Patent Application
20200166197
The present invention relates to a light source unit including a phosphor, which converts a laser beam emitted from a pump light source into emitted light, and a retro-reflector, which has an output aperture that allows emission of part of the emitted light obtained after being converted by the phosphor and which reflects another part of the emitted light to a light converter layer.
A light source unit including a laser pump light source, a phosphor, and a dome-shaped retro-reflector is known (PTL 1). This light source unit includes a laser pump light source, which emits laser pump light, a phosphor, which converts the laser pump light into wavelength-converted light (fluorescence), and a retro-reflector, which is joined to the phosphor and has an output aperture that allows emission of part of the wavelength-converted light (fluorescence). The retro-reflector reflects another part of the wavelength-converted light (fluorescence) back to the phosphor.
However, the light source unit described in PTL 1 has the following problem.
The phosphor included in the light source unit typically emits emitted light in Lambertian angular distribution, and is generally composed of particles (for example, cerium-doped yttrium aluminum garnet (YAG)) that absorb blue light and emit a broad wavelength range of wavelength-converted light from green to red. These particles not only absorb blue light hitting those particles but also scatter the light. Specifically, when the phosphor is irradiated with a blue laser beam, a broad wavelength range of light from green to red, which is wavelength-converted light, is mixed with the scattered blue laser beam, so that white light is emitted.
To emit light in Lambertian angular distribution, large optics are required to highly efficiently use the light. To highly efficiently use the emitted light with small optics, a pump light source that emits light at a smaller angle than the Lambertian distribution is preferable.
A retro-reflector with an output aperture of an angle 2α functions to return the wavelength-converted light back and the laser beam scattered by the phosphor at an angle larger than 2α again onto the phosphor. The laser beam and wavelength-converted light returned to the phosphor are again absorbed or scattered by the phosphor and re-emitted from the phosphor.
White light reflected off the retro-reflector is incident again on the phosphor at an angle within the range of 0 degrees to 90 degrees, and is re-emitted from the phosphor as white light in Lambertian distribution.
The inventors have found that white light (mixture of scattered laser beam and wavelength-converted light) emitted when the phosphor is excited by a laser beam in a structure not including a retro-reflector has a colour temperature different from that of white light emitted when the phosphor is excited by a laser beam in a structure including a retro-reflector. White light emitted when the phosphor is excited by a laser beam in a structure including a retro-reflector has a lower colour temperature (that is, the light exhibits a red shift in color). This shift of the colour temperature to a lower colour temperature in a structure including the retro-reflector is not desirable in the application of the light source unit to, for example, car headlights.
This shift of the colour temperature to a lower colour temperature in a structure including the retro-reflector is dependent on the dimension (angle 2α) of the output aperture of the retro-reflector. This is because the output aperture having a smaller size allows more white light to be reflected by the retro-reflector, so that more blue light is absorbed by the phosphor.
Use of the retro-reflector changes the colour temperature of white obtained by mixing the scattered laser beam and the wavelength-converted light from the colour temperature of white emitted from a structure not including the retro-reflector. White light reflected by the retro-reflector is directed again onto the phosphor, and components of the scattered laser beam in the white light are absorbed again by the phosphor to form wavelength-converted light. On the other hand, components of the wavelength-converted light in the white light that have been returned to the phosphor are scattered again or absorbed without being subjected to wavelength conversion again. Thus, it is assumed that, every time white light is returned to the phosphor by being reflected by the retro-reflector, components of blue-color wavelength corresponding to the scattered laser beam are deducted from the white light, so that the colour temperature gradually decreases.
PTL 1 describes a change of the characteristics of a dome-shaped retro-reflector and the wavelength of laser pump light to solve the above problem.
However, associating the wavelength of the laser pump light with the characteristics of the retro-reflector causes inconvenience in color mixture, and reducing the wavelength of the laser pump light degrades the system efficiency.
An aspect of the present invention is to provide a light source unit that includes a retro-reflector and that is capable of emitting preferable white light.
(1) An embodiment of the present invention is a light source unit that includes a pump light source that emits a laser beam; a phosphor that converts the laser beam emitted from the pump light source into converted light; and a retro-reflector that has an output aperture, which allows emission of part of the converted light converted by the phosphor as emitted light, the retro-reflector reflecting another part of the converted light back to the phosphor as retro-reflection light. The phosphor includes a blue-light-ratio increasing member, which increases the blue light ratio of the converted light.
(2) An embodiment of the present invention provides a light source unit having the structure described in the paragraph (1), in which the blue-light-ratio increasing member is scattering particles included in the phosphor to diffusely reflect or scatter the laser beam emitted from the pump light source.
(3) An embodiment of the present invention provides a light source unit having the structure described in the paragraph (1), in which the scattering particles are formed from a high thermal conductivity material to improve the thermal properties of the phosphor.
(4) An embodiment of the present invention provides a light source unit having the structure described in the paragraph (1), in which the blue-light-ratio increasing member is the phosphor having a particle density adjusted in accordance with a size of an output aperture of the retro-reflector.
(5) An embodiment of the present invention provides a light source unit having the structure described in the paragraph (1), in which the blue-light-ratio increasing member is a scattering layer disposed on a surface of the light converter layer facing the pump light source to diffusely reflect or scatter the laser beam emitted from the pump light source.
(6) An embodiment of the present invention provides a light source unit having the structure described in the paragraph (1), in which the blue-light-ratio increasing member is scattering particles disposed on a surface of the phosphor facing the pump light source to diffusely reflect or scatter the laser beam emitted from the pump light source.
(7) An embodiment of the present invention provides a light source unit having the structure described in the paragraph (1), that further includes a substrate that supports the phosphor, and in which the blue-light-ratio increasing member is constituted of a combination the substrate and the phosphor into a geometric pattern.
(8) An embodiment of the present invention provides a light source unit and having the structure described in the paragraph (1), in which a desired colour temperature of the emitted light is greater than or equal to 2000 K and smaller than or equal to 10000 K.
(9) An embodiment of the present invention provides a light source unit having the structure described in the paragraph (1), in which the retro-reflector has a hollow dome shape or a flat plate shape.
(10) An embodiment of the present invention provides a light source unit having the structure described in the paragraph (1), in which the retro-reflector is coupled to the phosphor directly or via an intermediate layer.
(11) An embodiment of the present invention provides a light source unit having the structure described in the paragraph (1), in which the blue light ratio increased by the blue-light-ratio increasing member is determined by a formula relating to the desired colour temperature and the size of the output aperture.
(12) An embodiment of the present invention provides a light source unit having the structure described in the paragraph (1), that further includes a different pump light source that emits a different laser beam, and in which the phosphor converts the laser beam emitted from the pump light source and the different laser beam emitted from the different pump light source into the emitted light.
An aspect of the present invention provides a light source unit including a retro-reflector and capable of emitting preferable white light.
Embodiments of the present invention will be described in detail, below. To solve the above problem, embodiments of the present invention each provide a structure that controls the colour temperature of white emitted light emitted from a structure including a retro-reflector to a desired colour temperature. Thus, the colour temperature of white light emitted from the phosphor itself (emitted without using a retro-reflector) is intentionally increased to solve the problem. A light source unit according to one embodiment may include a substrate and a wavelength converter that includes a phosphor formed from multiple different materials, and the phosphor may have a coating applied to its surface.
The phosphor according to any of embodiments of the present application emits white light having a high colour temperature, which is a blue colour temperature, when used without a retro-reflector. White light having a high colour temperature without a retro-reflector can be obtained by improving the internal structure of the phosphor, additionally disposing, on the upper surface of the phosphor, a structure that further scatters a blue laser beam, or by changing the geometric shape of the substrate.
Thus, the blue component of the finally emitted light obtained when a retro-reflector is used can be increased.
The phosphor 3 is supported by a substrate 10. The substrate 10 and the phosphor 3 constitute a converter 14.
The retro-reflector 4 has a coupling aperture 15, which guides the laser pump light 11 emitted from the pump light source 2 to the phosphor 3.
The pump light source 2 includes a laser diode that emits the laser pump light 11, and a lens disposed between a laser diode and the coupling aperture 15 of the retro-reflector 4 to further collimate and/or condense the laser pump light 11. The lens may change the light intensity distribution of the laser pump light 11.
The phosphor 3 is mounted on the substrate 10, and preferably formed from, for example, YAG and a binder (binding member) as a material. The substrate 10 may be preferably formed from aluminium, copper, ceramics, or other materials having high thermal conductivity.
The retro-reflector 4 has a hollow dome shape, and has a highly reflective inner peripheral surface. The retro-reflector 4 may be formed from a glass that transmits visible light, BK7, or other materials. In this example, the retro-reflector 4 may be mounted in contact with the phosphor 3. The phosphor 3 may have high thermal conductivity. A gap may be left between the phosphor 3 and an end surface of the hollow dome-shaped retro-reflector 4 facing the phosphor 3.
The coupling aperture 15 may have any shape. The coupling aperture 15 needs to have a size greater than the size of the laser pump light 11 not to interfere with the optical path of the laser pump light 11.
The output aperture 5 preferably has a circular shape, but may have any of other shapes including a square or rectangular shape.
The laser pump light 11 has a peak emission wavelength shorter than the peak emission wavelength of fluorescence emitted from the phosphor 3. A general application of the light source unit 1 is an illumination that emits white light. The phosphor 3 is made of YAG or other wavelength converting materials with similar properties, and the peak emission wavelength of the laser pump light 11 is preferably on or around 450 nm.
The scattering particles 7 are added to the phosphor 3 to scatter the blue laser pump light 11.
In the embodiment illustrated in
The scattering particles 7 may include different materials, such as, Al2O3, diamond, and TiO2. The scattering particles 7 are made of a material having very low absorption of the light in the visible range. The scattering particles 7 may be made of high thermal conductivity materials to improve the thermal properties of the phosphor 3.
A problem usually occurs when the scattering particles 7 are used alone without the retro-reflector. This is because the scattering particles 7 decrease the wavelength conversion efficiency of the phosphor 3, increase the size of the emission spot of the phosphor 3, and worsen the color mixing. However, when the retro-reflector 4 and the scattering particles 7 are used in combination, these problems can be partially or completely suppressed. Thanks to the recycling of the white light 12 due to reflection at the inner peripheral surface of the retro-reflector 4, the color homogeneity will be improved and the excessive absorption of the blue light will be decreased, so that a desired colour temperature can be obtained.
The laser pump light 11 emitted from the pump light source 2 passes through the coupling aperture 15 to the inside of the retro-reflector 4 to be incident on the phosphor 3. Part of the white light 12, which is the mixture of a scattered laser beam emitted from the phosphor 3 and fluorescence, is emitted through the output aperture 5 of the retro-reflector 4 as the emitted light 13, and another part is reflected off the inner peripheral surface of the retro-reflector 4 back to the phosphor 3 as retro-reflection light. The reflected retro-reflection light can be scattered by the phosphor 3 to be added to the emitted light 13 and directed to the output aperture 5. This can be said as a basic structure used to reduce an etendue of the pump light source 2.
This white light 12 has a problem on the colour temperature. The white light 12 is formed from the laser pump light 11 and the converted light converted by the phosphor 3. When the white light 12 hits the phosphor 3 as retro-reflection light reflected by the retro-reflector 4, the retro-reflection light is absorbed or scattered by the phosphor 3, and is partially subjected to wavelength conversion.
However, when the retro-reflection light reflected by the retro-reflector 4 hits the phosphor 3, the blue light component contained in the retro-reflection light is absorbed by the phosphor 3, and the retro-reflection light has its wavelength converted and is then added to the emitted light 13 emitted through the output aperture 5. Thus, the emitted light 13 emitted through the output aperture 5 becomes more yellowish (colour temperature decreases). The more cycles of the white light 12 reflected off the inner peripheral surface of the retro-reflector 4 and returned to the phosphor 3 as retro-reflection light take place, the more yellow the emitted light 13 emitted through the output aperture 5 becomes. The emitted light 13 becomes more yellowish as the size of the output aperture 5 decreases.
To solve this problem, the present invention proposes to increase the ratio of the laser pump light 11 converted to the white light 12 after the laser pump light 11 has hit the phosphor 3, and to have the phosphor 3 that emits more blueish light with reduction of the blue light absorption of the phosphor 3 to keep preferable wavelength conversion efficiency. In other words, the white light 12 inside the retro-reflector 4 is adjusted to emit white light having a higher colour temperature than the light emitted by only the phosphor 3 without the retro-reflector 4. Thus, a colour temperature shift due to the increase of the blue light absorption of the phosphor 3 in the recycling of the white light 12 due to reflection at the inner peripheral surface of the retro-reflector 4 is compensated.
In the present embodiment, the blue light component in the white light 12 is increased by modifying the internal structure of the phosphor 3.
When the white light 12 is reflected between the phosphor 3 and the retro-reflector 4 to be returned to the phosphor 3, the phosphor 3 absorbs blue light, but does not absorb yellow light. As the number of reflection increases, the more yellowish emitted light 13 is emitted through the output aperture 5 of the retro-reflector 4.
The colour temperature (CCT) of the emitted light 13 emitted through the output aperture 5 decreases as the number of reflection increases, as illustrated in
When an angle α, representing the size of the output aperture 5 of the retro-reflector 4, is changed, the chromaticity coordinates (x, y) and the final colour temperature (CCT) of the emitted light 13 emitted through the output aperture 5 are changed. As the angle α of the output aperture 5 becomes smaller, the colour temperature (CCT) of the emitted light 13 from the output aperture 5 further decreases, as illustrated in
With reference to
All the curves in
CCTwr(α)=Y0+A1eBYR/t1+A2eBYR/t2 (Formula 1)
Here, factors Y0, A1, t1, A2, and t2 are dependent on the angle α of the output aperture 5 of the retro-reflector 4. BYR is a ratio between the blue light part and the yellow light part of the spectra of the white light 12 from the phosphor 3.
The above expression (Formula 1) can be used to calculate the colour temperature (CCT) finally obtained after the infinite number of times of retro-reflection at each BYR and each angle α. The expression (Formula 1) is derived from the fitting resulting from a simulation. The expression (Formula 1) is useful in that it can estimate the colour temperature of white light that can be obtained when structure parameters (including BYR and α) are found.
The horizontal axis represents the blue-yellow ratio (BYR, or blue light ratio), and the vertical axis represents the colour temperature (CCT) when the retro-reflector 4 is provided.
To obtain the colour temperature (CCT) of BYR=1 for each angle α of the output aperture 5, the spectra of the white light 12 from the standard YAG phosphor 3 with a colour temperature (CCT) of 6500 K are used for reference.
For example, to obtain the emitted light 13 at the angle α of 30 degrees of the output aperture 5 of the retro-reflector 4 and at the colour temperature of 6000 K, the BYR needs to be approximately 2.75, as illustrated in
The parameters illustrated in
The factors Y0, A1, t1, A2, and t2 in the above expression (Formula 1) are calculated by a simulation of the colour temperature (CCT) finally obtained after the infinite number of times of retro-reflection performed at each BYR and each angle α, and are derived by fitting the simulation results. The above expression (Formula 1) and the factors Y0, A1, t1, A2, and t2 have no physical meanings. The above expression (Formula 1) is a simplified approximate expression obtained by the fittings to express the simulation results with a simple expression.
First, the spectra of the laser pump light 11 and the spectra of the white light 12 are selected. Then, the blue light ratio is changed, and the colour temperature (CCT) at the angle α of 90 degrees (no retro-reflector 4 is provided) is calculated. In the example illustrated in
This is based on the concept to use the phosphor 3 that originally emits more blueish white light in order to achieve a desired colour temperature of the emitted light 13 from the output aperture 5.
When the chromaticity of white light is plotted on the Planckian locus (blackbody locus), the white light can be regarded as natural light in the nature (such as light from charcoal, a candle flame, or light from an incandescent lamp). By controlling the chromaticity of this white light to be proximate to the blackbody locus, the white light further approximates to natural illumination, which is technically significant and economically valuable.
By changing the BYR from 1 to 2:1, as illustrated in
A converter 14A includes a substrate 10 and a phosphor 3A. The phosphor 3A has its particle density adjusted in accordance with the angle α of the output aperture 5 of the retro-reflector 4. The particle density of the phosphor 3A is adjusted to reduce blue light absorption to thus increase the colour temperature (CCT).
Reduction of the particle density of the phosphor 3A increases the ratio of a binder material of the phosphor 3A. This ratio has some variations.
For a pump light source of the present embodiment used in automotive applications, the colour of emitted light is preferably white and with a colour temperature of around 6000 K. An optimized ratio for the colour temperature (CCT)=6000 K without the retro-reflector 4 is YAG (Ce (Ce=0.7 mol %, d50=8 um)):SiO2 binder=80%:20%.
If the retro-reflector 4 with an output aperture 5 of α=30 degrees is added, the colour temperature (CCT) shifts to 4250 K according to calculations.
When the ratio of the phosphor 3A to the binder material are adjusted to these values YAG (Ce (Ce=0.7 mol, d50=8 um)):SiO2 binder=65%:35*, it would be possible to achieve a colour temperature (CCT) of 6000 K at the output aperture 5 of angle α=30 degrees.
Another way to achieve the target colour temperature (CCT) would be to reduce the density of Ce, which is the emission center of the phosphor 3A, to these values YAG (Ce (Ce=0.4 mol %, d50=8 um)):SiO2 binder=80%:20%.
Another way would be to reduce the particle size of the phosphor 3A to these values YAG (Ce (Ce=0.7 mol %, d50=2 um):SiO2 binder=80%:20%.
For the phosphor 3A, a phosphor material that emits light with a shorter wavelength, such as GAL, than that of a standard YAG material may be used. This may lower the conversion efficiency of the phosphor 3A, but this should not be a big problem, because the blue light will be recycled with the retro-reflector 4, and so increase the probability of being absorbed by the phosphor 3A.
A nanophosphor adjusted to emit light at a desired colour temperature may be used. Nanophosphors are typically particles with the diameter of 100 nm or smaller. Their properties of emission depend on the material and the particle size.
A converter 14B includes a substrate 10 and a phosphor 3B. The phosphor 3B includes air bubbles 16, as illustrated in
Another embodiment of the present invention will be described, below. For convenience of illustration, components having the same functions as those described in any of the above embodiments are denoted with the same reference signs without being described repeatedly.
As illustrated in
The phosphor 3C is made of a standard phosphor conversion material containing YAG particles and a binder material. The scattering layer 8 transmits 100% of yellow light. The scattering layer 8 transmits part of, that is, 90% of blue light of the wavelength of 450 nm, and scatters 10% of the blue light. Thus, most part of the blue light is transmitted to the phosphor 3C through the scattering layer 8, and converted into yellow light by the phosphor 3C. The ratio of blue light transmitted through the scattering layer 8 and blue light scattered by the scattering layer 8 can be changed to adjust the colour temperature of the blue light. The scattering layer 8 can be made of a dielectric multilayer (DBR) made of TiO2 and SiO2 on a rough surface.
As illustrated in
The scattering particles 9 are formed from fine particles such as polystyrene, TiO2, or Al2O3, or nanoparticles, which do not absorb light in the visible wavelength range. The scattering particles 9 are spherical to avoid polarization dependence. If polarization dependence is desired, non spherical nanoparticles are used for the scattering particles 9. The dimension of nanoparticles forming the scattering particles 9 should be similar to the wavelength (450 nm) of the laser pump light 11. Increasing the dimension of nanoparticles will shift the scattering peak wavelength toward the red, and decreasing the dimension of nanoparticles will shift the scattering peak wavelength toward the violet.
The scattering layer 8 and the scattering particles 9 may be combined to form a converter.
In Embodiment 3, geometric pattern combinations between any of substrates 10E, 10F, and 10G and any of phosphors 3E, 3F, and 3G form blue-light-ratio increasing members that increase the blue light ratio of the white light 12 converted by the phosphors 3E, 3F, and 3G.
As illustrated in
As illustrated in
The triangular portions and the curved portions may be combined to form a substrate.
As illustrated in
Preferably, the substrate 10G has an exposed portion devised to diffusively reflect the laser pump light 11 when the laser pump light 11 hits the surface of the substrate 10G. Specifically, the surface of the substrate 10G diffusively reflects the blue light and the white light 12. The substrate 10G can obtain properties of diffusively reflecting the blue light and the white light 12 by selecting the substrate 10G that has a surface having diffusive reflective properties suitable for these types of light or by depositing a coating having similar diffusive reflective properties on the substrate 10G.
Geometric patterns different from the patterns illustrated in
Thermal properties of the phosphors 3E, 3F, and 3G can also be improved in this way because the phosphors 3E, 3F, and 3G have larger areas that are in contact with the substrates 10E, 10F, and 10G. Preferably, the substrates 10E, 10F, and 10G are made of a metal with high thermal conductivity such as aluminium or copper but can also be made of other material such as an aluminum oxide. The use of the substrates 10E, 10F, and 10G of such geometric patterns may be thought to reduce the color mixing if the phosphors 3E, 3F, and 3G are used without a retro-reflector 4. However, this problem is solved by the retro-reflector 4 that recycles the white light 12 and so increases the color mixing by increasing the number of reflection inside of the retro-reflector 4.
The laser pump light 11 emitted from the semiconductor laser diode of the pump light source 2 and focused via a lens system is incident on the phosphor 3 in a spot size of 0.5 mm diameter. Part of the white light 12 resulting from wavelength conversion is reflected by the retro-reflector 4 back to the phosphor 3 as retro-reflection light, while another part is scattered by the phosphor 3. The emitted light 13, which is another part of the white light 12, is emitted through the output aperture 5 of the angle 2α. The colour temperature (CCT) of the emitted light 13 can be changed by changing the angle α of the output aperture 5 or by changing the colour temperature of the white light 12 emitted by the phosphor 3. A small angle α is usually desirable to result in a pump light source 2 with a small etendue. For a fixed small angle α (for example, 30 degrees), the colour temperature of the emitted light 13 emitted through the output aperture 5 can be adjusted by changing the colour temperature of the white light 12 emitted by the phosphor 3.
The retro-reflector 4 includes an output aperture 5 of the angle 2α and a coupling aperture 15 for a laser pump light 11. Preferably, the retro-reflector 4 is a half sphere having the coupling aperture 15 with a diameter larger than the diameter of the laser pump light 11 when the laser pump light 11 hits the phosphor 3. The retro-reflector 4 can be made of a hollow structure with a highly reflective internal surface. The structure of the retro-reflector 4 could be made of a metal, a plastic, or any material that can function in such a way. The retro-reflector 4 can also be made of a transparent solid half sphere such as glass, BK7, or any other material that are transparent to visible light. The outer peripheral surface of the transparent half sphere is then coated with a reflective layer that could be made of aluminium, titanium, palladium, nickel, or any other material that has a high reflectivity. When the retro-reflector 4 is a metal shell retro-reflector, the inner wall of the half sphere is coated with a highly reflective material. When the retro-reflector 4 is a retro-reflector made of a transparent member such as glass, the outer wall of the half sphere is coated with a highly reflective material.
The retro-reflector 4 can be mounted in contact with the phosphor 3 using a non light absorbing layer. This non light absorbing layer may have high thermal conductivity. There may also be a gap between the phosphor 3 and the end surface of the retro-reflector 4 facing the phosphor 3.
The coupling aperture 15 may have any shape. The coupling aperture 15 needs to have a size larger than the size of the laser pump light 11 to prevent the laser pump light 11 from being blocked. Typically, the coupling aperture 15 has a size smaller than the size of the output aperture 5 to reduce the loss of light that could escape out of the coupling aperture 15. If the coupling aperture 15 is too large, it will also affect the colour temperature of the emitted light 13 emitted through the output aperture 5, which is not desirable.
The laser pump light 11 is preferably incident on the coupling aperture 15 of the retro-reflector 4 so that it hits the surface of the phosphor 3 at the center of the retro-reflector 4. In the case where the retro-reflector 4 has a half sphere structure, the laser pump light 11 hits the surface of the phosphor 3 at the center of the retro-reflector 4.
The output aperture 5 is most preferably circular. In the case where the retro-reflector 4 has a hollow structure, the coupling aperture 15 and the output aperture 5 are formed by forming holes in the structure. In the case where the retro-reflector 4 has a solid structure such as glass, the coupling aperture 15 and the output aperture 5 are formed by not coating the area of the coupling aperture 15 and the output aperture 5 by a reflective layer so that the area is transparent to visible light.
This changing in the colour temperature of the white light 12 from the phosphor 3 can be obtained by adding the scattering particles 7 in the phosphor 3 with the following characteristic: adding the scattering particles 7 within the phosphor 3 to decrease the phosphor density and increase scattering of the laser beam. These scattering particles 7 could be of different materials, such as Al2O3, diamond, or TiO2. A typical diameter of the scattering particles 7 is around 500 μm to 600 μm. The scattering particles 7 preferably have very low absorption of the light in the visible range. The scattering particles 7 could be made of high thermal conductivity materials to improve the thermal properties of the phosphor 3.
If the scattering particles 7 are used alone without a retro-reflector, it is usually a problem because they will decrease the light emitting efficiency of the phosphor 3, increase the emission area of the phosphor 3 due to scattering of light at the scattering particles 7, and fail to obtain an appropriate colour temperature. However, when the retro-reflector 4 and the scattering particles 7 are used in combination, these problems can be partially or completely suppressed. Thanks to the retro-reflector 4 recycling the white light 12, the color homogeneity will be improved, so that white light with an appropriate colour temperature can be obtained. Using the retro-reflector 4 having the output aperture 5 with a small angle α will decrease the emission angle of the white light, which is advantageous.
The light source unit 1H differs from the light source unit 1 described above with
Instead of the two pump light sources 2, three or more pump light sources may be provided.
The light source unit 1I differs from the light source unit 1 described above with
This changing in the colour temperature of the white light 12 from the phosphor 3C is obtained by adding the scattering layer 8 with the following characteristics on the upper surface of the phosphor 3C.
The scattering layer 8 transmits 100% of the green to yellow light, or light having a wavelength above 500 nm. The scattering layer 8 transmits part of (80% or less) blue light of a wavelength of 450 nm of the laser pump light 11, and partially diffusively reflects or scatters another part of (20% or more) blue light. Specifically, the scattering layer 8 transmits most part of the blue light. The phosphor 3C absorbs part of the blue light that has been transmitted through the scattering layer 8, and the part of the blue light is subjected to wavelength conversion to be formed into yellow light. By changing the ratio of the diffusively reflected or scattered blue light with the scattering layer 8, the colour temperature of the white light 12 from the phosphor 3 can also be changed.
The scattering layer 8 could be made of a multi-layer structure of SiO2/TiO2 layers or any dielectric layers that are arranged to make an interference filter with such properties.
This modification example differs from the light source unit 1 described above in
Any of light source units 1 and 1H to 1K according to a first aspect of the present invention includes a pump light source 2 that emits a laser beam (laser pump light 11); a phosphor 3 that converts the laser beam (laser pump light 11) emitted from the pump light source 2 into converted light (white light 12), and a retro-reflector 4 or 41 that has an output aperture 5, which allows emission of part of the converted light (white light 12) converted by the phosphor 3 as emitted light 13, the retro-reflector 4 or 41 reflecting another part of the converted light (white light 12) back to the phosphor 3. The phosphor 3 includes a blue-light-ratio increasing member (scattering particles 7, a scattering layer 8, or scattering particles 9), which increases the blue light ratio of the converted light (white light 12).
In the above structure, the phosphor reflects part of the retro-reflection light returned from the retro-reflector toward the output aperture to add the part of the retro-reflection light to the emitted light. With the addition of the part of the retro-reflection light, the blue light ratio of the converted light converted by the phosphor increases on the basis of a desired colour temperature of the emitted light emitted through the output aperture and the dimension of the output aperture. Thus, a phenomenon of decreasing the white colour temperature of emitted light emitted through the output aperture due to the addition of part of the retro-reflection light can be partially or completely suppressed. Thus, a light source unit capable of emitting preferable white light can be achieved.
In a light source unit 1, 1H, 1I, or 1K according to a second aspect of the present invention having the structure according to the first aspect, the blue-light-ratio increasing member may be scattering particles 7 included in the light converter layer (converter 14) to scatter the laser beam (laser pump light 11) emitted from the pump light source 2.
In the above structure, the scattering particles scatter blue light of the laser beam. Thus, the blue light absorption of the phosphor can be partially or completely suppressed. The blue light ratio of the converted light converted by the phosphor is thus increased.
In a light source unit 1, 1H, 1I, or 1K according to a third embodiment of the present invention and having the structure according to the above aspect 1, the scattering particles 7 may be formed from a high thermal conductivity material to improve the thermal properties of the phosphor 3.
In the above structure, the blue light absorption of the phosphor is further suppressed.
In a light source unit 1 according to a fourth aspect of the present invention and having the structure according to the first aspect, the blue-light-ratio increasing member may be the phosphor 3A having a particle density adjusted in accordance with a size of the output aperture 5 of the retro-reflector 4.
In the above structure, the particle density of the phosphor is adjusted in accordance with the size of the output aperture of the retro-reflector. Thus, the blue light absorption of the phosphor can be partially or completely suppressed, so that the blue light ratio of the converted light converted by the phosphor increases.
In a light source unit 1J according to a fifth aspect of the present invention having the structure according to the first aspect, the blue-light-ratio increasing member may be a scattering layer 8 disposed on a surface of the phosphor 3 facing the pump light source 2 to diffusely reflect or scatter the laser beam (laser pump light 11) emitted from the pump light source 2.
In the above structure, a laser beam emitted from a pump light source is reflected or scattered by a scattering layer. Thus, the blue light absorption of the phosphor can be partially or completely suppressed, so that the blue light ratio of the converted light converted by the phosphor increases.
In a light source unit 1 according to a sixth aspect of the present invention and having the structure according to the first aspect, the blue-light-ratio increasing member may be scattering particles 9 disposed on a surface of the phosphor 3 facing the pump light source 2 to diffusely reflect or scatter the laser beam (laser pump light 11) emitted from the pump light source 2.
In the above structure, a laser beam emitted from the pump light source is diffusedly reflected or scattered by the scattering particles disposed on the surface of the phosphor facing the pump light source. Thus, the blue light absorption of the phosphor can be partially or completely suppressed, so that the blue light ratio of the converted light converted by the phosphor increases.
A light source unit 1 according to a seventh aspect of the present invention and having the structure according to the first aspect may further include substrates 10E, 10F, and 10G that support the phosphors 3E, 3F, and 3G, and in which the blue-light-ratio increasing member may be constituted of a combination of geometric patterns of the substrates 10E, 10F, and 10G and the phosphors 3E, 3F, and 3G.
In the above structure, the substrates and the phosphors are combined into geometric patterns. Thus, the blue light absorption of the phosphor can be partially or completely suppressed, so that the blue light ratio of the converted light converted by the phosphor increases.
In any of the light source units 1 and 1H to 1K according to an eighth aspect of the present invention and having the structure according to the first aspect, a desired colour temperature of the emitted light 13 may be larger than or equal to 2000 K and smaller than or equal to 10000 K.
In the above structure, the blue light ratio of the converted light converted by the phosphor can be increased on the basis of the size of the output aperture of the retro-reflector.
In any of the light source units 1 and 1H to 1K according to a ninth aspect of the present invention and having the structure according to the first aspect, the retro-reflector may have a hollow dome shape or a flat plate shape.
In the above structure, the retro-reflector can reflect another part of the converted light back to the phosphor as retro-reflection light.
In any of the light source units 1 and 1H to 1K according to a tenth aspect of the present invention and having the structure according to the first aspect, the retro-reflector 4 or 41 may be coupled to the phosphor 3 directly or via an intermediate layer.
In the above structure, the retro-reflector and the phosphor can have a simple structure.
In any of the light source units 1 and 1H to 1K according to an eleventh aspect of the present invention and having the structure according to the first aspect, the blue light ratio increased by the blue-light-ratio increasing member may be determined by the following formula 1 relating to the desired colour temperature and the size of the output aperture: CCTwr(α)=Y0+A1eBYR/t1+A2eBYR/t2 . . . (Formula 1), in which the factors Y0, A1, t1, A2, and t2 may be dependent on the angle α representing the size of the output aperture of the retro-reflector, and the BYR may be a ratio between the blue light part and the yellow light part of the spectra of the converted light from the phosphor.
In the above structure, the blue light ratio can be easily determined based on the desired colour temperature and the size of the output aperture.
A light source unit 1H according to a twelfth aspect of the present invention and having the structure according to the first aspect may further include a different pump light source 2 that emits a different laser beam (laser pump light 11), and in which the phosphor 3 may convert the laser beam (laser pump light 11) emitted from the pump light source 2 and the different laser beam (laser pump light 11) emitted from the different pump light source 2 into the emitted light (white light 12).
In the above structure, a light source unit capable of emitting preferable white light with high intensity can be achieved.
The present invention is not limited to the above-described embodiments, and may be changed in various manners within the scope of claims, and the embodiments obtained by appropriately combining technical devices disclosed in any two or more different embodiments are also included in the technical scope of the present invention. Moreover, new technical features can be formed by combining the technical devices described in the embodiments.
| Number | Date | Country | |
|---|---|---|---|
| 62772191 | Nov 2018 | US |
