detected, which is preferable.
In the illumination method, it is preferable that when the index SATave(φSSL2(λ)) is increased, the luminance in the object is decreased. If the index is increased, a more vivid appearance can be implemented, and a sense of brightness normally increased in this situation, hence the luminance can be decreased, whereby energy consumption can be conserved. This also means that it is preferable that when the index SATave(φSSL2(λ)) is decreased, the luminance in the object is increased.
In the illumination method, it is preferable that when the correlated color temperature TSSL2 (K) is increased, the luminance in the object is increased. If it is driven such that the luminance is increased when the correlated color temperature TSSL2 (K) is increased, a comfortable illumination can be implemented by the Kruithof Effect. When the color temperature is decreased, on the other hand, it may be controlled to decrease the luminance of the illumination object. These are control techniques applying the Kruithof effect, and are preferable.
In the illumination method, it is preferable that when the distance Duv(φSSL2(λ)) from the black-body radiation locus is decreased, the luminance in the object is decreased. According to various visual experiments, if the distance Duv(φSSL2(λ)) from the black-body radiation locus is decreased, a sense of brightness improves, hence even if the luminance is decreased, a good appearance of colors can still be maintained in the illumination object, and therefore energy consumption of the light-emitting device can be conserved, which is preferable. In the same manner, when the distance Duv(φSSL2(λ)) from the black-body radiation locus is increased, it is preferable to maintain a good appearance of colors in the illumination object by increasing the luminance.
In the illumination method, it is preferable that when L is a maximum distance between two arbitrary points on a virtual outer periphery enveloping the entire light-emitting areas closest to each other, and H is a distance between the light-emitting device and the illumination object, the distance H is set so as to satisfy 5×L≤H≤500×L.
In this case, the base point of the light-emitting device to measure the distance is the irradiation port.
If this illumination method is used, color separation of lights from the light sources is not visually recognized clearly when the light-emitting device is observed from the position of the illumination object, and spatial color unevenness is hardly generated in the illumination object, which is preferable.
In the maximum distance L between two arbitrary points on a virtual outer periphery enveloping the entire light-emitting areas closest to each other, and the distance H between the light-emitting device and the illumination object, H is favorably 5×L or more, more favorably 10×L or more, extremely favorably 15×L or more, and dramatically favorably 20×L or more. Because as H is greater within an appropriate range, that is, as H is more distant from the maximum distance L between two arbitrary points on a virtual outer periphery enveloping different light-emitting areas, the colors of the lights emitted from different light-emitting areas are more thoroughly mixed spatially, which is preferable. On the other hand, H is favorably 500×L or less, more favorably 250×L or less, extremely favorably 100×L or less, and dramatically favorably 50×L or less. Because if H is more distant than necessary, sufficient luminance cannot be assured for the illumination object, and maintaining the distance of H and L within this range is important to implement a good luminance environment with driving power in an appropriate range.
The description of a light-emitting device according to the first aspect of the first invention of the present invention applies to favorable embodiments for implementing a light-emitting device according to the first aspect of the second invention of the present invention. In addition, modes for implementing a light-emitting device according to the first aspect of the second invention of the present invention are not limited to these embodiments.
<3. Third Invention>
The third invention of the present invention includes an aspect related to the light-emitting device (a first aspect of the third invention) as well as an aspect related to a method for designing the light-emitting device (a second aspect of the third invention), an aspect related to an illumination method (a fourth aspect of the third invention), and an aspect related to a method for manufacturing the light-emitting device (a fifth aspect of the third invention). It should be noted that a third aspect of the third invention of the present invention will not be described for the sake of convenience.
In order to solve the problems described in the section titled “Technical Problem” presented earlier, the present inventor has arrived with a light-emitting device having improved light source efficiency and a design guideline for the light-emitting device in Japanese Patent Application No. 2014-159784.
The light sources that satisfy the requirements which Japanese Patent Application No. 2014-159784 defined and which the present inventor have already discovered can implement a natural, vivid, highly visible, and comfortable appearance of colors and an appearance of objects under an indoor luminance environment as if the objects were seen under an outdoor environment.
However, LED illumination is already common, but many products which do not consider the appearance of colors are on the market. Many LED lighting fixtures/lighting systems are already in practical use. However even if a user experiences an unnatural feeling and is unsatisfied with the appearance of colors, it is impractical to replace the target lighting fixtures/systems or the like to improve the appearance of colors thereof, if time constraints and economic issues of the user are considered.
The third invention of the present invention has been made in order to solve such problems and to improve the appearance of colors of a light-emitting device which currently exists or is in use, and which includes a semiconductor light-emitting device of which appearance of colors is inferior. Further, the third invention of the present invention discloses a method for designing and a method for manufacturing this light-emitting device, and also discloses an illumination method using this light-emitting device.
Moreover, the third invention of the present invention also discloses a method or the like for further adjusting the appearance of colors of a semiconductor light-emitting device having good appearance of colors and having improved light source efficiency in accordance with the taste of the user using similar techniques.
To achieve the above objects, the first aspect of the third invention of the present invention relates to the following matters.
[1]
A light-emitting device having a light-emitting element and a control element, the light-emitting device at least including as the light-emitting element
a blue semiconductor light-emitting element,
a green phosphor, and
a red phosphor,
wherein when λ(nm) denotes wavelength,
Φelm3(λ) denotes a spectral power distribution of light emitted from the light-emitting element in a main radiant direction, and φSSL3(λ) denotes a spectral power distribution of light emitted from the light-emitting device in the main radiant direction,
light having Φelm3(λ) does not satisfy at least one of Conditions 1 to 4 described below but light having φSSL3(λ) satisfies all of the Conditions 1 to 4 described below.
When φ(λ) denotes a spectral power distribution of object light, φref(λ) denotes a spectral power distribution of reference light which is selected in accordance with a correlated color temperature T of the object light,
(X, Y, Z) denote tristimulus values of the object light,
(Xref, Yref, Zref) denote tristimulus values of reference light which is selected in accordance with the correlated color temperature T,
a normalized spectral power distribution S(λ) of the object light, a normalized spectral power distribution Sref(λ) of reference light of the object light, and a difference ΔS(λ) of between normalized spectral power distributions are respectively defined as
S(λ)=φ(λ)/Y,
S
ref(λ)=φref(λ)/Yref,
ΔS(λ)=Sref(λ)−S(λ), and
in a case where λRL-max (nm) represents a wavelength that provides a longest wavelength local maximum value of S(λ) in a wavelength range of 380 nm or more and 780 nm or less, and when a wavelength Λ4 that is represented by S(λRL-max)/2 exists on a longer wavelength-side of λRL-max,
an index Acg represented by the following formula (3-1) satisfies
−10.0<Acg≤120.0,
but in a case where λRL-max (nm) represents a wavelength that provides the longest wavelength local maximum value of S(λ) in a wavelength range of 380 nm or more and 780 nm or less, and when the wavelength Λ4 that is represented by S(λRL-max)/2 does not exist on the longer wavelength-side of λRL-max,
an index Acg represented by the following formula (3-2) satisfies
−10.0<Acg≤120.0,
[Expression 35]
A
cg=∫380495ΔS(λ)dλ+∫495590(−ΔS(λ))dλ+∫590Λ4ΔS(λ)dλ (3-1)
[Expression 36]
A
cg=∫380495ΔS(λ)dλ+∫495590(−ΔS(λ))dλ+∫590780ΔS(λ)dλ (3-2)
a distance Duv of the spectral power distribution φ(λ) of object light from a black-body radiation locus defined by ANSI C78.377 satisfies
−0.0220≤Duv≤−0.0070;
when a maximum value of spectral intensity in a range of 430 nm or more and 495 nm or less is defined as φBM-max and a minimum value of spectral intensity in a range of 465 nm or more and 525 nm or less is defined as φBG-min, the spectral power distribution φ(λ) of object light satisfies
0.2250≤φBG-min/φBM-max≤0.7000; and
in the spectral power distribution φ(λ) of object light, when a maximum value of spectral intensity in a range of 590 nm or more and 780 nm or less is defined as φRM-max, a wavelength λRM-max that provides φRM-max satisfies
605(nm)≤λRM-max≤653(nm).
[2]
The light-emitting device according to [1], wherein light having Φelm3(λ) does not satisfy at least one of Conditions I to IV described below but light having φSSL3(λ) satisfies all of the Conditions I to IV described below.
when a*n and b*n (where n is a natural number from 1 to 15) respectively denote the a* value and b* value in the CIE 1976 L*a*b* color space of the following 15 Munsell renotation color samples of #01 to #15 based on a mathematical assumption that illumination is performed by the object light, and when a*nref and b*nref (where n is a natural number from 1 to 15) respectively denote the a* value and b* value in the CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples based on a mathematical assumption that illumination is performed by reference light which is selected in accordance with the correlated color temperature T (K) of the object light, each saturation difference ΔCn satisfies
−4.00≤ΔCn≤8.00(where n is a natural number from1to15);
an average saturation difference of the object light represented by the following formula (3-3) satisfies
when a maximum saturation difference value of the object light is denoted by ΔCmax and a minimum saturation difference value of the object light is denoted by ΔCmin, a difference |ΔCmax−ΔCmin| between the maximum saturation difference value and the minimum saturation difference value satisfies
2.00≤|ΔCmax−ΔCmin|≤10.00,
where ΔCn=√{(a*n)2+(b*n)2}−√{(a*nref)2+(b*nref)2},
with the 15 Munsell renotation color samples being:
when θn (degrees) (where n is a natural number from 1 to 15) denotes a hue angle in the CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples based on a mathematical assumption that illumination is performed by the object light, and
when θnref (degrees) (where n is a natural number from 1 to 15) denotes a hue angle in the CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples based on a mathematical assumption that illumination is performed by reference light which is selected in accordance with the correlated color temperature T of the object light, an absolute value of each difference in hue angles |Δhn| satisfies
0.00 degree≤|Δhn|≤12.50 degrees(where n is a natural number from1to15),
where Δhn=θn−θnref.
[3]
A light-emitting device having a light-emitting element and a control element, the light-emitting device at least including as the light-emitting element
a blue semiconductor light-emitting element,
a green phosphor, and
a red phosphor,
wherein when λ(nm) denotes wavelength,
Φelm3(λ) denotes a spectral power distribution of light emitted from the light-emitting element in a main radiant direction, and φSSL3(λ) denotes a spectral power distribution of light emitted from the light-emitting device in the main radiant direction,
light having Φelm3(λ) satisfies all of the Conditions 1 to 4 described below and light having φSSL3(λ) also satisfies all of the Conditions 1 to 4 described below.
When φ(λ) denotes a spectral power distribution of object light, φref(λ) denotes a spectral power distribution of reference light which is selected in accordance with a correlated color temperature T of the object light,
(X, Y, Z) denote tristimulus values of the object light,
(Xref, Yref, Zref) denote tristimulus values of reference light which is selected in accordance with the correlated color temperature T,
a normalized spectral power distribution S(λ) of the object light, a normalized spectral power distribution Sref(λ) of reference light of the object light, and a difference ΔS(λ) of between normalized spectral power distributions are respectively defined as
S(λ)=φ(λ)/Y,
S
ref(λ)=φref(λ)/Yref,
ΔS(λ)=Sref(λ)−S(λ), and
in a case where λRL-max (nm) represents a wavelength that provides a longest wavelength local maximum value of S(λ) in a wavelength range of 380 nm or more and 780 nm or less, and when a wavelength Λ4 that is represented by S (λRL-max)/2 exists on a longer wavelength-side of λRL-max,
an index Acg represented by the following formula (3-1) satisfies
−10.0<Acg≤120.0,
but in a case where λRL-max (nm) represents a wavelength that provides the longest wavelength local maximum value of S(λ) in a wavelength range of 380 nm or more and 780 nm or less, and when the wavelength Λ4 that is represented by S(λRL-max)/2 does not exist on the longer wavelength-side of λRL-max,
an index Acg represented by the following formula (3-2) satisfies
−10.0<Acg≤120.0,
[Expression 39]
A
cg=∫380495ΔS(λ)dλ+∫495590(−ΔS(λ))dλ+∫590Λ4ΔS(λ)dλ (3-1)
[Expression 40]
A
cg=∫380495ΔS(λ)dλ+∫495590(−ΔS(λ))dλ+∫590780ΔS(λ)dλ (3-2)
a distance Duv of the spectral power distribution φ(λ) of object light from a black-body radiation locus defined by ANSI C78.377 satisfies
−0.0220≤Duv≤−0.0070;
when a maximum value of spectral intensity in a range of 430 nm or more and 495 nm or less is defined as φBM-max and a minimum value of spectral intensity in a range of 465 nm or more and 525 nm or less is defined as φBG-min, the spectral power distribution φ(λ) of object light satisfies
0.2250≤φBG-min/φBM-max≤0.7000; and
in the spectral power distribution φ(λ) of object light, when a maximum value of spectral intensity in a range of 590 nm or more and 780 nm or less is defined as φRM-max, a wavelength λRM-max that provides φRM-max satisfies
605(nm)≤λRM-max≤653(nm).
[4]
The light-emitting device according to [3], wherein light having Φelm3(λ) satisfies all of Conditions I to IV described below and light having φSSL3(λ) also satisfies all of the Conditions I to IV described below.
when a*n and b*n (where n is a natural number from 1 to 15) respectively denote the a* value and b* value in the CIE 1976 L*a*b* color space of the following 15 Munsell renotation color samples of #01 to #15 based on a mathematical assumption that illumination is performed by the object light, and when a*nref and b*nref (where n is a natural number from 1 to 15) respectively denote the a* value and b* value in the CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples based on a mathematical assumption that illumination is performed by reference light which is selected in accordance with the correlated color temperature T (K) of the object light, each saturation difference ΔCn satisfies
−4.00≤ΔCn≤8.00(where n is a natural number from1to15);
an average saturation difference of the object light represented by the following formula (3-3) satisfies
when a maximum saturation difference value of the object light is denoted by ΔCmax and a minimum saturation difference value of the object light is denoted by ΔCmin, a difference |ΔCmax−ΔCmin| between the maximum saturation difference value and the minimum saturation difference value satisfies
2.00≤|ΔCmax−ΔCmin|≤10.00,
where ΔCn=√{(a*n)2+(b*n)2}−√{(a*nref)2+(b*nref)2},
with the 15 Munsell renotation color samples being:
and
when θn (degrees) (where n is a natural number from 1 to 15) denotes a hue angle in the CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples based on a mathematical assumption that illumination is performed by the object light, and
when θnref (degrees) (where n is a natural number from 1 to 15) denotes a hue angle in the CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples based on a mathematical assumption that illumination is performed by reference light which is selected in accordance with the correlated color temperature T of the object light, an absolute value of each difference in hue angles |Δhn| satisfies
0.00 degree≤|Δhn|≤12.50 degrees(where n is a natural number from1to15),
where Δhn=θn−θnref.
[5]
The light-emitting device according to [1] or [3], wherein
if Duv derived from the spectral power distribution of the light emitted from the light-emitting element in the main radiant direction is denoted by Duv(Φelm3(λ)), and Duv derived from the spectral power distribution of the light emitted from the light-emitting device in the main radiant direction is denoted by Duv(φSSL3(λ))
Duv(φSSL3(λ))<Duv(Φelm3(λ)) is satisfied.
[6]
The light-emitting device according to [1] or [3], wherein
if Acg derived from the spectral power distribution of the light emitted from the light-emitting element in the main radiant direction is denoted by Acg (Φelm3(λ)), and Acg derived from the spectral power distribution of the light emitted from the light-emitting device in the main radiant direction is denoted by Acg(φSSL3(λ))
Acg(φSSL3(λ))<Acg(Φelm3(λ)) is satisfied.
[7]
The light-emitting device according to [2] or [4], wherein
if an average saturation difference derived from the spectral power distribution of the light emitted from the light-emitting element in the main radiant direction is denoted by SATave(Φelm3(λ)), and
if an average saturation difference derived from the spectral power distribution of the light emitted from the light-emitting device in the main radiant direction is denoted by SATave(φSSL3(λ)),
SATave(Φelm3(λ))<SATave(φSSL3(λ)) is satisfied.
[8]
The light-emitting device according to any one of [1] to [7], wherein
the control element is an optical filter that absorbs or reflects light in a range of 380 nm≤λ(nm)≤780 nm.
[9]
The light-emitting device according to any one of [1] to [8], wherein
the control element has a collection function and/or a diffusion function of the light emitted from the light-emitting element.
[10]
The light-emitting device according to [9], wherein
the collection function and/or the diffusion function of the control element is implemented by at least one of the functions of a concave lens, a convex lens and a Fresnel lens.
[11]
The light-emitting device according to any one of [1] to [10], wherein
illuminance at which the light emitted from the light-emitting device in the radiant direction illuminates objects is 51 lx or more and 10000 lx or less.
[12]
The light-emitting device according to any one of [1] to [11], wherein
in Condition 2, the light-emitting device satisfies
−0.0184≤Duv≤−0.0084.
[13]
The light-emitting device according to [1] or [12], wherein
in Condition 4,
625 (nm)≤λRM-max≤647 (nm) is satisfied.
[14]
The light-emitting device according to any one of [1] to [13], wherein
light having Φelm3(λ) does not satisfy Condition 5 described below but light having φSSL3(λ) satisfies Condition 5 described below.
In the spectral power distribution φ(λ) of object light, a wavelength λBM-max that provides φBM-max satisfies
430(nm)≤λRM-max≤480(nm).
[15]
The light-emitting device according to any one of [1] to [13], wherein
light having Φelm3(λ) does not satisfy Condition 6 described below but light having φSSL3(λ) satisfies Condition 6 described below.
The spectral power distribution φ(λ) of object light satisfies
0.1800≤φBG-min/φRM-max≤0.8500.
[16]
The light-emitting device according to [15], wherein
in Condition 6,
0.1917≤φBG-min/(φRM-max≤0.7300 is satisfied.
[17]
The light-emitting device according to any one of [1] to [13], wherein
light having Φelm3(λ) does not satisfy Condition 7 described below but light having φSSL3(λ) satisfies Conditions 7 described below.
A luminous efficacy of radiation K (lm/W) in a wavelength range of 380 nm to 780 nm derived from a spectral power distribution φ(λ) of object light satisfies
210.0lm/W≤K≤290.0lm/W.
[18]
The light-emitting device according to any one of [1] to [13], wherein
light having Φelm3(λ) does not satisfy Condition 8 described below but light having φSSL3(λ) satisfies Conditions 8 described below.
A correlated color temperature T (K) of object light satisfies
2600K≤T≤7700K.
[19]
The light-emitting device according to [14], wherein light having Φelm3(λ) satisfies at least one of Conditions 6 to 8 described below but if there are conditions not satisfied by light having Φelm3(λ) among the Conditions 6 to 8 described below, light having φSSL3(λ) satisfies at least one of such conditions.
The spectral power distribution φ(λ) of object light satisfies
0.1800≤φBG-min/φRM-max≤0.8500.
A luminous efficacy of radiation K(lm/W) in a wavelength range of 380 nm to 780 nm derived from a spectral power distribution φ(λ) of object light satisfies
210.0lm/W≤K≤290.0lm/W.
A correlated color temperature T (K) of object light satisfies
2600K≤T≤7700K.
[20]
The light-emitting device according to [15] or [16], wherein
light having Φelm3(λ) satisfies at least one of Conditions 5, 7 and 8 described below but if there are conditions not satisfied by light having Φelm3(λ) among the Conditions 5, 7 and 8 described below, light having φSSL3(λ) satisfies at least one of such conditions.
In the spectral power distribution φ(λ) of object light, a wavelength λBM-max that provides φBM-max satisfies
430(nm)≤λBM-max≤480(nm).
A luminous efficacy of radiation K (lm/W) in a wavelength range of 380 nm to 780 nm derived from a spectral power distribution φ(λ) of object light satisfies
210.0lm/W≤K≤290.0lm/W.
A correlated color temperature T (K) of object light satisfies
2600K≤T≤7700K.
[21]
The light-emitting device according to [17], wherein
light having Φelm3(λ) satisfies at least one of Conditions 5, 6 and 8 described below but if there are conditions not satisfied by light having Φelm3(λ) among the Conditions 5, 6 and 8 described below, light having φSSL3(λ) satisfies at least one of such conditions.
In the spectral power distribution φ(λ) of object light, a wavelength λBM-max that provides φBM-max satisfies
430(nm)≤λBM-max≤480(nm).
The spectral power distribution φ(λ) of object light satisfies
0.1800≤φBG-min/φRM-max≤0.8500.
A correlated color temperature T (K) of object light satisfies
2600K≤T≤7700K.
[22]
The light-emitting device according to [18], wherein
light having Φelm3(λ) satisfies at least one of Conditions 5 to 7 described below but if there are conditions not satisfied by light having Φelm3(λ) among the Conditions 5 to 7 described below, light having φSSL3(λ) satisfies at least one of such conditions.
In the spectral power distribution φ(λ) of object light, a wavelength λBM-max that provides φBM-max satisfies
430(nm)≤λBM-max≤480(nm).
The spectral power distribution φ(λ) of object light satisfies
0.1800≤φBG-min/φRM-max≤0.8500.
A luminous efficacy of radiation K (lm/W) in a wavelength range of 380 nm to 780 nm derived from a spectral power distribution φ(λ) of object light satisfies
210.0lm/W≤K≤290.0lm/W.
[23]
The light-emitting device according to any one of [1] to [13], wherein
light having Φelm3(λ) satisfies all of the Conditions 5 to 8 described below and light having φSSL3(λ) also satisfies all of the Conditions 5 to 8 described below.
In the spectral power distribution φ(λ) of object light, a wavelength λBM-max that provides φBM-max satisfies
430(nm)≤λBM-max≤480(nm).
The spectral power distribution φ(λ) of object light satisfies
0.1800≤φBG-min/φRM-max≤0.8500.
A luminous efficacy of radiation K (lm/W) in a wavelength range of 380 nm to 780 nm derived from a spectral power distribution φ(λ) of object light satisfies
210.0lm/W≤K≤290.0lm/W.
A correlated color temperature T (K) of object light satisfies
2600K≤T≤7700K.
[24]
The light-emitting device according to any one of [1] to [23], wherein
light having φSSL3(λ) does not have effective intensity derived from the light-emitting element in a range of 380 nm or more and 405 nm or less.
[25]
The light-emitting device according to any one of [1] to [24], wherein
the blue semiconductor light-emitting element is configured such that a dominant wavelength λCHIP-BM-dom of the blue semiconductor light-emitting element alone when pulse-driven is 445 nm or more and 475 nm or less.
[26]
The light-emitting device according to any one of [1] to [25], wherein
the green phosphor is a wide-band green phosphor.
[27]
The light-emitting device according to any one of [1] to [26], wherein
the green phosphor is configured such that a wavelength λPHOS-GM-max that provides maximum emission intensity when light is excited by the green phosphor alone is 511 nm or more and 543 nm or less, and
a full-width at half-maximum WPHOS-GM-fwhm thereof is 90 nm or more and 110 nm or less.
[28]
The light-emitting device according to any one of [1] to [27], wherein
wherein the light-emitting device includes substantially no yellow phosphor.
[29]
The light-emitting device according to any one of [1] to [28], wherein
the red phosphor is configured such that a wavelength λPHOS-RM-max that provides maximum emission intensity when light is excited by the red phosphor alone is 622 nm or more and 663 nm or less, and
a full-width at half-maximum WPHOS-RM-fwhm thereof is 80 nm or more and 105 nm or less.
[30]
The light-emitting device according to any one of [1] to [29], wherein
the blue semiconductor light-emitting element is an AlInGaN light-emitting element.
[31]
The light-emitting device according to any one of [1] to [30], wherein
the green phosphor is Ca3 (Sc,Mg)2Si3O12:Ce (CSMS phosphor), CaSc2O4:Ce (CSO phosphor), Lu3Al5O12:Ce (LuAG phosphor), or Y3 (Al, Ga)5O12:Ce (G-YAG phosphor).
[32]
The light-emitting device according to any one of [1] to [31], wherein
the red phosphor includes (Sr,Ca)AlSiN3:Eu (SCASN phosphor), CaAlSi(ON)3:Eu (CASON phosphor), or CaAlSiN3:Eu (CASN phosphor).
[33]
The light-emitting device according to any one of [1] to [32], wherein
the blue semiconductor light-emitting element is an AlInGaN light-emitting element with a dominant wavelength λCHIP-BM-dom when the blue semiconductor light-emitting element alone is pulse-driven, of 452.5 nm or more and 470 nm or less,
the green phosphor is a CaSc2O4:Ce (CSO phosphor) or a Lu3Al5O12:Ce (LuAG phosphor) with a wavelength λPHOS-GM-max that provides maximum emission intensity when light is excited by the green phosphor alone is 515 nm or more and 535 nm or less and a full-width at half-maximum WPHOS-GM-fwhm thereof is 90 nm or more and 110 nm or less, and
the red phosphor is a CaAlSi(ON)3:Eu (CASON phosphor) or a CaAlSiN3:Eu (CASN phosphor) with a wavelength that provides maximum emission intensity λPHOS-RM-max when light is excited by the red phosphor alone is 640 nm or more and 663 nm or less and a full-width at half-maximum WPHOS-RM-fwhm thereof is 80 nm or more and 105 nm or less.
[34]
The light-emitting device according to any one of [1] to [33], wherein the light-emitting device is a packaged LED, a chip-on-board LED, an LED module, an LED light bulb, an LED lighting fixture, or an LED lighting system.
[35]
The light-emitting device according to any one of [1] to [34], which is used as a residential uses' illumination device.
[36]
The light-emitting device according to any one of [1] to [34], which is used as an exhibition illumination device.
[37]
The light-emitting device according to any one of [1] to [34], which is used as a presentation illumination device.
[38]
The light-emitting device according to any one of [1] to [34], which is used as a medical illumination device.
[39]
The light-emitting device according to any one of [1] to [34], which is used as a work illumination device.
[40]
The light-emitting device according to any one of [1] to [34], which is used as an illumination device incorporated in industrial equipments.
[41]
The light-emitting device according to any one of [1] to [34], which is used as an illumination device for interior of transportation.
[42]
The light-emitting device according to any one of [1] to [34], which is used as an illumination device for works of art.
[43]
The light-emitting device according to any one of [1] to [34], which is used as an illumination device for aged persons.
To achieve the above objects, the fifth aspect of the third invention of the present invention relates to the following matters.
[44]
A method for manufacturing a light-emitting device having a light-emitting element and a control element, the manufacturing method comprising the steps of:
preparing a first light-emitting device which at least includes a blue semiconductor light-emitting element, a green phosphor, and a red phosphor as the light-emitting element; and
manufacturing a second light-emitting device by arranging the control element so as to act on at least a part of light emitted from the first light-emitting device in a main radiant direction, and
when λ(nm) denotes wavelength,
Φelm3(λ) denotes a spectral power distribution of light emitted from the first light-emitting device in the main radiant direction, and φSSL3(λ) denotes a spectral power distribution of light emitted from the second light-emitting device in the main radiant direction,
light having Φelm3(λ) does not satisfy at least one of Conditions 1 to 4 described below but light having φSSL3(λ) satisfies all of the Conditions 1 to 4 described below.
When φ(λ) denotes a spectral power distribution of object light, φref(λ) denotes a spectral power distribution of reference light which is selected in accordance with a correlated color temperature T of the object light,
(X, Y, Z) denote tristimulus values of the object light,
(Xref, Yref, Zref) denote tristimulus values of reference light which is selected in accordance with the correlated color temperature T,
a normalized spectral power distribution S(λ) of the object light, a normalized spectral power distribution Sref(λ) of reference light of the object light, and a difference ΔS(λ) of between normalized spectral power distributions are respectively defined as
S(λ)=φ(λ)/Y,
S
ref(λ)=φref(λ)/Yref,
ΔS(λ)=Sref(λ)−S(λ), and
in a case where λRL-max (nm) represents a wavelength that provides a longest wavelength local maximum value of S(λ) in a wavelength range of 380 nm or more and 780 nm or less, and when a wavelength Λ4 that is represented by S(λRL-max)/2 exists on a longer wavelength-side of λRL-max,
an index Acg represented by the following formula (3-1) satisfies
10.0<Acg≤120.0,
but in a case where λRL-max (nm) represents a wavelength that provides the longest wavelength local maximum value of S(λ) in a wavelength range of 380 nm or more and 780 nm or less, and when the wavelength Λ4 that is represented by S(λRL-max)/2 does not exist on the longer wavelength-side of λRL-max,
an index Acg represented by the following formula (3-2) satisfies
10.0<Acg≤120.0,
[Expression 43]
A
cg=∫380495ΔS(λ)dλ+∫495590(−ΔS(λ))dλ+∫590Λ4ΔS(λ)dλ (3-1)
[Expression 44]
A
cg=∫380495ΔS(λ)dλ+∫495590(−ΔS(λ))dλ+∫590780ΔS(λ)dλ (3-2)
a distance Duv of the spectral power distribution φ(λ) of object light from a black-body radiation locus defined by ANSI C78.377 satisfies
−0.0220≤Duv≤−0.0070;
when a maximum value of spectral intensity in a range of 430 nm or more and 495 nm or less is defined as φBM-max and a minimum value of spectral intensity in a range of 465 nm or more and 525 nm or less is defined as φBG-min, the spectral power distribution φ(λ) of object light satisfies
0.2250≤φBG-min/φBM-max≤0.7000; and
in the spectral power distribution φ(λ) of object light, when a maximum value of spectral intensity in a range of 590 nm or more and 780 nm or less is defined as φRM-max, a wavelength λRM-max that provides φRM-max satisfies
605(nm)≤λRM-max≤653(nm).
[45]
The method for manufacturing a light-emitting device according to [44], wherein light having Φelm3(λ) does not satisfy at least one of Conditions I to IV described below but light having φSSL3(λ) satisfies all of the Conditions I to IV described below.
when a*n and b*n (where n is a natural number from 1 to 15) respectively denote the a* value and b* value in the CIE 1976 L*a*b* color space of the following 15 Munsell renotation color samples of #01 to #15 based on a mathematical assumption that illumination is performed by the object light, and
when a*nref and b*nref (where n is a natural number from 1 to 15) respectively denote the a* value and b* value in the CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples based on a mathematical assumption that illumination is performed by reference light which is selected in accordance with the correlated color temperature T (K) of the object light, each saturation difference ΔCn satisfies
−4.00≤ΔCn≤8.00(where n is a natural number from1to15);
an average saturation difference of the object light represented by the following formula (3-3) satisfies
when a maximum saturation difference value of the object light is denoted by ΔCmax and a minimum saturation difference value of the object light is denoted by ΔCmin, a difference |ΔCmax−ΔCmin| between the maximum saturation difference value and the minimum saturation difference value satisfies
2.00≤|ΔCmax−ΔCmin|≤10.00,
where ΔCn=√{(a*n)2+(b*n)2}−√{(a*nref)2+(b*nref)2},
with the 15 Munsell renotation color samples being:
when θn (degrees) (where n is a natural number from 1 to 15) denotes a hue angle in the CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples based on a mathematical assumption that illumination is performed by the object light, and
when θnref (degrees) (where n is a natural number from 1 to 15) denotes a hue angle in the CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples based on a mathematical assumption that illumination is performed by reference light which is selected in accordance with the correlated color temperature T of the object light, an absolute value of each difference in hue angles |Δhn| satisfies
0.00 degree≤|Δhn|≤12.50 degrees(where n is a natural number from1to15),
where Δhn=θn−θnref.
[46]
A method for manufacturing a light-emitting device having a light-emitting element and a control element, the manufacturing method comprising the steps of:
preparing a first light-emitting device which at least includes a blue semiconductor light-emitting element, a green phosphor, and a red phosphor as the light-emitting element; and
manufacturing a second light-emitting device by arranging the control element so as to act on at least a part of light emitted from the first light-emitting device in a main radiant direction, and
when λ(nm) denotes wavelength,
Φelm3(λ) denotes a spectral power distribution of light emitted from the first light-emitting device in the main radiant direction, and φSSL3(λ) denotes a spectral power distribution of light emitted from the second light-emitting device in the main radiant direction,
light having Φelm3(λ) satisfies all of Conditions 1 to 4 described below and light having φSSL3(λ) also satisfies all of the Conditions 1 to 4 described below.
when φ(λ) denotes a spectral power distribution of object light, φref(λ) denotes a spectral power distribution of reference light which is selected in accordance with a correlated color temperature T of the object light,
(X, Y, Z) denote tristimulus values of the object light,
(Xref, Yref, Zref) denote tristimulus values of reference light which is selected in accordance with the correlated color temperature T,
a normalized spectral power distribution S(λ) of the object light, a normalized spectral power distribution Sref(λ) of reference light of the object light, and a difference ΔS(λ) of between normalized spectral power distributions are respectively defined as
S(λ)=φ(λ)/Y,
S
ref(λ)=φref(λ)/Yref,
ΔS(λ)=Sref(λ)−S(λ), and
in a case where λRL-max (nm) represents a wavelength that provides a longest wavelength local maximum value of S(λ) in a wavelength range of 380 nm or more and 780 nm or less, and when a wavelength Λ4 that is represented by S(λRL-max)/2 exists on a longer wavelength-side of λRL-max,
an index Acg represented by the following formula (3-1) satisfies
−10.0<Acg≤120.0,
but in a case where λRL-max (nm) represents a wavelength that provides the longest wavelength local maximum value of S(λ) in a wavelength range of 380 nm or more and 780 nm or less, and when the wavelength Λ4 that is represented by S(λRL-max)/2 does not exist on the longer wavelength-side of λRL-max,
an index Acg represented by the following formula (3-2) satisfies
−10.0<Acg≤120.0.
[Expression 47]
A
cg=∫380495ΔS(λ)dλ+∫495590(−ΔS(λ))dλ+∫590Λ4ΔS(λ)dλ (3-1)
[Expression 48]
A
cg=∫380495ΔS(λ)dλ+∫495590(−ΔS(λ))dλ+∫590780ΔS(λ)dλ (3-2)
a distance Duv of the spectral power distribution φ(λ) of object light from a black-body radiation locus defined by ANSI C78.377 satisfies
−0.0220≤Duv≤−0.0070;
when a maximum value of spectral intensity in a range of 430 nm or more and 495 nm or less is defined as φBM-max and a minimum value of spectral intensity in a range of 465 nm or more and 525 nm or less is defined as φBG-min, the spectral power distribution φ(λ) of object light satisfies
0.2250≤φBG-min/φBM-max≤0.7000; and
in the spectral power distribution φ(λ) of object light, when a maximum value of spectral intensity in a range of 590 nm or more and 780 nm or less is defined as φRM-max, a wavelength λRM-max that provides φRM-max satisfies
605(nm)≤λRM-max≤653(nm).
[47]
The method for manufacturing a light-emitting device according to [46], wherein light having Φelm3(λ) satisfies all of Conditions I to IV described below and light having φSSL3(λ) also satisfies all of the Conditions I to IV described below.
when a*n and b*n (where n is a natural number from 1 to 15) respectively denote the a* value and b* value in the CIE 1976 L*a*b* color space of the following 15 Munsell renotation color samples of #01 to #15 based on a mathematical assumption that illumination is performed by the object light, and
when a*nref and b*nref (where n is a natural number from 1 to 15) respectively denote the a* value and b* value in the CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples based on a mathematical assumption that illumination is performed by reference light which is selected in accordance with the correlated color temperature T (K) of the object light, each saturation difference ΔCn satisfies
−4.00≤ΔCn≤8.00(where n is a natural number from1to15);
an average saturation difference of the object light represented by the following formula (3-3) satisfies
when a maximum saturation difference value of the object light is denoted by ΔCmax and a minimum saturation difference value of the object light is denoted by ΔCmin, a difference |ΔCmax−ΔCmin| between the maximum saturation difference value and the minimum saturation difference value satisfies
2.00≤|ΔCmax−ΔCmin|≤10.00,
where ΔCn=√{(a*n)2+(b*n)2}−√{(a*nref)2+(b*nref)2},
with the 15 Munsell renotation color samples being:
and
when θn (degrees) (where n is a natural number from 1 to 15) denotes a hue angle in the CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples based on a mathematical assumption that illumination is performed by the object light, and
when θnref (degrees) (where n is a natural number from 1 to 15) denotes a hue angle in the CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples based on a mathematical assumption that illumination is performed by reference light which is selected in accordance with the correlated color temperature T of the object light, an absolute value of each difference in hue angles |Δhn| satisfies
0.00 degree≤|Δhn|≤12.50 degrees(where n is a natural number from1to15),
where Δhn=θn−θnref.
In addition, to achieve the above objects, the second aspect of the third invention of the present invention relates to the following matters.
[43]
A method for designing a light-emitting device having a light-emitting element and a control element,
the light-emitting device at least including as the light-emitting element
a blue semiconductor light-emitting element,
a green phosphor, and
a red phosphor,
wherein the method for designing involves designing the light-emitting device so that
when λ(nm) denotes wavelength,
Φelm3(λ) denotes a spectral power distribution of light emitted from the light-emitting element in a main radiant direction, and φSSL3(λ) denotes a spectral power distribution of light emitted from the light-emitting device in the main radiant direction,
light having Φelm3(λ) does not satisfy at least one of Conditions 1 to 4 described above but light having φSSL3(λ) satisfies all of the Conditions 1 to 4 described above.
[44]
The method for designing a light-emitting device according to [43], wherein light having Φelm3(λ) does not satisfy at least one of Conditions I to IV described above but light having φSSL3(λ) satisfies all of the Conditions I to IV described above.
[45]
A method for designing a light-emitting device having a light-emitting element and a control element,
the light-emitting device at least including as the light-emitting element
a blue semiconductor light-emitting element,
a green phosphor, and
a red phosphor,
wherein the method for designing involves designing the light-emitting device so that
when λ(nm) denotes wavelength,
Φelm3(λ) denotes a spectral power distribution of light emitted from the light-emitting element in a main radiant direction, and φSSL3(λ) denotes a spectral power distribution of light emitted from the light-emitting device in the main radiant direction,
light having Φelm3(λ) satisfies all of Conditions 1 to 4 described above and light having φSSL3(λ) also satisfies all of the Conditions 1 to 4 described above.
[46]
The method for designing a light-emitting device according to [45], wherein light having Φelm3(λ) satisfies all of Conditions I to IV described above and light having φSSL3(λ) also satisfies all of the Conditions I to IV described above.
In addition, to achieve the above objects, the fourth aspect of the third invention of the present invention relates to the following matters.
[47]
An illumination method comprising an illuminated object preparing step of preparing an illuminated object and an illuminating step of illuminating an object by light emitted from a light-emitting device having a light-emitting element and a control element, wherein
the light-emitting device at least includes as the light-emitting element
a blue semiconductor light-emitting element,
a green phosphor, and
a red phosphor, and
in the illuminating step, when light emitted from the light-emitting element illuminates the object, light measured at a position of the object does not satisfy at least one of <1> to <4> described below, but when light emitted from the light-emitting device illuminates the object, light measured at a position of the object satisfies all of <1> to <4> described below.
<1>
When a*n and b*n (where n is a natural number from 1 to 15) respectively denote the a* value and the b* value in the CIE 1976 L*a*b* color space of the following 15 Munsell renotation color samples of #01 to #15 based on a mathematical assumption that illumination is performed by light emitted from the light-emitting device as measured at a position of the object, and
when a*nref and b*nref (where n is a natural number from 1 to 15) respectively denote the a* value and the b* value in the CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples based on a mathematical assumption that illumination is performed by reference light which is selected in accordance with a correlated color temperature T(K) of light emitted from the light-emitting device as measured at a position of the object, each saturation difference ΔCn satisfies
−4.00≤ΔCn≤8.00 (where n is a natural number from 1 to 15);
<2>
an average saturation difference represented by the following formula (3-3) satisfies
<3>
when a maximum saturation difference value is denoted by ΔCmax and a minimum saturation difference value is denoted by ΔCmin, a difference |ΔCmax−ΔCmin| between the maximum saturation difference value and the minimum saturation difference value satisfies
2.00≤|ΔCmax−ΔCmin|≤10.00,
where ΔCn=√{(a*n)2+(b*n)2}−√{(a*nref)2+(b*nref)2},
with the 15 Munsell renotation color samples being:
and
<4>
When θn (degrees) (where n is a natural number from 1 to 15) denotes a hue angle in the CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples based on a mathematical assumption that illumination is performed by the light emitted from the light-emitting device as measured at a position of the object, and
when θnref (degrees) (where n is a natural number from 1 to 15) denotes a hue angle in the CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples based on a mathematical assumption that illumination is performed by reference light which is selected in accordance with the correlated color temperature T of the light emitted from the light-emitting device as measured at a position of the object, an absolute value of each difference in hue angles |Δhn| satisfies
0.00 degree≤|Δhn|≤12.50 degrees (where n is a natural number from 1 to 15),
where Δhn=θn−θnref.
[48]
The illumination method according to [47], wherein illumination is provided so as to further satisfy all of <5> to <8> described below.
<5>
When λ denotes wavelength, φ(λ) denotes a spectral power distribution of light emitted from the light-emitting device as measured at a position of the object,
φref(λ) denotes a spectral power distribution of reference light which is selected in accordance with a correlated color temperature T of the light emitted from the light-emitting device as measured at a position of the object,
(X, Y, Z) denote tristimulus values of the light emitted from the light-emitting device as measured at a position of the object,
(Xref, Yref, Zref) denote tristimulus values of reference light which is selected in accordance with T of the light emitted from the light-emitting device as measured at a position of the object,
a normalized spectral power distribution S(λ) of the light emitted from the light-emitting device as measured at a position of the object, a normalized spectral power distribution Sref(λ) of reference light which is selected in accordance with T (K) of the light emitted from the light-emitting device as measured at a position of the object, and a difference ΔS(λ) of between normalized spectral power distributions are respectively defined as
S(λ)=φ(λ)/Y,
S
ref(λ)=φref(λ)/Yref,
ΔS(λ)=Sref(λ)−S(λ), and
in a case where λRL-max (nm) represents a wavelength that provides a longest wavelength local maximum value of S(λ) in a wavelength range of 380 nm or more and 780 nm or less, and when a wavelength Λ4 that is represented by S(λRL-max)/2 exists on a longer wavelength-side of λRL-max,
an index Acg represented by the following formula (3-1) satisfies
−10.0<Acg≤120.0,
but in a case where λRL-max (nm) represents a wavelength that provides the longest wavelength local maximum value of S(λ) in a wavelength range of 380 nm or more and 780 nm or less, and when the wavelength Λ4 that is represented by S(λRL-max)/2 does not exist on the longer wavelength-side of λRL-max,
an index Acg represented by the following formula (3-2) satisfies
−10.0<Acg≤120.0.
[Expression 53]
A
cg=∫380495ΔS(λ)dλ+∫495590(−ΔS(λ))dλ+∫590Λ4ΔS(λ)dλ (3-1)
[Expression 54]
A
cg=∫380495ΔS(λ)dλ+∫495590(−ΔS(λ))dλ+∫590780ΔS(λ)dλ (3-2)
<6>
a distance Duv of the spectral power distribution φ(λ) of light from a black-body radiation locus defined by ANSI C78.377 satisfies
−0.0220≤Duv≤−0.0070;
<7>
when a maximum value of spectral intensity in a range of 430 nm or more and 495 nm or less is defined as φBM-max and a minimum value of spectral intensity in a range of 465 nm or more and 525 nm or less is defined as φBG-min, the spectral power distribution φ(λ) of light satisfies
0.2250≤φBG-min/φBM-max≤0.7000; and
<8>
in the spectral power distribution φ(λ) of light, when a maximum value of spectral intensity in a range of 590 nm or more and 780 nm or less is defined as φRM-max, a wavelength λRM-max that provides φRM-max satisfies
605(nm)≤λRM-max≤653(nm).
[49]
An illumination method comprising an illuminated object preparing step of preparing an illuminated object and an illuminating step of illuminating an object by light emitted from a light-emitting device having a semiconductor light-emitting element as a light-emitting element and a control element, wherein
the light-emitting device at least includes as the light-emitting element
a blue semiconductor light-emitting element,
a green phosphor, and
a red phosphor, and
in the illuminating step, when light emitted from the light-emitting element illuminates the object, light measured at a position of the object satisfies all of <1> to <4> described above, and when light emitted from the light-emitting device illuminates the object, light measured at a position of the object also satisfies all of <1> to <4> described above.
[50]
The illumination method according to [49], the light measured at a position of the object satisfies <5> to <8> described above.
The third invention of the present invention can realize a light-emitting device and an illumination method that are capable of realizing a truly favorable appearance of colors of object which, even with substantially similar CCT and substantially similar luminance, many test subjects would statistically determine to be better than a case where illumination is provided by reference light (also referred to as “experimental reference light”), a case where illumination is provided by a light-emitting device that irradiates light of which appearance of colors is close to reference light and which has high Ra and high Ri (also referred to as “experimental pseudo-reference light”), and can improve the appearance of colors of a light-emitting device which currently exists or is currently in use and which includes a semiconductor light-emitting device with inferior appearance of colors to the favorable appearance of colors mentioned above. Furthermore, according to the third invention of the present invention, the appearance of colors of the semiconductor light-emitting device, which excels in the appearance of colors, can be further adjusted according to the taste of the user using a similar technique.
In particular, even with a semiconductor light-emitting device with inferior color appearance when used for illumination purposes, a natural, vivid, highly visible and comfortable appearance of colors and appearance of objects, as if the object are seen outdoors, can be realized. Effects of such a color appearance can be illustrated in more concrete terms as follows.
First, when illuminating by a light-emitting device according to the third invention of the present invention such as a light source, a fixture, or a system or illuminating with the illumination method according to the third invention of the present invention, compared to cases where illumination is performed with experimental reference light or experimental pseudo-reference light, white appears whiter, more natural, and more comfortable even at an approximately similar CCT and/or an approximately similar illuminance. Furthermore, differences in lightness among achromatic colors such as white, gray, and black become more visible. As a result, for example, black letters or the like on an ordinary sheet of white paper become more legible. Moreover, while details will be given later, such an effect is completely unexpected in the context of conventional wisdom.
Second, with illuminance that is realized by a light-emitting device according to the third invention of the present invention or illuminance when illuminating with the illumination method according to the third invention of the present invention, a truly natural color appearance as though viewed under several tens of thousands of lx such as under outdoor illuminance on a sunny day is achieved for a majority of colors such as purple, bluish purple, blue, greenish blue, green, yellowish green, yellow, reddish yellow, red, and reddish purple, and in some cases, all colors even in an ordinary indoor environment of around several thousand lx to several hundred lx. In addition, the skin colors of subjects (Japanese), various foods, clothing, wooden colors, and the like which have intermediate chroma also acquire a natural color appearance which many of the subjects feel more favorable.
Third, when illuminating by a light-emitting device according to the third invention of the present invention or illuminating with the illumination method according to the third invention of the present invention, colors among close hues can be identified more easily and work or the like can be performed as comfortably as though under a high-illuminance environment as compared to cases where illumination is performed with experimental reference light or experimental pseudo-reference light even at an approximately similar CCT and/or an approximately similar illuminance. Furthermore, specifically, for example, a plurality of lipsticks with similar red colors can be more readily distinguished from each other.
Fourth, when illuminating by a light source, a fixture, or a system according to the third invention of the present invention or illuminating with the illumination method according to the third invention of the present invention, objects can be viewed more clearly and readily as though viewed under a high-illuminance environment as compared to cases where illumination is performed with experimental reference light or experimental pseudo-reference light even at an approximately similar CCT and/or an approximately similar illuminance.
In addition to these effects, the appearance of colors can be further adjusted in accordance with the taste of the user, even in a semiconductor ligh-emitting device which excels in the appearance of colors when used for illumination purposes.
Hereinafter, while the third invention of the present invention will be described in detail, the following description presents differences from the description of the first invention of the present invention. For descriptions common to the first invention and the third invention of the present invention, the description of the first invention of the present invention provided earlier will apply.
While the third invention of the present invention will be described in detail hereinafter, it is to be understood that the third invention of the present invention is not limited to the embodiments described below and that various modifications can be made without departing from the spirit and scope of the invention.
A first aspect of the third invention of the present invention is a light-emitting device. A light-emitting device according to the first aspect of the third invention of the present invention has a light-emitting element and a control element.
The control element according to the first aspect of the third invention of the present invention is a passive element that itself has no amplifying function, and is not especially limited if the intensity modulation for each wavelength can be performed in an appropriate range, on light that is emitted from a light-emitting element or a light-emitting device having relatively low level processing, in the main direction, and can constitute a light-emitting device having high level processing. Examples of the control element of the first aspect of the third invention of the present invention are passive devices, such as a reflection mirror, an optical filter and an optical lens. The control element according to the first aspect of the third invention of the present invention may be an absorption material that is disposed in the sealing material of the packaged LED, so as to perform intensity modulation for each wavelength in an appropriate range. However, a light-emitting element and a reflection mirror, optical filter, an absorption material or the like that can perform intensity modulation, of which wavelength dependency is low, on the light emitted from a light-emitting device having relatively low level processing, are not included in the control element.
An overview of the light-emitting device according to the first aspect of the third invention of the present invention will be further described with reference to
An overview of the light-emitting device according to the first aspect of the third invention of the present invention will be further described with reference to
The light (radiant flux) emitted from the light-emitting element in the main radiant direction that is referred to in this description is a total of the light (radiant flux) emitted from all the light-emitting elements in the main radiant direction, and here this spectral power distribution is denoted as Φelm3(λ). Φelm3(λ) is a function of the wavelength λ. Φelm3(λ) can be measured by performing radiant measurement for the light-emitting device, from which the control element according to this description is removed. In the case of the light-emitting device which includes the LED chip and the phosphor as the light-emitting element, and which has an optical filter that performs intensity modulation for each wavelength in an appropriate range as the control element, as shown in
If there is “a light-emitting device having mid-level processing or a light-emitting device having high level processing” which partially exists in “a light-emitting device having even higher level processing” as shown in
According to the first aspect of the third invention of the present invention, on the other hand, the spectral power distribution Φelm3(λ) of the light, emitted from a light-emitting element included in the light-emitting device in a main radiant direction, is controlled by a control element included in the light-emitting device, and the light is then emitted in the “main radiant direction”. Therefore, light-emitting devices capable of radiating light including light in a “main radiant direction” which meets requirements of the third invention of the present invention controlled by the control element are to be included in the spirit and scope of the third invention of the present invention. According to the fifth and second aspect of the third invention of the present invention, a method for manufacturing and a method for designing a light-emitting device that can irradiate light, including light in the “main radiant direction” which satisfies the requirement of the third invention of the present invention controlled by the control element, are provided, and manufacturing and designing of the light-emitting device by disposing the control element that belongs to the scope of the third invention of the present invention. In addition, an illumination method according to a fourth aspect of the third invention of the present invention specifies the invention based on light at a position where an object is illuminated in a case where light emitted from the light-emitting device illuminates the object. Therefore, illumination methods used by light-emitting devices capable of emitting light at a “position where an object is illuminated” which meets requirements of the third invention of the present invention by disposing the control element are to be included in the spirit and scope of the third invention of the present invention.
The spectral power distribution of light emitted from the light-emitting device in the main radiant direction is preferably measured at a distance where luminance at the measurement is practical luminance such as between 5 lx and 10000 lx.
Although a light-emitting device according to the first aspect of the third invention of the present invention includes a light-emitting element and has at least a blue semiconductor light-emitting element, a green phosphor and a red phosphor as the light-emitting element, the light-emitting device may include other light-emitting elements. The other light-emitting elements are not particularly limited as long as it can emit light corresponding to a range of 380 nm to 780 nm in some way, and examples of the light-emitting element include thermal emission light from a hot filament or the like, electric discharge emission light from a fluorescent tube, a high-pressure sodium lamp, or the like, stimulated emission light from a laser or the like, spontaneous emission light from a semiconductor light-emitting element, and spontaneous emission light from a phosphor. The light-emitting device according to the first aspect of the third invention of the present invention includes a control element as well, but other configurations are not especially limited. An individual semiconductor light-emitting element to which a lead or the like as a conducting mechanism is added or a packaged LED to which a heat dissipating mechanism is further added and integrated with a phosphor, chip-on-board or the like may be adopted as the light-emitting element. The light-emitting device can be an LED module in which a robust heat dissipating mechanism is added to one or more packaged LEDs and which is generally mounted with a plurality of packaged LEDs may be adopted as the light-emitting device. Furthermore, an LED lighting fixture in which a lens, a reflecting mechanism, and the like are added to a packaged LED may be adopted. Moreover, a lighting system which supports a large number of LED lighting fixtures or the like and which is configured to be capable of illuminating an object may be adopted. Still further, for example, an individual electric discharge tube to which a mechanism capable of applying a high voltage is added or an electric discharge tube having a phosphor arranged in the interior or circumference thereof may be adopted as the light-emitting device according to the first aspect of the third invention of the present invention when the light-emitting device includes an electric discharge tube as the light-emitting element. A lighting fixture in which a plurality of fluorescent tubes incorporating one or more phosphors are disposed may also be adopted. Furthermore, a lighting fixture to which a reflecting mechanism or the like is added may be adopted. Moreover, a control circuit or the like may be added to the lighting fixture to provide a lighting system. The light-emitting device according to the first aspect of the third invention of the present invention encompasses all of the above.
In the third invention of the present invention, the light-emitting element may be a light-emitting device. In other words, the light-emitting element according to the third invention of the present invention may be an LED module, an LED lighting fixture, a lighting system, or a lighting fixture having another mechanism.
On the other hand, a spectral power distribution φSSL3(λ) of the light-emitting device itself according to the first aspect of the third invention is based on characteristics when power is being continuously supplied thereto and is characterized by the following indexes.
Specifically, the spectral power distribution φSSL3(λ) of the light-emitting device is characterized by a maximum value φSSL3-BM-max of spectral intensity and a wavelength λSSL3-BM-max that provides the maximum value φSSL3-BM-max of spectral intensity in a range of 430 nm or more and 495 nm or less,
a minimum value φSSL3-BG-min of spectral intensity and a wavelength λSSL3-BG-min that provides the minimum value φSSL3-BG-min of spectral intensity in a range of 465 nm or more and 525 nm or less,
a maximum value φSSL3-RM-max of spectral intensity and a wavelength λSSL3-RM-max that provides the maximum value φSSL3-RM-max of spectral intensity in a range of 590 nm or more and 780 nm or less, and
λSSL3-RL-max that provides a longest wavelength local maximum value φSSL3-RL-max of a normalized spectral power distribution SSSL3(λ) which is derived from the spectral power distribution φSSL3 (λ) in a range of 380 nm or more and 780 nm or less which is used in the definition of an index Acg(φSSL3(λ)) to be described later.
Therefore, for example, λCHIP-BM-dom generally differs from λSSL3-BM-max and λPHOS-RM-max also generally differs from λSSL3-RM-max. On the other hand, λSSL3-RL-max may sometimes assume a same value as λSSL3-RM-max.
Moreover, while a spectral power distribution of light emitted from a light-emitting element may be denoted by Φelm3(λ) and a spectral power distribution of light emitted from a light-emitting device may be denoted by φSSL3(λ) in the present specification, the spectral power distribution of both lights may be denoted by φ(λ) in cases of generalization. In a similar manner, in a general spectral power distribution φ(λ) of light, indexes derived according to same concepts as φSSL3-BM-max, λSSL3-BM-max, and the like may sometimes be represented by omitting the suffix SSL3 as φBM-max, λBM-max, and the like.
<Index Acg(φSSL3(λ))>
The index Acg(φSSL3(λ) is defied as below, as disclosed as the index Acg in Japanese Patent No. 5252107 and Japanese Patent No. 5257538.
Let φSSL-ref3(λ) and φSSL3(λ) respectively denote spectral power distributions of calculational reference light and test light which represent color stimuli that differ from one another when measuring light emitted in a main radiant direction from a light-emitting device of the first aspect of the third invention of the present invention, x(λ), y(λ), and z(λ) denote a color-matching function, and (XSSL-ref3, YSSL-ref3, ZSSL-ref3) and (XSSL3, YSSL3, ZSSL3) respectively denote tristimulus values corresponding to the calculational reference light and the test light. In this case, the following is satisfied regarding the calculational reference light and the test light, where k denotes a constant.
Y
SSL-ref3
=k∫φ
SSL-ref3(λ)·y(λ)dλ
Y
SSL3
=k∫φ
SSL3(λ)·y(λ)dλ
At this point, normalized spectral power distributions obtained by normalizing the spectral power distributions of the calculational reference light and the test light by their respective Y were defined as
S
SSL-ref3(λ)=φSSL-ref3(λ)/YSSL-ref3and
S
SSL3(λ)=φSSL3(λ)/YSSL3,
and a difference between the normalized reference light spectral power distribution and the normalized test light spectral power distribution was represented by
ΔSSSL3(λ)=SSSL-ref3(λ)−SSSL3(λ).
Furthermore, at this point, the index Acg(φSSL3(λ)) was defined as follows.
A
cg(ϕSSL3(λ))=∫Λ1Λ2ΔSSSL3(λ)dλ+∫Λ2Λ3(−ΔSSSL3(λ))dλ+∫Λ3Λ4ΔSSSL3(λ)dλ [Expression 55]
Moreover, upper and lower limit wavelengths of the integrals were respectively set to
Λ1=380 nm,
Λ2=495 nm, and
Λ3=590 nm.
In addition, Λ4 is defined by dividing Λ4 into the two cases described below. First, if a wavelength that provides a longest wavelength local maximum value in a range of 380 nm or more and 780 nm or less in a normalized test light spectral power distribution SSSL3(λ) is denoted by λSSL3-RL-max (nm) and a normalized spectral intensity thereof is denoted by SSSL3(λSSL3-RL-max), then a wavelength which is on a longer wavelength-side of λSSL3-RL-max and which has an intensity of SSSL3(λSSL3-RL-max)/2 is denoted as Λ4. If such a wavelength does not exist in a range up to 780 nm, then Λ4 is assumed to be 780 nm.
Moreover, while a spectral power distribution of light emitted from a light-emitting element may be denoted by Φelm3(λ) and a spectral power distribution of light emitted from a light-emitting device may be denoted by φSSL3(λ) in the present specification, the spectral power distribution of both lights may be denoted by φ(λ) in cases of generalization. In a similar manner, in a general spectral power distribution φ(λ) of light, indexes derived according to same concepts as SSSL3(λ) and the like may sometimes be represented by omitting the suffix SSL3 as SSSL3(λ) and the like.
<φSSL3-BG-min/φSSL3-BM-max and φSSL3-BG-min/φSSL3-RM-max>
φSSL3-BG-min mainly appears in a portion where a longer wavelength-side tail (a base portion where spectral radiant flux intensity decreases) of a spectral radiant flux due to emission of light by a blue semiconductor light-emitting element and a shorter wavelength side tail (a base portion where spectral radiant flux intensity decreases) of a spectral radiant flux due to emission of light by a light-emitting element responsible for the intermediate wavelength region overlap with each other. In other words, φSSL3-BG-min often occurs as a recess with a shape of φSSL3(λ) in a range of 465 nm or more and 525 nm or less which straddles the short wavelength region and the intermediate wavelength region.
In order to relatively uniformly improve saturation of color appearance of the 15 specific mathematically-derived Munsell renotation color samples to be described later, φSSL3-BG-min/φSSL3-BM-max obtained by normalizing φSSL3-BG-min with a maximum value of spectral intensity in a range of 430 nm to 495 nm and φSSL3-BG-min/φSSL3-RM-max obtained by normalizing φSSL3-BG-min with a maximum value of spectral intensity in a range of 590 nm to 780 nm must be controlled with care. In other words, in the light-emitting device according to the first aspect of the third invention of the first invention, φSSL3-BG-min/φSSL3-BM-max and φSSL3-BG-min/φSSL3-RM-max have optimum ranges as will be described later.
Moreover, while a spectral power distribution of light emitted from a light-emitting element may be denoted by Φelm3(λ) and a spectral power distribution of light emitted from a light-emitting device may be denoted by φSSL3(λ) in the present specification, the spectral power distribution of both lights may be denoted by φ(λ) in cases of generalization. In a similar manner, in a general spectral power distribution φ(λ) of light, indexes derived according to same concepts as φSSL3-BG-min, φSSL3-RM-max, and the like may sometimes be represented by omitting the suffix SSL3 as φBG-min, λRM-max, and the like.
When the light-emitting device according to the first aspect of the third invention emits test light in the main radiant direction, the a* values and the b* values of the 15 color samples in the CIE 1976 L*a*b* color space of the test light (related to the light-emitting device according to the first aspect of the third invention of the present invention) are to be respectively denoted by a*nSSL3 and b*nSSL3 (where n is a natural number from 1 to 15), and hue angles of the 15 color samples are to be respectively denoted by θnSSL3 (degrees) (where n is a natural number from 1 to 15). In addition, when mathematically assuming illumination by a calculation reference light (black-body radiation light when lower than 5000 K and CIE daylight when equal to or higher than 5000 K) which is selected in accordance with the correlated color temperature TSSL3 of the test light described above, the a* values and the b* values of the 15 color samples in the CIE 1976 L*a*b* color space are to be respectively denoted by a*nSSL-ref3 and b*nSSL-ref3 (where n is a natural number from 1 to 15), and hue angles of the 15 color samples are to be respectively denoted by θnSSL-ref3 (degrees) (where n is a natural number from 1 to 15). In this case, an absolute value |ΔhnSSL3| of each difference in hue angles ΔhnSSL3 (degrees) (where n is a natural number from 1 to 15) of each of the 15 Munsell renotation color samples when illuminated by the two types of light may be represented by
|ΔhnSSL3|=|θnSSL3−θnSSL-ref3|.
Moreover, while a spectral power distribution of light emitted from a light-emitting element may be denoted by Φelm3(λ) and a spectral power distribution of light emitted from a light-emitting device may be denoted by φSSL3(λ) in the present specification, the spectral power distribution of both lights may be denoted by φ(λ) in cases of generalization. In a similar manner, in a general spectral power distribution φ(λ) of light, indexes derived according to same concepts as ΔhnSSL3, θnSSL3, a*nSSL3, and the like may sometimes be represented by omitting the suffix SSL3 as Δhn, θn, a*n, and the like. In addition, indexes derived according to same concepts as θnSSL-ref3, and the like may sometimes be represented by omitting the suffix SSL3 as θnref, and the like.
In addition, each saturation difference ΔCnSSL3 (where n is a natural number from 1 to 15) of the 15 Munsell renotation color samples when assuming illumination by the test light and the calculation reference light is represented by
ΔCnSSL3=√{(a*nSSL3)2+(b*nSSL3)2}−√{(a*nSSL-ref3)2+(b*nSSL-ref3)2}.
Furthermore, an average saturation difference of the 15 Munsell renotation color samples is represented by
(hereinafter, may be denoted as SATave(φSSL3(λ)). Moreover, when a maximum saturation difference value of the 15 Munsell renotation color samples is denoted by ΔCSSL-max3 and a minimum saturation difference value is denoted by ΔCSSL-min3, a difference between a maximum saturation difference and a minimum saturation difference (difference among differences between maximum and minimum degrees of saturation) is represented by
|ΔCSSL-max3−ΔCSSL-min3|.
Moreover, while a spectral power distribution of light emitted from a light-emitting element may be denoted by Φelm3(λ) and a spectral power distribution of light emitted from a light-emitting device may be denoted by φSSL3(λ) in the present specification, the spectral power distribution of both lights may be denoted by φ(λ) in cases of generalization. In a similar manner, in a general spectral power distribution φ(λ) of light, indexes derived according to same concepts as θnSSL3, a*nSSL3, and the like may sometimes be represented by omitting the suffix SSL3 as θn, a*n, and the like. In addition, indexes derived according to same concepts as ΔCSSL3-max, and the like may sometimes be represented by omitting the suffix SSL3 as ΔCmax, and the like.
<Luminous Efficacy of Radiation KssL3 (Lm/W) and Luminous Efficacy of a Source ηssL3 (Lm/W)>
Furthermore, when evaluating the test light spectral power distribution φSSL3(λ) when measuring light emitted in a main radiant direction from a light-emitting device of the first aspect of the third invention of the present invention, the widely-used definition below was adopted for luminous efficacy of radiation KssL3 (lm/W).
K
SSL3
=Km×[∫380780{ϕSSL3(λ)×V(λ)}dλ]/[∫380780ϕSSL3(λ)dλ] [Expression 57]
In the equation above,
Km: maximum luminous efficacy (lm/W),
V(λ): spectral luminous efficiency, and
λ: wavelength (nm).
Therefore, a luminous efficacy of radiation KSSL3 (lm/W) of a test light spectral power distribution φSSL3(λ) when measuring light in the main radiant direction emitted from the light-emitting device according to the first aspect of the third invention of the present invention can be described as efficiency inherent in the shape of the spectral power distribution.
On the other hand, light source efficiency ηSSL3 (lm/W) is a quantity indicating how much of power supplied to the light-emitting device according to the first aspect of the third invention of the present invention is converted into a luminous flux.
Furthermore, the luminous efficacy of radiation KSSL3 (lm/W) of a test light spectral power distribution φSSL3(λ) when measuring light in the main radiant direction emitted from the light-emitting device is efficiency inherent in the shape of the spectral power distribution itself and may be described as a quantity that equals light source efficiency ηSSL3 (lm/W) when assuming that characteristics of all materials constituting the light-emitting device (for example, internal quantum efficiency of semiconductor light-emitting elements, light extraction efficiency, internal quantum efficiency of phosphors, external quantum efficiency, and efficiency related to light transmission characteristics of encapsulants) have 100% efficiency.
Moreover, while a spectral power distribution of light emitted from a light-emitting element may be denoted by Φelm3(λ) and a spectral power distribution of light emitted from a light-emitting device may be denoted by φSSL3(λ) in the present specification, the spectral power distribution of both lights may be denoted by φ(λ) in cases of generalization. In a similar manner, in a general spectral power distribution φ(λ) of light, indexes derived according to same concepts as KSSL3, ηSSL3, and the like may sometimes be represented by omitting the suffix SSL3 as K, η, and the like.
The present inventor, first, mathematically and experimentally evaluated whether or not both preferable color appearance and high light source efficiency can be achieved when the index Acg has a value outside a range of −360 or more and −10 or less and particularly a value larger than −10 without a function of a control element. The description of the first invention of the present invention will be applied to this evaluation.
Results of experimental examples and the like presented in the description of the first aspect of the first invention of the present invention reveal that, even with a light-emitting device including a control element according to the first aspect of the third invention of the present invention, the various indexes shown in Tables 1-2 to 1-15 are favorably within appropriate ranges in order to obtain such perception. This requirement also applies to each parameter related to the method for manufacturing a light-emitting device according to the fifth aspect of the third invention of the present invention and to each parameter related to the method for designing a light-emitting device according to the second aspect of the third invention in a similar manner to a light-emitting device according to the first aspect of the third invention described above.
In addition, it was found that, in order to obtain such perception with a illumination method according to the fourth aspect of the third invention of the present invention, the various indexes shown in Tables 1-2 to 1-15 are favorably within appropriate ranges.
In particular, from the results of the test lights judged to be favorable in the visual experiments, in consideration of the characteristics of |Δhn|, SATave, ΔCn, and |ΔCmax−ΔCmin|, it was found that the following trends exist. Specifically, test lights which produced a favorable color appearance or a favorable object appearance had the following characteristics with respect to the color appearance of the 15 color samples when illumination by calculational reference light is assumed and the color appearance of the 15 color samples when illumination by an actually measured test light spectral power distribution is assumed.
The difference in hue angles (|Δhn|) of the 15 color samples between illumination by test lights and illumination by calculational reference light is relatively small, and an average saturation, SATave, of the 15 color samples when illuminated by the test lights had increased in an appropriate range as compared to that when illuminated by the calculational reference light. Moreover, in addition to the average values, individual saturations (ΔCn) of the 15 color samples also show that none of the respective ΔCn of the 15 color samples when illuminated by the test lights was excessively lower or higher than the same values when illuminated by the calculational reference light and were all in appropriate ranges. As a result, the difference among differences between maximum and minimum degrees of saturation |ΔCmax−ΔCmin| was narrow in an appropriate range. When further simplified, it is inferable that an ideal case features small differences in hue angles among the hues of all 15 color samples and a relatively uniform increase in saturation of the 15 color samples within appropriate ranges when assuming illumination by test light as compared to when assuming illumination of the 15 color samples by reference light.
A solid line in
Furthermore,
In this manner, it is shown that when a favorable color appearance or a favorable object appearance is obtained in the visual experiments, differences in hue angles among the hues of all 15 color samples are small and saturation of the 15 color samples increase relatively uniformly within appropriate ranges when assuming illumination by the test light as compared to when assuming illumination of the 15 color samples by the reference light.
Furthermore, the selection of each saturation difference ΔCn described in Condition I is conceivably characterized as follows when considering the results classified into ranks +1 to +5.
Each saturation difference ΔCn can be selected from a range of −4.00 or more and 8.00 or less,
based on the results of all experimental examples, slightly favorably, each saturation difference ΔCn is −3.49 or more and 7.11 or less,
based on the results of ranks +2 to +5, favorably, each saturation difference ΔCn is −3.33 or more and 7.11 or less, based on the results of ranks +4 to +5, extremely favorably, each saturation difference ΔCn is −1.73 or more and 6.74 or less, and
based on the result of rank +5, dramatically favorably, each saturation difference ΔCn is −0.93 or more and 6.74 or less.
Furthermore, the selection of the SATave described in Condition II is conceivably characterized as follows when considering the results classified into ranks +1 to +5.
The SATave can be selected from a range of 0.50 or more and 4.00 or less,
based on the results of all experimental examples, slightly favorably, the value of SATave is 0.53 or more and 3.76 or less,
based on the results of ranks +2 to +5, favorably, the SATave is 1.04 or more and 3.76 or less,
based on the results of ranks +3 to +5, more favorably, the SATave is 1.11 or more and 3.76 or less,
based on the results of ranks +4 to +5, extremely favorably, the SATave is 1.40 or more and 3.76 or less, and
based on the result of rank +5, dramatically favorably, the SATave is 1.66 or more and 3.76 or less.
Furthermore, the selection of a difference |ΔCmax−ΔCmin| between the maximum saturation difference value and the minimum saturation difference value described in Condition III is conceivably characterized as follows when considering the results classified into ranks +1 to +5.
A difference |ΔCmax−ΔCmin| can be selected from a range of 2.00 or more and 10.00 or less,
based on the results of all experimental examples, slightly favorably, the difference |ΔCmax−ΔCmin| is 3.22 or more and 9.52 or less,
based on the results of ranks +4 to +5, extremely favorably, the difference |ΔCmax−ΔCmin| is 4.12 or more and 7.20 or less, and
based on the result of rank +5, dramatically favorably, the difference |ΔCmax−ΔCmin| is 4.66 or more and 7.10 or less.
Furthermore, the selection of an absolute value of each difference in hue angles |Δhn| described in Condition IV is conceivably characterized as follows when considering the results classified into ranks +1 to +5.
A absolute value of each difference in hue angles |Δhn| can be selected from a range of 0.00 or more and 12.50 or less,
based on the results of all experimental examples, slightly favorably, the absolute value of each difference in hue angles |Δhn| is 0.00 or more and 12.43 or less,
based on the results of ranks +2 to +5, favorably, the absolute value of each difference in hue angles |Δhn| is 0.01 or more and 12.43 or less,
based on the results of ranks +3 to +5, more favorably, the absolute value of each difference in hue angles |Δhn| is 0.02 or more and 12.43 or less, and
based on the results of ranks +4 to +5, extremely favorably, the absolute value of each difference in hue angles |Δhn| is 0.02 or more and 9.25 or less.
Moreover, since an absolute value of each difference in hue angles |Δhn| is conceivably desirably 0, by adjusting a lower limit of values thereof, ideally,
a range of 0.00 or more and 12.43 or less is more favorably selected,
a range of 0.00 or more and 9.25 or less is extremely favorably selected,
a range of 0.00 or more and 7.00 or less is more extremely favorably selected, and
a range of 0.00 or more and 5.00 or less is further extremely favorably selected.
Furthermore, the selection of an index Acg described in Condition 1 is conceivably characterized as follows when considering the results classified into ranks +1 to +5.
An index Acg can be selected from a range of more than −10.0 and 120.0 or less,
based on the results of all experimental examples, slightly favorably, the index is −4.6 or more and 116.3 or less,
based on the results of ranks +3 to +5, more favorably, the index is −4.6 or more and 87.7 or less,
based on the results of ranks +4 to +5, extremely favorably, the index is −4.6 or more and 70.9 or less, and
based on the result of rank +5, dramatically favorably, the index is −1.5 or more and 26.0 or less.
Furthermore, the selection of a Duv described in Condition 2 is conceivably characterized as follows when considering the results classified into ranks +1 to +5.
A distance Duv can be selected from a range of −0.0220 or more and −0.0070 or less,
based on the results of all experimental examples, slightly favorably, the distance Duv is −0.0212 or more and −0.0071 or less,
based on the results of ranks +3 to +5, more favorably, the distance Duv is −0.0184 or more and −0.0084 or less,
based on the results of ranks +4 to +5, extremely favorably, the distance Duv is −0.0161 or more and −0.0084 or less, and
based on the result of rank +5, dramatically favorably, the distance Duv is −0.0145 or more and −0.0085 or less.
Moreover, based on an overall trend, Duv is further dramatically favorably selected from a range of −0.0145 or more and −0.0090 or less, even more dramatically favorably selected from a range of −0.0140 or more and less than −0.0100, and still even more dramatically favorably selected from a range of −0.0135 or more and less than −0.0120.
Furthermore, the selection of a value of φBG-min/φBM-max described in Condition 3 is conceivably characterized as follows when considering the results classified into ranks +1 to +5.
A value of φBG-min/φBM-max can be selected from a range of 0.2250 or more and 0.7000 or less,
based on the results of all experimental examples, slightly favorably, the value of φBG-min/φBM-max is 0.2278 or more and 0.6602 or less,
based on the results of ranks +4 to +5, extremely favorably, the value of φBG-min/φBM-max is 0.2427 or more and 0.6225 or less, and
based on the result of rank +5, dramatically favorably, the value of φBG-min/φBM-max is 0.2427 or more and 0.5906 or less.
Furthermore, the selection of a wavelength λRM-max described in Condition 4 is conceivably characterized as follows when considering the results classified into ranks +1 to +5.
A wavelength λRM-max can be selected from a range of 605 nm or more and 653 nm or less,
based on the results of all experimental examples, slightly favorably, the wavelength λRM-max is selected from a range of 606 nm or more and 652 nm or less,
based on the results of ranks +3 to +5, more favorably, the wavelength λRM-max is 607 nm or more and 647 nm or less, and
based on the results of ranks +4 to +5, extremely favorably, the wavelength λRM-max is 622 nm or more and 647 nm or less.
In addition, based on the trends described so far, λRM-max is conceivably further extremely favorably selected from a range of 625 nm or more and 647 nm or less.
Furthermore, based on the result of rank +5, λRM-max is dramatically favorably selected from a range of 630 nm or more and 647 nm or less.
Moreover, based on an overall trend, λRM-max is conceivably further dramatically favorably selected from a range of 631 nm or more and 647 nm or less.
These are trends that are conceivably required by the light-emitting device according to the first aspect of the third invention of the present invention to have irregularities of appropriate sizes at appropriate positions of the spectral power distribution φ(λ).
Furthermore, the selection of a wavelength λRM-max described in Condition 5 is conceivably characterized as follows when considering the results classified into ranks +1 to +5.
A wavelength λRM-max can be selected from a range of 430 nm or more and 480 nm or less,
based on the results of all experimental examples, slightly favorably, the wavelength λRM-max is selected from a range of 440 nm or more and 460 nm or less,
based on the results of ranks +4 to +5, extremely favorably, the wavelength λRM-max is 447 nm or more and 460 nm or less, and
based on the results of rank +5, dramatically favorably, the wavelength λRM-max is 450 nm or more and 457 nm or less.
In addition, based on an overall trend, λRM-max is conceivably further dramatically favorably selected from a range of 451 nm or more and 456 nm or less.
These are trends that are conceivably required by the light-emitting device according to the first aspect of the third invention of the present invention to have irregularities of appropriate sizes at appropriate positions of the spectral power distribution φ(λ).
Furthermore, the selection of a value of φBG-min/φRM-max described in Condition 6 is conceivably characterized as follows when considering the results classified into ranks +1 to +5.
A value of φBG-min/φRM-max can be selected from a range of 0.1800 or more and 0.8500 or less, based on the results of all experimental examples, slightly favorably, the value of φBG-min/φRM-max is 0.1917 or more and 0.8326 or less,
based on the results of ranks +3 to +5, more favorably, the value of φBG-min/φRM-max is 0.1917 or more and 0.6207 or less,
based on the results of ranks +4 to +5, extremely favorably, the value of φBG-min/φRM-max is 0.1917 or more and 0.6202 or less, and
based on the result of rank +5, dramatically favorably, the value of φBG-min/φRM-max is 0.1917 or more and 0.5840 or less.
Furthermore, based on an overall trend, φBG-min/φRM-max is conceivably favorably selected from a range of 0.1917 or more and 0.7300 or less.
These are trends that are conceivably required by the light-emitting device according to the first aspect of the third invention of the present invention to have irregularities of appropriate sizes at appropriate positions of the spectral power distribution φ(λ).
Furthermore, the selection of a luminous efficacy of radiation K (lm/W) described in Condition 7 is conceivably characterized as follows when considering the results classified into ranks +1 to +5.
A luminous efficacy of radiation K (lm/W) can be selected from a range of 210.0 (lm/W) or more and 290.0 (lm/W) or less,
based on the results of all experimental examples, slightly favorably, the luminous efficacy of radiation K (lm/W) is selected from a range of 212.2 (lm/W) or more and 286.9 (lm/W) or less,
based on the results of ranks +2 to +5, favorably, the luminous efficacy of radiation K (lm/W) is 212.2 (lm/W) or more and 282.3 (lm/W) or less,
based on the results of ranks +4 to +5, extremely favorably, the luminous efficacy of radiation K (lm/W) is 212.2 (lm/W) or more and 261.1 (lm/W) or less, and
based on the results of rank +5, dramatically favorably, the luminous efficacy of radiation K (lm/W) is 212.2 (lm/W) or more and 256.4 (lm/W) or less.
Furthermore, the selection of a correlated color temperature T (K) described in Condition 8 is conceivably characterized as follows when considering the results classified into ranks +1 to +5.
A correlated color temperature T (K) can be selected from a range of 2600 (K) or more and 7700 (K) or less,
based on the results of all experimental examples, slightly favorably, the correlated color temperature T (K) is 2644 (K) or more and 7613 (K) or less, and
based on the results of ranks +4 to +5, dramatically favorably, the correlated color temperature T (K) is 2644 (K) or more and 6797 (K) or less.
Next, the inventor introduced a control element, which was produced in the experiment described above, to the LED light source/fixture/system which does not include a control element, and extracted the metrological characteristics and photometric characteristics of the spectral power distribution of the light irradiated from the light-emitting device which includes the control element, based on the measured spectrum. In other words, the characteristics of numeric values, such as the index Acg, the luminous efficacy of radiation K (lm/W), CCT (K) and Duv of the light emitted from each light-emitting area and the light-emitting device in the main radiant direction, were extracted. At the same time, differences between color appearances of the 15 color samples when assuming illumination by calculational reference lights and color appearances of the 15 color samples when assuming a test light spectral power distribution actually measured were also compiled using |Δhn|, SATave, ΔCn, and |ΔCmax−ΔCmin| as indices. Moreover, while values of |Δhn| and ΔCn vary when n is selected, in this case, maximum and minimum values are shown. These values are also described in Tables 3-16, 3-17 and 3-18.
In concrete terms, the inventor experimented how Φelm3(λ), which is the spectral power distribution of the light emitted from the light-emitting element in the main radiant direction, and φSSL3(λ), which is the spectral power distribution of the light emitted from the light-emitting device in the main radiant direction, will change if the control element is included.
The experiments related to the third invention of the present invention will now be described.
Experimental Example 301
First an optical filter having spectral transmission characteristics shown in
Next, an LED lighting fixture of Experimental Example 301 was fabricated using the LED module. Here an optical filter having the spectral transmission characteristics shown in
Duv(φSSL3(λ)) of the lighting fixture of Experimental Example 301 was −0.0076, which was 0.0004 lower than −0.0072 of Duv(Φelm3(λ)) of the LED module of Reference Experimental Example 301. Acg(φSSL3(λ)) of the lighting fixture of Experimental Example 301 was 6.1, which was 64.8 lower than 70.9 of Acg(Φelm3(λ)) of the LED module of Reference Experimental Example 301. SATave(φSSL3(λ)) of the lighting fixture of Experimental Example 301 was 2.59, which was 0.92 higher than 1.67 of SATave(Φelm3(λ)) of the LED module of Reference Experimental Example 301, and a more clear and better appearance of colors was implemented when observed with a same luminance.
First an optical filter having spectral transmission characteristics shown in
Next, an LED lighting fixture of Experimental Example 302 was fabricated using the LED module. Here an optical filter having the spectral transmission characteristics shown in
Duv(φSSL3(λ)) of the lighting fixture of Experimental Example 302 was −0.0073, which was 0.0033 lower than −0.0040 of Duv(Φelm3(λ)) of the LED module of Reference Comparative Experimental Example 301. Acg(φSSL3(λ)) of the lighting fixture of Experimental Example 302 was 48.4, which was 73.9 lower than 122.3 of Acg(Φelm3(λ)) of the LED module of Reference Comparative Experimental Example 301. SATave(φSSL3(λ)) of the lighting fixture of Experimental Example 302 was 2.15, which was 2.62 higher than −0.47 of SATave(Φelm3(λ)) of the LED module of Reference Comparative Experimental Example 301.
As a result, even if a lighting fixture uses a semiconductor light-emitting element, a packaged LED and an LED module which cannot implement a good appearance of colors, an LED lighting fixture that can implement a good appearance of colors can be fabricated by the optical characteristics of a control element.
First an optical filter having spectral transmission characteristics shown in
Next, an LED lighting fixture of Experimental Example 303 is fabricated using the LED module. Here an optical filter having spectral transmission characteristics shown in
The solid line in
Duv(φSSL3(λ)) of the lighting fixture of Experimental Example 303 is −0.0123, which is 0.0006 lower than −0.0117 of Duv(Φelm3(λ)) of the LED module of Reference Comparative Experimental Example 302. Acg(φSSL3(λ)) of the lighting fixture of Experimental Example 303 is 66.9, which is 36.6 lower than 103.5 of Acg(Φelm3(λ)) of the LED module of Reference Comparative Experimental Example 302. SATave(φSSL3(λ)) of the lighting fixture of Experimental Example 303 is 2.29, which is 1.30 higher than 0.99 of SATave(Φelm3(λ)) of the LED module of Reference Comparative Experimental Example 302, and a more clear and better appearance of colors is implemented when observed with a same luminance.
An LED illumination device according to Comparative Experimental Example 301 was fabricated in a similar manner to Experimental Example 301 with the exception of preparing a package LED having a blue LED, a YAG phosphor, and a SCASN phosphor as the light-emitting element in a similar manner to Reference Comparative Experimental Example 302.
Characteristics of the LED illumination fixture according to Comparative Experimental Example 301 fabricated by mounting the optical filter shown in
Duv(φSSL3(λ)) of the lighting fixture of Comparative Experimental Example 301 is −0.0112, which is 0.0005 higher than −0.0117 of Duv(Φelm3(λ)) of the LED module of Reference Comparative Experimental Example 302. Acg(φSSL3(λ)) of the lighting fixture of Comparative Experimental Example 301 is 115.2, which is 11.7 higher than 103.5 of Acg(Φelm3(λ)) of the LED module of Reference Comparative Experimental Example 302. SATave(φSSL3(λ)) of the lighting fixture of Comparative Experimental Example 301 is 1.59, which is 0.60 higher than 0.99 of SATave(Φelm3(λ)) of the LED module of Reference Comparative Experimental Example 302.
As a result, even if a control element that can implement a good appearance of colors when combined with a specific light-emitting element, a good appearance of colors may not be implemented when this control element is combined with a lighting fixture using a different semiconductor light-emitting element, packaged LED and LED module.
(Discussion)
The following invention issues can be derived from the above mentioned experiment results.
As a result of Reference Comparative Experimental Example 301 and Experimental Example 302, or the result of Reference Comparative Experimental Example 302 and Experimental Example 303 show, the light-emitting devices of Experimental Example 302 and Experimental Example 303, which can implement a good appearance of colors, can be implemented respectively by disposing an appropriate control element in the light-emitting device of Reference Comparative Experimental Example 301 and Reference Comparative Experimental Example 302 (regarded as a light-emitting element in the third invention of the present invention), which cannot implement a good appearance of colors.
In other words, in a light-emitting device having a light-emitting element and a control element, wherein the light-emitting device at least has a blue semiconductor light-emitting element, a green phosphor, and a red phosphor as the light-emitting element, when λ (nm) is a wavelength, Φelm3(λ) is a spectral power distribution of a light which is emitted from the light-emitting element in a main radiant direction, φSSL3(λ) is a spectral power distribution of a light which is emitted from the light-emitting element in the main radiant direction, and light having Φelm3(λ) does not satisfy at least one of the following Conditions 1 to 4, and light having φSSL3(λ) satisfies all of the following Conditions 1 to 4, the light-emitting device (light-emitting element) which does not implement a good appearance of colors becomes a light-emitting device which can implement a good appearance of colors by the control element.
Particularly, if a specific control element is disposed in an LED lighting fixture which is already on the market and has not yet implemented a good appearance of colors, this LED lighting device can become a light-emitting device which can implement a good appearance of colors according to the first aspect of the third invention of the present invention.
Conditions 1 to 4 according to the first aspect of the third invention of the present invention are conditions derived from the above mentioned experimental examples.
When φ(λ) denotes a spectral power distribution of object light, φref(λ) denotes a spectral power distribution of reference light which is selected in accordance with a correlated color temperature T of the object light,
(X, Y, Z) denote tristimulus values of the object light,
(Xref, Yref, Zref) denote tristimulus values of reference light which is selected in accordance with the correlated color temperature T,
a normalized spectral power distribution S(λ) of the object light, a normalized spectral power distribution Sref(λ) of reference light of the object light, and a difference ΔS(λ) of between normalized spectral power distributions are respectively defined as
S(λ)=φ(λ)/Y,
S
ref(λ)=φref(λ)/Yref,
ΔS(λ)=Sref(λ)−S(λ), and
in a case where λRL-max (nm) represents a wavelength that provides a longest wavelength local maximum value of S(λ) in a wavelength range of 380 nm or more and 780 nm or less, and when a wavelength Λ4 that is represented by S(λRL-max)/2 exists on a longer wavelength-side of λRL-max,
an index Acg represented by the following formula (3-1) satisfies
−10.0<Acg≤120.0,
but in a case where λRL-max (nm) represents a wavelength that provides the longest wavelength local maximum value of S(λ) in a wavelength range of 380 nm or more and 780 nm or less, and when the wavelength Λ4 that is represented by S(λRL-max)/2 does not exist on the longer wavelength-side of λRL-max,
an index Acg represented by the following formula (3-2) satisfies
−10.0<Acg≤120.0,
[Expression 58]
A
cg=∫380495ΔS(λ)dλ+∫495590(−ΔS(λ))dλ+∫590Λ4ΔS(λ)dλ (3-1)
[Expression 59]
A
cg=∫380495ΔS(λ)dλ+∫495590(−ΔS(λ))dλ+∫590780ΔS(λ)dλ (3-2)
a distance Duv of the spectral power distribution φ(λ) of object light from a black-body radiation locus defined by ANSI C78.377 satisfies
−0.0220≤Duv≤−0.0070;
when a maximum value of spectral intensity in a range of 430 nm or more and 495 nm or less is defined as φBM-max and a minimum value of spectral intensity in a range of 465 nm or more and 525 nm or less is defined as φBG-min, the spectral power distribution φ(λ) of object light satisfies
0.2250≤φBG-min/φBM-max≤0.7000; and
in the spectral power distribution φ(λ) of object light, when a maximum value of spectral intensity in a range of 590 nm or more and 780 nm or less is defined as φRM-max, a wavelength λRM-max that provides φRM-max satisfies
605(nm)≤λRM-max≤653(nm).
It is preferable that light having Φelm3(λ) does not satisfy at least one of the following Conditions I to IV, and light having φSSL3(λ) satisfies all of Conditions I to IV. Conditions I to IV are also the conditions derived from the above mentioned experimental examples.
when a*n and b*n (where n is a natural number from 1 to 15) respectively denote the a* value and b* value in the CIE 1976 L*a*b* color space of the following 15 Munsell renotation color samples of #01 to #15 based on a mathematical assumption that illumination is performed by the object light, and when a*nref and b*nref (where n is a natural number from 1 to 15) respectively denote the a* value and b* value in the CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples based on a mathematical assumption that illumination is performed by reference light which is selected in accordance with the correlated color temperature T (K) of the object light, each saturation difference ΔCn satisfies
−4.00≤ΔCn≤8.00(where n is a natural number from1to15);
an average saturation difference represented by the following formula (3-3) satisfies
when a maximum saturation difference value of the object light is denoted by ΔCmax and a minimum saturation difference value of the object light is denoted by ΔCmin, a difference |ΔCmax−ΔCmin| between the maximum saturation difference value and the minimum saturation difference value satisfies
2.00≤|ΔCmax−ΔCmin|≤10.00,
where ΔCn=√{(a*n)2+(b*n)2}−√{(a*nref)2+(b*nref)2},
with the 15 Munsell renotation color samples being:
when θn (degrees) (where n is a natural number from 1 to 15) denotes a hue angle in the CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples based on a mathematical assumption that illumination is performed by the object light, and
when θnref (degrees) (where n is a natural number from 1 to 15) denotes a hue angle in the CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples based on a mathematical assumption that illumination is performed by reference light which is selected in accordance with the correlated color temperature T of the object light, an absolute value of each difference in hue angles |Δhn| satisfies
0.00 degree≤|Δhn|≤12.50 degrees(where n is a natural number from1to15),
where Δhn=θn−θnref.
According to the examination of the results of Reference Experimental Example 301 and Experimental Example 301, the light-emitting devices according to Experimental Example 301, which can implement an even better appearance of colors, can be implemented respectively by disposing an appropriate control element in the light-emitting device (regarded as a light-emitting element) according to Reference Experimental Example 301, which can implement a good appearance of colors.
In other words, in a light-emitting device having a light-emitting element and a control element, wherein the light-emitting device at least has a blue semiconductor light-emitting element, a green phosphor, and a red phosphor as the light-emitting element, if λ(nm) is a wavelength, Φelm3(λ) is the spectral power distribution of light emitted from this light-emitting element in the main radiant direction, φSSL3(λ) is the spectral power distribution of light emitted from the light-emitting device in the main radiant direction, light having Φelm3(λ) satisfies all of the above mentioned Conditions 1 to 4, and light having φSSL3(λ) satisfies all of the above mentioned Conditions 1 to 4, the light-emitting device (light-emitting element), which can implemented a good appearance of colors, becomes a light-emitting device which can implement an even better appearance of colors by the control element.
Particularly, even in a semiconductor light-emitting device in which appearance of colors is excellent when used for an illumination purpose, the appearance of colors can be further adjusted according to the taste of the user.
It is preferable that light having Φelm3(λ) satisfies all of the above mentioned Conditions I to IV, and light having φSSL3(λ) satisfies all of the above mentioned Conditions I to IV.
Furthermore, a light-emitting device (a light-emitting element) not realizing favorable color appearance more preferably becomes a light-emitting device capable of realizing favorable color appearance due to a control element when the following conditions are satisfied.
In other words, with the light-emitting device, more preferably, light having Φelm3(λ) does not satisfy Condition 5 described below but light having φSSL3(λ) satisfies Condition 5 described below.
In the spectral power distribution φ(λ) of object light, a wavelength λBM-max that provides φBM-max satisfies
430(nm)≤λBM-max≤480(nm).
In this case, with the light-emitting device, further preferably, light having Φelm3(λ) satisfies at least one of Conditions 6 to 8 described below but if there are conditions not satisfied by light having Φelm3(λ) among the Conditions 6 to 8 described below, light having φSSL3(λ) satisfies at least one of such conditions.
Moreover, in this case, the light-emitting device may be configured such that light having Φelm3(λ) satisfies at least one of Conditions 6 to 8 described below and light having φSSL3(λ) satisfies the same condition as satisfied by light having Φelm3(λ).
The spectral power distribution φ(λ) of object light satisfies
0.1800≤φBG-min/φRM-max≤0.8500.
A luminous efficacy of radiation K (lm/W) in a wavelength range of 380 nm to 780 nm derived from a spectral power distribution φ(λ) of object light satisfies
210.0lm/W≤K≤290.0lm/W.
A correlated color temperature T (K) of object light satisfies
2600K≤T≤7700K.
In addition, with the light-emitting device, more preferably, light having Φelm3(λ) does not satisfy Condition 6 described below but light having φSSL3(λ) satisfies Condition 6 described below.
The spectral power distribution φ(λ) of object light satisfies
0.1800≤φBG-min/φRM-max≤0.8500.
In addition, in Condition 6 described above, the light-emitting device further preferably satisfies
0.1917≤φBG-min/φRM-max≤0.7300.
In this case, with the light-emitting device, further preferably, light having Φelm3(λ) satisfies at least one of Conditions 5, 7 and 8 described below but if there are conditions not satisfied by light having Φelm3(λ) among the Conditions 5, 7 and 8 described below, light having φSSL3(λ) satisfies at least one of such conditions.
Moreover, in this case, the light-emitting device may be configured such that light having Φelm3(λ) satisfies at least one of Conditions 5, 7 and 8 described below and light having φSSL3(λ) satisfies the same condition as satisfied by light having Φelm3(λ).
In the spectral power distribution φ(λ) of object light, a wavelength λBM-max that provides φBM-max satisfies
430(nm)≤λRM-max≤480(nm).
A luminous efficacy of radiation K (lm/W) in a wavelength range of 380 nm to 780 nm derived from a spectral power distribution φ(λ) of object light satisfies
210.0lm/W≤K≤290.0lm/W.
A correlated color temperature T (K) of object light satisfies
2600K≤T≤7700K.
In addition, with the light-emitting device, more preferably, light having Φelm3(λ) does not satisfy Condition 7 described below but light having φSSL3(λ) satisfies Condition 7 described below.
A luminous efficacy of radiation K (lm/W) in a wavelength range of 380 nm to 780 nm derived from a spectral power distribution φ(λ) of object light satisfies
210.0lm/W≤K≤290.0lm/W.
In this case, with the light-emitting device, further preferably, light having Φelm3(λ) satisfies at least one of Conditions 5, 6 and 8 described below but if there are conditions not satisfied by light having Φelm3(λ) among the Conditions 5, 6 and 8 described below, light having φSSL3(λ) satisfies at least one of such conditions.
Moreover, in this case, the light-emitting device may be configured such that light having Φelm3(λ) satisfies at least one of Conditions 5, 6 and 8 described below and light having φSSL3(λ) satisfies the same condition as satisfied by light having Φelm3(λ).
In the spectral power distribution φ(λ) of object light, a wavelength λBM-max that provides φBM-max satisfies
430(nm)≤λRM-max≤480(nm).
The spectral power distribution φ(λ) of object light satisfies
0.1800≤φBG-min/φRM-max≤0.8500.
A correlated color temperature T (K) of object light satisfies
2600K≤T≤7700K.
In addition, with the light-emitting device, more preferably, light having Φelm3(λ) does not satisfy Condition 8 described below but light having φSSL3(λ) satisfies Condition 8 described below.
A correlated color temperature T (K) of object light satisfies
2600K≤T≤7700K.
In this case, with the light-emitting device, further preferably, light having Φelm3(λ) satisfies at least one of Conditions 5 to 7 described below but if there are conditions not satisfied by light having Φelm3(λ) among the Conditions 5 to 7 described below, light having φSSL3(λ) satisfies at least one of such conditions.
Moreover, in this case, the light-emitting device may be configured such that light having Φelm3(λ) satisfies at least one of Conditions 5 to 7 described below and light having φSSL3(λ) satisfies the same condition as satisfied by light having Φelm3(λ).
In the spectral power distribution φ(λ) of object light, a wavelength λBM-max that provides φBM-max satisfies
430(nm)≤λRM-max≤480(nm).
The spectral power distribution φ(λ) of object light satisfies
0.1800≤φBG-min/φRM-max≤0.8500.
A luminous efficacy of radiation K (lm/W) in a wavelength range of 380 nm to 780 nm derived from a spectral power distribution φ(λ) of object light satisfies
210.0lm/W≤K≤290.0lm/W.
Furthermore, a light-emitting device (a light-emitting element) realizing favorable color appearance preferably becomes a light-emitting device capable of realizing further favorable color appearance due to a control element when the following conditions are satisfied.
In other words, with the light-emitting device, still further preferably, light having Φelm3(λ) satisfies all of the Conditions 5 to 8 described below and light having φSSL3(λ) also satisfies all of the Conditions 5 to 8 described below.
In the spectral power distribution φ(λ) of object light, a wavelength λBM-max that provides φBM-max satisfies
430(nm)≤λRM-max≤480(nm).
The spectral power distribution φ(λ) of object light satisfies
0.1800≤φBG-min/φRM-max≤0.8500.
A luminous efficacy of radiation K (lm/W) in a wavelength range of 380 nm to 780 nm derived from a spectral power distribution φ(λ) of object light satisfies
210.0lm/W≤K≤290.0lm/W.
A correlated color temperature T (K) of object light satisfies
2600K≤T≤7700K.
On the other hand, the method for manufacturing the light-emitting device according to the fifth aspect of the third invention of the present invention can be derived from the above mentioned experiment results.
In other words, this is a method for manufacturing a light-emitting device having a light-emitting element and a control element, the manufacturing method comprising: a step of preparing a first light-emitting device at least having a blue semiconductor light-emitting element, a green phosphor and a red phosphor, as the light-emitting element; and a step of manufacturing a second light-emitting device by disposing the control element so that at least a part of the light emitted from the first light-emitting device in the main radiant direction transmits through, and when λ (nm) is a wavelength, Φelm3(λ) is a spectral power distribution of a light emitted from the first light-emitting device in the main radiant direction, and φSSL3(λ) is a spectral power distribution of a light emitted from the second light-emitting device in the main radiant direction, light having Φelm3(λ) does not satisfy at least one of the above mentioned Conditions 1 to 4, and φSSL3(λ) satisfies all of the above mentioned Conditions 1 to 4.
Particularly, manufacturing the light-emitting device that can implement a good appearance of colors according to the fifth aspect of the third invention of the present invention, by executing a step of disposing a specific control element in an LED lighting device which is already on the market and does not implement a good appearance of colors, is within the technical scope of the fifth aspect of the third invention of the present invention.
In addiotion, this is a method for manufacturing a light-emitting device having a light-emitting element and a control element, the manufacturing method comprising: a step of preparing a first light-emitting device at least having a blue semiconductor light-emitting element, a green phosphor and a red phosphor, as the light-emitting element; and a step of manufacturing a second light-emitting device by disposing the control element so that at least a part of the light emitted from the first light-emitting device in the main radiant direction transmits through, and when λ (nm) is a wavelength, Φelm3(λ) is a spectral power distribution of a light emitted from the first light-emitting device in the main radiant direction, and φSSL3(λ) is a spectral power distribution of a light emitted from the second light-emitting device in the main radiant direction, light having Φelm3(λ) satisfies all of the above mentioned Conditions 1 to 4, and φSSL3(λ) also satisfies all of the above mentioned Conditions 1 to 4.
In addition, the method for designing the light-emitting device according to the second aspect of the third invention of the present invention can be derived from the above mentioned experiment results.
In other words, a method for designing a light-emitting device having a light-emitting element and a control element, the light-emitting device at least including, as the light-emitting element, a blue semiconductor light-emitting element, a green phosphor, and a red phosphor, wherein the method for designing involves designing the light-emitting device so that when λ (nm) denotes wavelength, Φelm3(λ) denotes a spectral power distribution of light emitted from the light-emitting element in a main radiant direction, and φSSL3(λ) denotes a spectral power distribution of light emitted from the light-emitting device in the main radiant direction, light having Φelm3(λ) does not satisfy at least one of Conditions 1 to 4 described above but light having φSSL3(λ) satisfies all of the Conditions 1 to 4 described above.
In addition, a method for designing a light-emitting device having a light-emitting element and a control element, the light-emitting device at least including, as the light-emitting element, a blue semiconductor light-emitting element, a green phosphor, and a red phosphor, wherein the method for designing involves designing the light-emitting device so that when λ(nm) denotes wavelength, Φelm3(λ) denotes a spectral power distribution of light emitted from the light-emitting element in a main radiant direction, and φSSL3(λ) denotes a spectral power distribution of light emitted from the light-emitting device in the main radiant direction, light having Φelm3(λ) satisfies all of the Conditions 1 to 4 described above and light having φSSL3(λ) also satisfies all of the Conditions 1 to 4 described above.
Further, the illumination method according to the fourth aspect of the third invention of the present invention can be derived from the above mentioned experiment results in the same manner.
In other words, an illumination method comprising an illuminated object preparing step of preparing an illuminated object and an illuminating step of illuminating an object by light emitted from a light-emitting device having a semiconductor light-emitting element that is a light-emitting element and a control element, wherein the light-emitting device at least includes, as the light-emitting element, a blue semiconductor light-emitting element, a green phosphor, and a red phosphor, and in the illuminating step, when light emitted from the light-emitting element illuminates the object, light measured at a position of the object does not satisfy at least one of <1> to <4> described below, and when light emitted from the light-emitting device illuminates the object, light measured at a position of the object satisfies all of <1> to <4> described below.
The conditions <1> to <4> are the conditions derived from the above mentioned experimental examples.
<1>
When a*n and b*n (where n is a natural number from 1 to 15) respectively denote the a* value and the b* value in the CIE 1976 L*a*b* color space of the following 15 Munsell renotation color samples of #01 to #15 based on a mathematical assumption that illumination is performed by light emitted from the light-emitting device as measured at a position of the object, and
when a*nref and b*nref (where n is a natural number from 1 to 15) respectively denote the a* value and the b* value in the CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples based on a mathematical assumption that illumination is performed by reference light which is selected in accordance with a correlated color temperature T(K) of light emitted from the light-emitting device as measured at a position of the object, each saturation difference ΔCn satisfies
−4.00≤ΔCn≤8.00 (where n is a natural number from 1 to 15);
<2>
an average saturation difference represented by the following formula (3-3) satisfies
<3>
when a maximum saturation difference value is denoted by ΔCmax and a minimum saturation difference value is denoted by ΔCmin, a difference |ΔCmax−ΔCmin| between the maximum saturation difference value and the minimum saturation difference value satisfies
2.00≤|ΔCmax−ΔCmin|≤10.00,
where ΔCn=√{(a*n)2+(b*n)2}−√{(a*nref)2+(b*nref)2},
with the 15 Munsell renotation color samples being:
<4>
When θn (degrees) (where n is a natural number from 1 to 15) denotes a hue angle in the CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples based on a mathematical assumption that illumination is performed by the light emitted from the light-emitting device as measured at a position of the object, and
when θnref (degrees) (where n is a natural number from 1 to 15) denotes a hue angle in the CIE 1976 L*a*b* color space of the 15 Munsell renotation color samples based on a mathematical assumption that illumination is performed by reference light which is selected in accordance with the correlated color temperature T of the light emitted from the light-emitting device as measured at a position of the object, an absolute value of each difference in hue angles |Δhn| satisfies
0.00 degree≤|Δhn|≤12.50 degrees (where n is a natural number from 1 to 15),
where Δhn=θn−θnref.
In addition, a mode is preferable in which light emitted from a light-emitting device satisfies all of <5> to <8>. Moreover, <5> to <8> are also conditions derived from the experimental examples described earlier.
<5>
When λ denotes wavelength, φ(λ) denotes a spectral power distribution of light emitted from the light-emitting device as measured at a position of the object,
φref(λ) denotes a spectral power distribution of reference light which is selected in accordance with a correlated color temperature T of the light emitted from the light-emitting device as measured at a position of the object,
(X, Y, Z) denote tristimulus values of the light emitted from the light-emitting device as measured at a position of the object,
(Xref, Yref, Zref) denote tristimulus values of reference light which is selected in accordance with T of the light emitted from the light-emitting device as measured at a position of the object,
a normalized spectral power distribution S(λ) of the light emitted from the light-emitting device as measured at a position of the object, a normalized spectral power distribution Sref(λ) of reference light which is selected in accordance with T(K) of the light emitted from the light-emitting device as measured at a position of the object, and a difference ΔS(λ) of between normalized spectral power distributions are respectively defined as
S(λ)=φ(λ)/Y,
S
ref(λ)=φref(λ)/Yref,
ΔS(λ)=Sref(λ)−S(λ), and
in a case where λRL-max (nm) represents a wavelength that provides a longest wavelength local maximum value of S(λ) in a wavelength range of 380 nm or more and 780 nm or less, and when a wavelength Λ4 that is represented by S(λRL-max)/2 exists on a longer wavelength-side of λRL-max,
an index Acg represented by the following formula (3-1) satisfies
−10.0<Acg≤120.0,
but in a case where λRL-max (nm) represents a wavelength that provides the longest wavelength local maximum value of S(λ) in a wavelength range of 380 nm or more and 780 nm or less, and when the wavelength Λ4 that is represented by S(λRL-max)/2 does not exist on the longer wavelength side of λRL-max,
an index Acg represented by the following formula (3-2) satisfies
−10.0<Acg≤120.0,
[Expression 64]
A
cg=∫380495ΔS(λ)dλ+∫495590(−ΔS(λ))dλ+∫590Λ4ΔS(λ)dλ (3-1)
[Expression 65]
A
cg=∫380495ΔS(λ)dλ+∫495590(−ΔS(λ))dλ+∫590780ΔS(λ)dλ (3-2)
<6>
a distance Duv of the spectral power distribution φ(λ) of light from a black-body radiation locus defined by ANSI C78.377 satisfies
−0.0220≤Duv≤−0.0070;
<7>
when a maximum value of spectral intensity in a range of 430 nm or more and 495 nm or less is defined as φBM-max and a minimum value of spectral intensity in a range of 465 nm or more and 525 nm or less is defined as φBG-min, the spectral power distribution φ(λ) of light satisfies
0.2250≤φBG-min/φBM-max≤0.7000; and
<8>
in the spectral power distribution φ(λ) of light, when a maximum value of spectral intensity in a range of 590 nm or more and 780 nm or less is defined as φRM-max, a wavelength λRM-max that provides φRM-max satisfies
605(nm)≤λRM-max≤653(nm).
In addition, an illumination method comprising an illuminated object preparing step of preparing an illuminated object and an illuminating step of illuminating an object by light emitted from a light-emitting device having a semiconductor light-emitting element that is a light-emitting element and a control element, wherein the light-emitting device at least includes, as the light-emitting element, a blue semiconductor light-emitting element, a green phosphor, and a red phosphor, and in the illuminating step, when light emitted from the light-emitting element illuminates the object, light measured at a position of the object satisfies all of <1> to <4> described below, and when light emitted from the light-emitting device illuminates the object, light measured at a position of the object also satisfies all of <1> to <4> described below.
In addition, a mode is preferable in which light emitted from a light-emitting device satisfies <5> to <8>.
While a favorable embodiment for implementing the light-emitting device, the method for manufacturing the light-emitting device, the method for designing the light-emitting device and the illumination method according to the third invention of the present invention will be described below, it is to be understood that modes for implementing the light-emitting device, the method for manufacturing the light-emitting device, the method for designing the light-emitting device and the illumination method according to the third invention of the present invention are not limited to those used in the following description.
With the light-emitting device, the method for manufacturing the light-emitting device and the method for designing the light-emitting device according to the third invention of the present invention, no restrictions are placed on configurations, materials, and the like of the light-emitting device as long as a radiometric property and a photometric property of test light which is irradiated from the light-emitting device in a main radiant direction and which becomes a color stimulus with respect to an illuminated object are in appropriate ranges.
In the illumination method according to the third invention of the present invention, no restrictions are placed on configurations, materials, and the like of the light-emitting device as long as a photometric property of test light which is irradiated on an illuminated object and which becomes a color stimulus is in an appropriate range and, at the same time, a difference between color appearances of the 15 color samples when illumination by calculational reference light is assumed and color appearances of the 15 color samples when illumination by an actually measured test light spectral power distribution is assumed is in an appropriate range.
A light-emitting device for implementing the light-emitting device, the method for manufacturing the light-emitting device, the method for designing the light-emitting device or the illumination method according to the third invention of the present invention such as an illumination light source, a lighting fixture including the illumination light source, or a lighting system including the illumination light source or the lighting fixture includes at least a light-emitting element and at least a control element. In addition, at least a blue semiconductor light-emitting element, a green phosphor, and a red phosphor are provided as light-emitting elements.
Moreover, when the various conditions described above are satisfied and the effect of a light-emitting device, a method for manufacturing a light-emitting device, a method for designing a light-emitting device, or an illumination method according to the third invention of the present invention is produced, illuminating light sources including semiconductor light-emitting elements may include, in addition to a blue semiconductor light-emitting element, for example, a plurality of semiconductor light-emitting elements of different types such as green and red in a single illuminating light source, a single illuminating light source may include a blue semiconductor light-emitting element, another single illuminating light source may include a green semiconductor light-emitting element, yet another single illuminating light source may include a red semiconductor light-emitting element, in which case these illuminating light sources may be integrated together with a filter, a lens, a reflecting mirror, a drive circuit, and the like in a lighting fixture to be provided in an illuminating system. Furthermore, in a case where one illumination light source is included in one lighting fixture and an individual semiconductor light-emitting element is incorporated in the illumination light source, even if the illumination method or the light-emitting device according to the third invention of the present invention cannot be implemented as an individual illumination light source or an individual lighting fixture, a lighting system may be configured such that light radiated as the lighting system satisfies desired characteristics at a position of an illuminated object due to additive color mixing with light from a different lighting fixture that exists in the lighting system or the lighting system may be configured such that light in a main radiant direction among light radiated as the lighting system satisfies desired characteristics. In any mode, light in a main radiant direction among light emitted from the light-emitting device or light as a color stimulus which is ultimately irradiated on an illuminated object need only satisfy appropriate conditions according to the third invention of the present invention.
Hereinafter, characteristics will be described which are favorably attained by the light-emitting device according to the first aspect of the third invention of the present invention, a light-emitting device for implementing the method for manufacturing the light-emitting device according to the fifth aspect of the third invention of the present invention, the method for designing the light-emitting device according to the second aspect of the third invention of the present invention and the illumination method according to the fourth aspect of the third invention of the present invention on the basis of satisfying the appropriate conditions described above.
In the light-emitting device according to the first aspect of the third invention of the present invention, it is favorable to use the light-emitting elements (light-emitting materials) heretofore described because the index Acg, the distance Duv, the value φBG-min/φRM-max, the wavelength λRM-max, and the like can be more readily set to desired values. Using the light-emitting elements described above is also favorable because ΔCn, SATave, |ΔCmax−ΔCmin| and |Δhn| which are related, when light is treated as a color stimulus, to a difference between color appearances of the 15 color samples when illumination by the light-emitting device is assumed and color appearances when illumination by calculational reference light is assumed can also be more readily set to desired values.
Various means are conceivable for lowering Duv from zero to set Duv to an appropriate negative value. For example, when a light-emitting device having one light-emitting element in each of the three wavelength ranges is assumed, an emission position of the light-emitting element in the short wavelength range can be moved toward a shorter wavelength side, an emission position of the light-emitting element in the long wavelength range can be moved toward a longer wavelength-side, an emission position of the light-emitting element in the intermediate wavelength range can be displaced from 555 nm. Furthermore, a relative emission intensity of the light-emitting element in the short wavelength range can be increased, a relative emission intensity of the light-emitting element in the long wavelength range can be increased, a relative emission intensity of the light-emitting element in the intermediate wavelength range can be decreased, or the like. In doing so, in order to vary Duv without varying the CCT, the emission position of the light-emitting element in the short wavelength range may be moved toward a shorter wavelength side and, at the same time, the emission position of the light-emitting element in the long wavelength range may be moved toward a longer wavelength-side, or the like. Moreover, operations opposite to those described above may be performed to vary Duv toward a positive side.
In addition, when a light-emitting device respectively having two light-emitting elements in each of the three wavelength ranges is assumed, Duv can be lowered by, for example, increasing a relative intensity of a light-emitting element on a relatively shorter wavelength side among the two light-emitting elements in the short wavelength range, increasing a relative intensity of a light-emitting element on a relatively longer wavelength-side among the two light-emitting elements in the long wavelength range, or the like. In doing so, in order to vary Duv without varying the CCT, the relative intensity of the light-emitting element on a relatively shorter wavelength side among the two light-emitting elements in the short wavelength range is increased and, at the same time, the relative intensity of the light-emitting element on a relatively longer wavelength-side among the two light-emitting elements in the long wavelength range is increased. Moreover, operations opposite to those described above may be performed to vary Duv toward a positive side.
Meanwhile, as means for varying |Δhn|, SATave, ΔCn, and |ΔCmax−ΔCmin| which are related to a difference between color appearances of the 15 color samples when illumination by the light-emitting device is assumed and color appearances when illumination by calculational reference light is assumed and, in particular, as means for increasing ΔCn, operations such as described below can be performed after adjusting an entire spectral power distribution so that Duv assumes a desired value. Operations which may be performed include replacing each light-emitting element with a material having a narrow full-width at half-maximum, forming a spectrum shape in which light-emitting elements are appropriately separated from each other, installing a filter that absorbs a desired wavelength in an illumination light source, a lighting fixture, or the like in order to form a concave and/or a convex shape in a spectrum of each light-emitting element, and additionally mounting a light-emitting element which performs emission at a narrower band in a light-emitting element.
In the first aspect of the third invention of the present invention, the control element is a passive element that itself has no amplifying function, and is not especially limited if the intensity modulation for each wavelength can be performed in an appropriate range on light that is emitted from a light-emitting element or a light-emitting device having relatively low level processing, in the main radiant direction, and can constitute a light-emitting device having high level processing. In the first aspect of the third invention of the present invention, this function may be expressed as an action of the control element on a light-emitting element. Examples of the control element according to the first aspect of the third invention of the present invention are passive devices, such as a reflection mirror, an optical filter and various types of optical lenses. The control element according to the first aspect of the third invention of the present invention may be an absorption material that is dispersed in the sealing material of the packaged LED, so as to perform intensity modulation for each wavelength in an appropriate range. However, a light-emitting element and a reflection mirror, an optical filter, an absorption material or the like that can perform intensity modulation, of which wavelength dependency is low, on the light emitted from a light-emitting device having relatively low level processing, are not included in the control element.
In the first aspect of the third invention of the present invention, the control element is for converting the spectral power distribution of the light emitted from the light-emitting element in the main radiation direction into a spectral power distribution of the light that satisfies all of Conditions 1 to 4 described above. Therefore the characteristics of the control element according to the first aspect of the third invention of the present invention depend on the spectral power distribution of the light emitted from the light-emitting element in the main radiant direction.
However, in some cases, certain characteristics of the light-emitting element are preferable to make a good appearance of colors of the light emitted from the light-emitting device to an even better appearance of colors.
In the first aspect of the third invention of the present invention, it is preferable that when Duv(Φelm3(λ)) denotes Duv derived from the spectral power distribution of the light emitted from the light-emitting element in the main radiant direction, and Duv(φSSL3(λ)) denotes Duv derived from the spectral power distribution of the light emitted from the light-emitting device in the main radiant direction, the control element satisfies Duv(φSSL3(λ))<Duv(Φelm3(λ)).
The above mentioned Condition 2 specifies that −0.0220≤Duv(φSSL3(λ))≤−0.0070 is satisfied. Duv in this range is a very small value compared with a common LED illumination which is already on the market. Therefore it is preferable that the control element according to the first aspect of the third invention of the present invention has a characteristic to decrease Duv of the spectral power distribution. However even if the control element according to the first aspect of the third invention of the present invention increase Duv, this is acceptable for certain if the light-emitting device satisfies Condition 2. For example, in the case of a light-emitting element with which appearance of colors becomes too strong (glaring), a good appearance of colors may be implemented by disposing a control element that increases Duv.
There are various means of decreasing Duv, from zero to an appropriate negative value as described above, but these means can also be used to select a suitable control element according to the third invention of the present invention. For example, a control element, that increases the relative emission intensity of the light-emitting element in a short wavelength region, increases the relative emission intensity of the light-emitting element in a long wavelength region, and decreases the relative emission intensity of the light-emitting element in an intermediate wavelength range, more specifically, a control element of which light transmittance is high in the short wavelength region and the long wavelength region, and of which light transmittance is low in the intermediate wavelength range can be selected. A control element that adds convex/concave portions to the spectral power distribution of the light emitted from the light-emitting element in the main direction, can also be selected. To change Duv in a positive side, an operation the opposite of the above mentioned operation can be performed.
In the third invention of the present invention, it is preferable that when Acg(Φelm3(λ)) denotes Acg derived from the spectral power distribution of the light emitted from the light-emitting element in the main radiant direction, and Acg(φSSL3(λ)) denotes Acg derived from the spectral power distribution of the light emitted from the light-emitting device in the main radiant direction, the control element satisfies Acg(φSSL3(λ))<Acg(Φelm3(λ)).
The above Condition 1 specifies that −10.0<Acg≤120.0 is satisfied. Acg in this range is a very small value compared with a common LED illumination which is already on the market. Therefore it is preferable that the control element according to the third invention of the present invention has a characteristic to decrease Acg. However even if the control element according to the third invention of the present invention increases Acg, it is acceptable for certain if the light-emitting device satisfies Condition 2. For example, in the case of a light-emitting element with which appearance of colors becomes too strong (glaring), a good appearance of colors may be implemented by disposing a control element that increases Acg.
In the first aspect of the third invention of the present invention, it is preferable that when SATave(Φelm3(λ)) denotes an average saturation difference derived from the spectral power distribution of the light emitted from the light-emitting element in the main radiant direction, and SATave(φSSL3(λ)) denotes an average saturation difference derived from the spectral power distribution of the light emitted from the light-emitting device in the main radiation direction, the control element satisfies SATave(Φelm3(λ))<SATave(φSSL3(λ)).
If the average saturation difference SATave increases within an appropriate range, appearance of colors becomes better, hence it is preferable that the control element according to the first aspect of the third invention of the present invention has a characteristic to increase SATave when the illumination by the spectral power distribution is mathematically assumed. However even if the control element according to the first aspect of the third invention of the present invention decreases SATave, a good appearance of colors may be implemented by disposing a control element that decreases SATave in the case of a light-emitting element with which appearance of colors becomes too strong (glaring).
In the first aspect of the third invention of the present invention, it is preferable that the control element absorbs or reflects light in the range of 380 nm≤λ (nm)≤780 nm.
In the first aspect of the third invention of the present invention, it is preferable that the control element includes a collection and/or diffusion function of light emitted from the light-emitting element, such as the function(s) of a concave lens, a convex lens and a Fresnel lens.
In the first aspect of the third invention of the present invention, it is preferable that the control element, which is often disposed close to the light-emitting element, is heat resistant. A control element that is heat resistant is, for example, a control element made of a heat resistant material, such as glass. In the control element according to the first aspect of the third invention of the present invention, a desired element may be doped and colored to implement desired reflection characteristics and transmission characteristics.
For the above mentioned control element according to the first aspect of the third invention of the present invention, an appropriate filter on the market that satisfies the requirements of the first aspect of the third invention of the present invention may be selected. A filter may be designed and fabricated such that the light emitted from the light-emitting device has a desired spectral power distribution.
For example, to fabricate a filter having a plurality of absorption peaks, a plurality of types of films having a characteristic to absorb a light in a certain wavelength region and films having a characteristic to absorb a light in other wavelength regions may be prepared, and a multilayer filter may be created by layering these films. Dielectric films may be stacked to create a multilayer film, so as to implement desired characteristics.
As described above, the first aspect of the third invention of the present invention discloses a method of implementing a light-emitting device with controlling secondary influence by light irradiation, even for illumination objects for which this secondary influence is of concern, while implementing a natural, vivid, highly visible and comfortable appearance of objects as if the objects are seen, in a high luminance environment exceeding 10000 lx, as outdoors, for various illumination objects having various hues, within a 5 lx to about 10000 lx luminous range. In particular, the first aspect of the third invention of the present invention provides respective hues with natural vividness and, at the same time, enables white objects to be perceived more whiter as compared to experimental reference light.
Especially the first aspect of the third invention of the present invention is an extremely practical technique to provide an illumination device that implements a good appearance of colors by a very simple method of disposing such a control element as a filter and reflection mirror, in an illumination device which is already on the market, and cannot implement a good appearance of colors.
In addition, the light-emitting device according to the first aspect of the third invention of the present invention is a light-emitting device in which means for producing a color appearance which is as natural, vivid, highly visible, and comfortable as perceived in a high-illuminance environment involve setting the index Acg, Duv, φBG-min/φBM-max, and λRM-max as obtained from a spectral power distribution of light emitted in a main radiant direction to within an appropriate range.
In other words, according to the first aspect of the third invention of the present invention, intensity modulation is performed on an appropriate wavelength in the light emitted from the light-emitting element using a control element, and the light emitted from the light-emitting device satisfies all of Conditions 1 to 4, and as long as this requirement is satisfied, the light-emitting device may have any configuration. For example, the device may be any of an individual illumination light source, an illuminating module in which at least one or more of the light sources is mounted on a heatsink or the like, and a lighting fixture in which a lens, a light-reflecting mechanism, a driving electric circuit, and the like are added to the light source or the module. Furthermore, the device may be a lighting system which is a collection of individual light sources, individual modules, individual fixtures, and the like and which at least has a mechanism for supporting such components.
Means according to the illumination method of the fourth aspect of the third invention of the present invention for producing a color appearance which is as natural, vivid, highly visible, and comfortable as perceived in a high-illuminance environment involve providing a light-emitting device setting Duv of light at a position of an illuminated object to within an appropriate range and, at the same time, setting indices related to a difference between color appearances of the 15 color samples when illumination by the light is assumed and color appearances when illumination by calculational reference light is assumed such as |Δhn|, SATave, ΔCn, and |ΔCmax−ΔCmin| to within appropriate ranges.
In other words, the illumination method according to the fourth aspect of the third invention of the present invention is an illumination method in which light emitted from a semiconductor light-emitting element is included in the spectral power distribution as a constituent element and, at the same time, the illumination method according to the fourth aspect of the third invention of the present invention is an illumination method of illuminating light in which |Δhn|, SATave, ΔCn, |ΔCmax−ΔCmin|, Duv, and the like are within appropriate ranges to an illuminated object, and a light-emitting device used in the illumination method according to the fourth aspect of the third invention of the present invention can be configured in any way as long as the device is capable of providing such illumination. For example, the device may be any of an individual illumination light source, an illuminating module in which at least one or more of the light sources is mounted on a heatsink or the like, and a lighting fixture in which a lens, a light-reflecting mechanism, a driving electric circuit, and the like are added to the light source or the module. Furthermore, the device may be a lighting system which is a collection of individual light sources, individual modules, individual fixtures, and the like and which at least has a mechanism for supporting such components.
In the third invention of the present invention, the metrological, photometric and colormetric characteristics of the light-emitting devices of the examples are shown in Table 3-16, Table 3-17 and Table 3-18, where appearance of colors of the illumination objects was generally very good.
The light-emitting device according to the first aspect of the third invention of the present invention is an illumination device that can implement a good appearance of colors for an illumination device that cannot implement a good appearance of colors, by using a very simple method of disposing such a control element as a filter and a reflection mirror in this illumination device, and also an illumination device that can implement a good appearance of colors suitable to the taste of the user, for an illumination device which is already capable of implementing a good appearance of colors, by using a very simple method of disposing such a control element as a filter and a reflection mirror in this illumination device.
The fifth aspect of the third invention of the present invention is a method for manufacturing a light-emitting device and the second aspect of the third invention of the present invention is a method for designing a light-emitting device. With a method for manufacturing and a method for designing according to these aspects of the third invention, a method for manufacturing and design guidelines for “a light-emitting device capable of realizing a natural, vivid, highly visible and comfortable appearance of colors or an appearance of objects” can be provided. In addition, the fourth aspect of the third invention of the present invention is an illumination method. With an illumination method according to the fourth aspect of the third invention of the present invention, “a natural, vivid, highly visible and comfortable appearance of colors or an appearance of objects” can be realized. All of the descriptions on the first aspect of the third invention of the present invention may be applied to the second, fourth, and fifth aspects of the third invention of the present invention.
<1. First Invention of Present Invention>
The light-emitting device according to the first invention of the present invention has an extremely wide field of application and may be used without being limited to particular uses. However, in consideration of the features of the light-emitting device according to the first invention of the present invention is favorably applied to the following fields.
For example, when illuminated by a light-emitting device according to the first invention of the present invention, white appears whiter, more natural, and more comfortable as compared to conventionally known light-emitting devices even with substantially similar CCT and substantially similar luminance. In addition, differences in lightness among achromatic colors such as white, gray, and black become more visible.
As a result, for example, black letters or the like on an ordinary sheet of white paper become more legible. To utilize such features, favorable applications include a reading light, lighting for a writing desk, and work lighting such as office lighting. In addition, work may conceivably involve performing a visual external examination of fine parts, distinguishing between near colors of cloth or the like, checking color in order to verify freshness of meat, performing a product inspection by comparing with a criteria sample, and the like at a factory or the like. In addition, illumination by the light-emitting device according to the first invention of the present invention makes color identification among close hues easier and realizes a work environment that is as comfortable as though in a high-illuminance environment. Even from such a perspective, applications to work lighting are favorable.
Furthermore, compared to the light-emitting devices disclosed in Japanese Patent No. 5252107 and Japanese Patent No. 5257538, illumination provided by a light-emitting device according to the first invention of the present invention results in high light source efficiency of the light-emitting device and emission of a larger luminous flux even when similar power is supplied. Therefore, the light-emitting device can be favorably used as a light-emitting device that illuminates an illuminated object from a higher ceiling surface than normal and an applicable range of the light-emitting device can be further expanded.
Furthermore, since color discrimination ability increases, for example, applications to medical lighting such as a light source for surgical operations and a light source used in a gastroscope or the like are also favorable. While arterial blood is vivid red due to its high oxygen content, venous blood is dark red due to its high carbon dioxide content. Although arterial blood and venous blood are both red, chromas of the colors differ from each other. Therefore, with the light-emitting device according to the first invention of the present invention which achieves favorable color appearance (chroma), it is expected that arterial blood and venous blood can be readily distinguished from each other. In addition, since it is obvious that favorable color representation in color image information such as an endoscope has a significant effect on diagnosis, it is expected that a normal location and a lesion location can be readily distinguished from each other. Due to similar reasons, the illumination method can be favorably applied to an illumination method used in industrial equipments such as a product image judgment device.
When illuminated by the light-emitting device according to the first invention of the present invention, a truly natural color appearance as though viewed under several tens of thousands of lx such as outdoor illuminance on a sunny day is achieved for a majority of, and in some cases, all colors such as purple, bluish purple, blue, greenish blue, green, yellowish green, yellow, reddish yellow, red, and reddish purple even when illuminance only ranges from around several thousand lx to several hundred lx. In addition, the skin color of the subjects (Japanese), various foods, clothing, wood colors, and the like which have intermediate chroma also acquire natural color appearances which many of the subjects feel more favorable.
Therefore, by applying the light-emitting device according to the first invention of the present invention to ordinary lighting for homes and the like, it is conceivable that food may appear fresher and more appetizing, newspapers, magazines, and the like may become more legible, and visibility of differences in level in the house may increase, thereby contributing to improving home safety. Accordingly, the light-emitting device according to the first invention of the present invention is favorably applied to residential uses' illumination. In addition, the present invention is also favorable as exhibit lighting for clothing, food, vehicles, suitcases, shoes, ornaments, furniture, and the like, and enables lighting which makes such items stand out from their surroundings. As described above, in particular, compared to the light-emitting devices disclosed in Japanese Patent No. 5252107 and Japanese Patent No. 5257538, illumination provided by a light-emitting device according to the first invention of the present invention results in higher light source efficiency of the light-emitting device and emission of a larger luminous flux even when similar power is supplied. Therefore, the light-emitting device can be favorably used as a light-emitting device that illuminates an illuminated object from a higher ceiling surface than normal. Due to such characteristics, a light-emitting device according to the first invention of the present invention is particularly preferably applied to illumination for exhibition.
Furthermore, the present invention is also favorable as lighting for goods such as cosmetics in which slight differences in color are the decisive factor when purchasing the goods. When used as exhibit lighting for white dresses and the like, since subtle differences in color become more visible such as a difference between bluish white and creamy white among similar whites, a person can select a color that is exactly according to his or her desire. Furthermore, the present invention is also favorable as presentation lighting at a wedding center, a theater, and the like, and enables a pure white dress or the like to be perceived as being pure white and kimonos, makeup, in kabuki or the like to appear vividly. The present invention also favorably highlights skin tones. In order to realize such illumination, since a light-emitting device according to the first invention of the present invention which has high light source efficiency is capable of providing illumination over a distance, a light-emitting device according to the first invention of the present invention is particularly preferably applied to illumination for presentation. In addition, by using the present invention as lighting in a hair salon, colors that are no different than those perceived outdoors can be obtained during hair coloring and excessive dyeing or insufficient dyeing can be prevented.
Furthermore, since white appears more white, achromatic colors can be readily distinguished, and chromatic colors attain their natural vividness, the first invention of the present invention are also favorable as a light source in a location where a wide variety of activities are conducted in a given limited space. For example, passengers in an airplane read, work, and eat at their seats. Similar situations take place on a train, a long-distance bus, and the like. The first invention of the present invention is favorably applicable as lighting for interior of transportation.
In addition, since white appears more white, achromatic colors can be readily distinguished, and chromatic colors attain their natural vividness, the first invention of the present invention enables paintings and the like in an art museum or the like to be illuminated in a natural tone as though viewed outdoors and is therefore also favorable as lighting for works of art.
On the other hand, the first invention of the present invention is also favorably applicable as lighting for aged persons. In other words, even in case where small characters are hard to read and difference in steps or the like are hard to see under normal illuminance, by applying the light-emitting device according to the first invention of the present invention, such problems can be solved since achromatic colors and chromatic colors can be readily distinguished from one another. Therefore, the first invention of the present invention is also favorably applicable to lighting in public facilities or the like which are used by the general public such as a waiting room in a retirement house or a hospital, a book store, and a library. While luminance itself must be increased in an appropriate range in order to realize such illumination, a light-emitting device according to the first invention of the present invention which has high light source efficiency is capable of increasing luminance of an illuminated surface even when supplied power is similar. Therefore, a light-emitting device according to the first invention of the present invention is particularly preferably applied to illumination for the aged persons.
Furthermore, the light-emitting device according to the first invention of the present invention can be favorably used in applications for securing visibility by adapting to an illumination environment in which illuminance is often at a relatively low level due to various circumstances.
For example, the light-emitting device according to the first invention of the present invention is favorably applied to street lamps, head lights of vehicles, and foot lamps to increase visibility as compared to using conventional light sources.
<2. Second Invention of Present Invention>
The description on the industrial applicability of the first invention of the present invention will also apply to the industrial applicability of the second invention of the present invention.
<3. Third Invention of Present Invention>
The light-emitting device such as an illumination light source, a lighting fixture, a lighting system, and the like, and the illumination method according to the third invention of the present invention has an extremely wide field of application and may be used without being limited to particular uses. However, in consideration of the features of the illumination method or the light-emitting device according to the third invention of the present invention, the illumination method or the light-emitting device according to the third invention of the present invention is favorably applied to the following fields.
For example, when illuminated by the light-emitting device or the illumination method according to the third invention of the present invention, white may be perceived as being whiter, more natural, and more comfortable as compared to a conventional a conventional light-emitting device or illumination method even at a similar CCT and a similar illuminance. Furthermore, differences in lightness among achromatic colors such as white, gray, and black become more visible.
As a result, for example, black letters or the like on an ordinary sheet of white paper become more legible. To utilize such features, favorable applications include a reading light, lighting for a writing desk, and work lighting such as office lighting. In addition, while work may conceivably involve performing a visual external examination of fine parts, distinguishing between near colors of cloth or the like, checking color in order to verify freshness of meat, performing a product inspection by comparing with a criteria sample, and the like at a factory or the like, illumination by the illumination method according to the third invention of the present invention makes color identification among close hues easier and realizes a work environment that is as comfortable as though in a high-illuminance environment. Even from such a perspective, applications to work lighting are favorable.
Furthermore, since color discrimination ability increases, for example, applications to medical lighting such as a light source for surgical operations and a light source used in a gastroscope or the like are also favorable. While arterial blood is vivid red due to its high oxygen content, venous blood is dark red due to its high carbon dioxide content. Although arterial blood and venous blood are both red, chromas of the colors differ from each other. Therefore, with the device or the illumination method according to the third invention of the present invention which achieves favorable color appearance (chroma), it is expected that arterial blood and venous blood can be readily distinguished from each other. In addition, since it is obvious that favorable color representation in color image information such as an endoscope has a significant effect on diagnosis, it is expected that a normal location and a lesion location can be readily distinguished from each other. Due to similar reasons, the illumination method can be favorably applied to an illumination method used in industrial equipments such as a product image judgment device.
When illuminated by the light-emitting device or the illumination method according to the third invention of the present invention, a truly natural color appearance as though viewed under several tens of thousands of lx such as outdoor illuminance on a sunny day is achieved for a majority of, and in some cases, all colors such as purple, bluish purple, blue, greenish blue, green, yellowish green, yellow, reddish yellow, red, and reddish purple even when illuminance only ranges from around several thousand lx to several hundred lx. In addition, the skin color of the subjects (Japanese), various foods, clothing, wood colors, and the like which have intermediate chroma also acquire natural color appearances which many of the subjects feel more favorable.
Therefore, by applying the light-emitting device or the illumination method according to the third invention of the present invention to ordinary lighting for homes and the like, it is conceivable that food may appear fresher and more appetizing, newspapers, magazines, and the like may become more legible, and visibility of differences in level in the house may increase, thereby contributing to improving home safety. Accordingly, the third invention of the present invention is favorably applied to residential uses' illumination. In addition, the present invention is also favorable as exhibit lighting for clothing, food, vehicles, suitcases, shoes, ornaments, furniture, and the like, and enables lighting which makes such items stand out from their surroundings.
The present invention is also favorable as lighting for goods such as cosmetics in which slight differences in color are the decisive factor when purchasing the goods. When used as exhibit lighting for white dresses and the like, since subtle differences in color become more visible such as a difference between bluish white and creamy white among similar whites, a person can select a color that is exactly according to his or her desire. Furthermore, the present invention is also favorable as presentation lighting at a wedding center, a theater, and the like, and enables a pure white dress or the like to be perceived as being pure white and kimonos, makeup, in kabuki or the like to appear vividly. The present invention also favorably highlights skin tones. In addition, by using the present invention as lighting in a hair salon, colors that are no different than those perceived outdoors can be obtained during hair coloring and excessive dyeing or insufficient dyeing can be prevented.
Furthermore, while a control element according to the third invention of the present invention has a function of improving color appearance and a function of adjusting color appearance in accordance with preferences of a user, the control element may additionally have a function of reducing relative spectral intensity of light with relatively high energy which may be irradiated from a light-emitting element such as a part of ultraviolet light, near-ultraviolet light, violet light, blue-violet light, and blue light. In such a case, for example, color degradation, alteration, corrosion, deterioration, and the like of illuminated objects such as clothing and food can be reduced. In addition, since a control element according to the third invention of the present invention is also capable of reducing relative spectral intensity of light from a light-emitting element with a wavelength that may potentially cause thermal radiation such as near infrared light, middle infrared light, and far infrared light, alteration, corrosion, deterioration, and the like of illuminated objects such as food can be reduced. Therefore, an effect of reducing alteration, corrosion, deterioration, and the like of illuminated objects such as food can also be provided.
Furthermore, since white appears more white, achromatic colors can be readily distinguished, and chromatic colors attain their natural vividness, the third invention of the present invention is also favorable as a light source in a location where a wide variety of activities are conducted in a given limited space. For example, passengers in an airplane read, work, and eat at their seats. Similar situations take place on a train, a long-distance bus, and the like. The third invention of the present invention is favorably applicable as lighting for interior of transportation.
In addition, since white appears more white, achromatic colors can be readily distinguished, and chromatic colors attain their natural vividness, the third invention of the present invention enables paintings and the like in an art museum or the like to be illuminated in a natural tone as though viewed outdoors and is therefore also favorable as lighting for works of art.
On the other hand, the third invention of the present invention is also favorably applicable as lighting for aged persons. In other words, even in case where small characters are hard to read and difference in steps or the like are hard to see under normal illuminance, by applying the illumination method or the light-emitting device according to the third invention of the present invention, such problems can be solved since achromatic colors and chromatic colors can be readily distinguished from one another. Therefore, the present invention is also favorably applicable to lighting in public facilities or the like which are used by the general public such as a waiting room in a retirement house or a hospital, a book store, and a library.
Furthermore, the light-emitting device or the illumination method according to the third invention of the present invention can be favorably used in applications for securing visibility by adapting to an illumination environment in which illuminance is often at a relatively low level due to various circumstances.
For example, the illumination method or the light-emitting device according to the third invention of the present invention is favorably applied to street lamps, head lights of vehicles, and foot lamps to increase visibility as compared to using conventional light sources.
While the invention has been described in detail and with reference to specific embodiments thereof, it will be apparent to one skilled in the art that various changes and modifications can be made therein without departing from the spirit and scope thereof.
| Number | Date | Country | Kind |
|---|---|---|---|
| 2013-272763 | Dec 2013 | JP | national |
| 2014-159784 | Aug 2014 | JP | national |
| 2014-178928 | Sep 2014 | JP | national |
| 2014-178941 | Sep 2014 | JP | national |
This is a divisional of U.S. application Ser. No. 15/191,734 filed Jun. 24, 2016, allowed and pending, which is a continuation of International Application PCT/JP2014/084487, filed on Dec. 26, 2014, and designated the U.S., and claims priority from Japanese Patent Application 2013-272763 which was filed on Dec. 27, 2013, Japanese Patent Application 2014-159784 which was filed on Aug. 5, 2014, Japanese Patent Application 2014-178928 which was filed on Sep. 3, 2014, and Japanese Patent Application 2014-178941 which was filed on Sep. 3, 2014, the entire contents of which are incorporated herein by reference.
| Number | Date | Country | |
|---|---|---|---|
| Parent | 15191734 | Jun 2016 | US |
| Child | 17815223 | US |
| Number | Date | Country | |
|---|---|---|---|
| Parent | PCT/JP2014/084487 | Dec 2014 | US |
| Child | 15191734 | US |
