 
                 Patent Application
 Patent Application
                     20080036364
 20080036364
                    
    
    
    
    
    
    
    
    
    
Disclosed herein are “smart” phosphor compositions capable of passively adjusting their own chromaticity (hence the term, “self-adjusting”) in response to variations in the excitation wavelengths of the blue/UV LED chips with whom they are partnered. The illumination product formed by combining the light emitted by the phosphor composition with the various light emitted by a library or selection of blue/UV LED chips has a substantially constant chromaticity. The term “constant chromaticity” in this context means that the x and y CIE chromaticity coordinates of the product illumination each vary by no more than five percent of a reference value.
The principles of operation of a “smart” phosphor composition may be illustrated by inspecting the data in 
The data in 
While not wishing to be bound by any particular theory, the observed behavior of the individual green and orange phosphors may be explained by the nature of the match between the energy of a photon from the excitation light and the electrical band gap of the phosphor; the “quality” of the match being related to the efficiency at which the phosphor emits light. The light emitted by a green phosphor has a higher energy and a shorter wavelength relative to that emitted by an orange phosphor, indicating that the green phosphor has a larger band gap. Thus, as the peak excitation wavelength is increased the energy of this excitation radiation decreases, becoming less and less optimally matched to the large band gap of the green phosphor (relative to orange), and the intensity of the emission decreases. In contrast, the orange phosphor's band gap is smaller than the green phosphor, such that as the excitation wavelength is increased the energy of the photons decrease, and the excitation becomes better and better matched to the smaller band gap (relative to green) of the orange phosphor. The efficiency at which the orange phosphor emits increases as the wavelength of the blue LED light is increased, indicating that the orange phosphor's lower band gap is more appropriately matched to lower energy excitation.
A “smart” phosphor composition may be defined as a combination of a first phosphor whose emission intensity decreases as the wavelength of the radiation being used to cause its luminescence is increased, with a second phosphor whose emission intensity increases as the excitation wavelength is increased. The advantages of such a phosphor composition include the realization of a lighting scheme that demonstrates substantially constant chromaticity under conditions of varying excitation wavelength. Such a variation in wavelength of the light emitted from different blue LED chips comes about predominantly as a result of manufacturing variations that occurred during production of the blue LED chips. Manufacturing variations can lead to batches of blue LED chips having a range of band gap widths, the consequence to commercial operations being a binning requirement, an exemplary protocol described earlier in this disclosure.
Returning to again to 
Referring to 
Advantages of the present embodiments are perhaps better appreciated when data is viewed graphically on a CIE chromaticity diagram. Shown in 
Referring again to 
Significant advantages of the present embodiments are that a substantially constant chromaticity is realized within a wide range of phosphor compositions, even with undesirable fluctuations in the excitation wavelength. Among the advantages of the present embodiments is that blue/UV LED chips no longer need be “sorted” or “binned” (at least to the extent that they were before) because the smart phosphor composition is able to “self-adjust” the chromaticity of its light output in response to LED variability. In the example of 
The capability of maintaining the chromaticity at a substantially constant value is important because the locus of chromaticity coordinates that lie along the curved line passing through about (0.3, 0.3) and about (0.45, 0.4) are said to lie along the Black Body Locus (BBL). This is a locus of points defined by Planck's equation:
  
  
  E(λ)=Aλ−5/(e(B/T)−1).
Here, E is the emission intensity of the phosphor composition, λ is the emission wavelength, T the color temperature of the black body, and A and B are constants. Color coordinates that lie on or near the BBL locus of points yield pleasing white light to a human observer. Thus, as shown in 
Further demonstration of the ability of the present compositions to self-adjust chromaticity; thereby maintaining chromaticity at substantially constant values even under variations of the excitation wavelength, is shown in 
Examination of 
In general, phosphor compositions having a self-adjusting chromaticity may be generated by blending a phosphor from a so-called group “A,” whose members share the common trend that emission intensity decreases with increasing excitation wavelength, with a Group “B” phosphor whose members show the opposite trend: emission intensity increases as the excitation wavelength is increased. An exemplary range of wavelengths is 450 to 460 nm.
The opposing trends used to group a phosphor make sense intuitively. The emission intensity of a phosphor is related to efficiency at which it absorbs its excitation radiation, and this efficiency is in turn related to the matching of the energy between a photon from the excitation radiation, and the band gap width of the phosphor. The light from the UV/blue LED, in this case, provides the excitation radiation to the phosphor, and in one embodiment, the UV/blue LED provides excitation radiation over a wavelength range of 450 to 460 nm.
A division between group A and group B phosphors may generally be made at a band gap energy substantially equivalent to the energy of a photon of yellow light. Thus, group A phosphors may be said to lie on the higher energy side of the yellow phosphors, and include blue, green, and yellow-green phosphors. Group B phosphors may be said to lie on the lower energy side of the yellow phosphors, and include yellow-orange, orange, and red phosphors. In the photoluminescent process, a phosphor is “down-converting” energy absorbed from a photon of excitation radiation to a photon that is emitted from the phosphor, the energy of the emission related to the phosphor's band gap through which an electronic relaxation process occurs, this energy difference being equal to the energy of the emitted photon.
Down-conversion in group A phosphors, with their larger band gaps, is more efficient with higher energy excitation radiation, meaning shorter wavelength light. Thus, emission intensity decreases as the energy of the excitation is reduced (remembering that an increase in excitation wavelength from 450 to 460 nm is a decrease in energy).
In contrast, group B phosphors lie on the orange side of yellow, and emit lower energy (longer wavelength) light relative to group A phosphors, because of their smaller band gap widths. In this case, the down-conversion process occurs more efficiently as the phosphor is excited by lower and lower energies, at least within a designated wavelength range. Thus, the emission intensity of a group B phosphor increases with increasing excitation wavelength.
Principles which may be used to design a self-adjusting phosphor are shown in 
The three phosphors at the top of the far left column are labeled “G-series,” “Y-series,” and “O-series,” and refer to phosphor compositions developed by the present inventors, each series emitting substantially in the green, yellow, and orange regions of the spectrum, respectively. YAG is the commonly known material yttrium aluminum garnet, having the formula Y3Al5O12:Ce3+, and the formula of the terbium aluminum garnet TAG is Tb3Al5O12:Ce3+. YAG and TAG are commercially available phosphors that emit in the yellow and orange regions of the spectrum, respectively. GP-4 is a green emitting YAG phosphor, also commercially available, having the formula Y3(AlGa)5O12:Ce3+, and like YAG and TAG, it too is activated by trivalent cerium.
Below those top three phosphors in the far left column are three sulfide-based phosphors, and below those, three phosphors based on silicon nitride and silicon oxynitride. Of the sulfides, two emit in a relatively narrow spectral range, SrGa2S4:Eu in the green, and CaS:Eu in the red. Distinguished from that is the sulfide ZnSexS, x:Cu, which can be configured to emit in a broad spectral range that includes the colors green, yellow, orange, and red. The silicon nitride and silicon oxynitrides are also capable of emitting over a relatively large spectral range, with SrSi2O2N2:Eu emitting in the green and yellow, and (Sr,Ba,Ca)2Si5N8:Eu emitting in the yellow, orange, and red, when compositional changes are made in the relative amounts of the alkaline earth components. In at least one case where the alkaline earth component was fixed using a single element, the phosphor emitted in a more narrow range of the spectrum, primarily within a single color range. For example, the silicon nitride based phosphor Si2Si5N8:Eu emitted in the red.
Referring again to 
While the trends demonstrated by the orange and green phosphors of 
Examples of the yellow phosphors that may be categorized as group B phosphors are the Y-series developed by the present inventors (although these may more accurately be described as “yellow-green,” as described below), and the silicon oxynitride SrSi2O2N2:Eu. One example of a phosphor falling into group A is the highly conventional and commercially available, Ce doped phosphor yellow-YAG; another is the silicon nitride compound (Sr,Ba,Ca)2Si5N8:Eu. The former observation may suggest that the yellow YAG may more accurately be thought of as a yellow-orange phosphor, whereas the output of the silicon nitride may be adjusted via the ratio of the alkaline earth elements. The copper activated sulfide phosphor ZnSexS1-x:Cu has a behavior that is difficult to interpret in that it may be configured to emit in any of the colors green, yellow, orange, and red, and a categorization of this phosphor into a specific group is not shown in 
A benchmark against which other group A/group B pairs may be judged, particularly in terms of the ability to self-regulate chromaticity, is the composition made by combining a “G-series” phosphor of the type M2SiO4, with an “O-series” phosphor of the type M3SiO5, where M is an alkaline earth element in both types of silicates, and where phosphors of the G and O-series were developed by the present inventors. The G-series phosphors may also be used in combination with a Y-series of phosphors, again belonging to the present inventors, where phosphors in the Y-series have the M2SiO4 configuration. Though the latter are represented in 
As alluded to previously, not all combinations of a group A phosphor and a group B successfully produce the constant chromaticity property. An example of a group A phosphor paired with a group B phosphor which combination does not produce any significant “smart activity” are the commercially available green YAG (also denoted as GP-4) and the cerium doped yellow YAG phosphor, shown as an unshaded cell in 
That the group A and group B phosphors of the present invention have contrasting behavior with regard to their excitation spectra is further illustrated in 
Further quantification of the behavior of group A and group B phosphors is shown in 
Excitation spectra of the commercially available phosphors YAG, TAG, and GP-4 are given in 
In addition to the benchmark of smart phosphor performance given by the present inventors' G and O-series phosphors, examples will be provided now utilizing at least one commercially available and/or prior art component phosphors. The results from testing pairs of phosphors are summarized in 
In another embodiment, a smart phosphor comprises a group B, green SrGa2S4:Eu phosphor and a group A, O-series phosphor invented and previously disclosed by the present inventors. The green SrGa2S4:Eu phosphor may also be combined with either a group A, yellow YAG or an orange TAG phosphor.
In another embodiment of the present invention, a smart phosphor is made by combining a group A, red CaS:Eu phosphor with a phosphor from either of the G or Y-series of green and yellow-green, silicate-based phosphors provided by the present inventors. The red CaS:Eu may also be combined with other group B phosphors, such as the GP-4 green YAG and the green SrGa2S4:Eu phosphors.
The copper activated phosphor ZnSexSi x:Cu is somewhat unusual among these examples in that it may be configured to emit in any of the four colors green, yellow, orange, and red. These particularly configured phosphors will be referred to as green ZnSexS1-xCu, yellow ZnSexSi1-x:Cu, orange ZnSexSi1-x:Cu, and red ZnSexSi1-x:Cu. In another embodiment of the present invention, a smart phosphor comprises a group A, red ZnSexS1-x:Cu and one or more of either of the group B, G or Y-series phosphors. The green or yellow ZnSexS1-x:Cu phosphors, in keeping with theory, may be combined with any of the group A phosphors selected from the group consisting of a yellow YAG, an orange TAG, and a red CaS:Eu phosphor.
Turning now to the silicon oxynitrides, the group B, green (and/or yellow) SrSi2O2N2:Eu compound may in one embodiment be combined with any of the group A phosphors selected from the group consisting of the present inventors' O-series, silicate-based phosphors previously disclosed, a yellow (possibly yellow-orange) YAG, an orange TAG, a red CaS:Eu, and a red ZnSexS1-x phosphor.
A number of smart phosphor compositions may be designed around the silicon nitride compound (Sr,Ba,Ca)2Si5N8:Eu. The relative content of the alkaline earth elements in this compound may be varied to construct a “family” of phosphors emitting either a green, yellow, orange, or red color, as desired. Accordingly, the green and yellow emitting versions of this phosphor demonstrate group B behavior; the orange and red version group A behavior. Each member of the series may be identified by it emission color: (Sr,Ba,Ca)2Si5N8:Eu, yellow (Sr,Ba,Ca)2Si5N8:Eu, orange (Sr,Ba,Ca)2Si5N8:Eu, red (Sr,Ba,Ca)2Si5N8:Eu phosphor, and the like.
In some embodiments of the present invention, a smart phosphor comprises a group B, green and/or yellow (Sr,Ba,Ca)2Si5N8:Eu silicon nitride phosphor with a group A, Y-series or O-series, silicate-based phosphor previously disclosed by the present inventors. Alternatively, the green and/or yellow (Sr,Ba,Ca)2Si5N8:Eu phosphor may be paired with a group A, yellow YAG or orange TAG phosphor. It may also be paired with either of the a group A sulfides, red CaS:Eu or ZnSexS1-x:Cu.
Common to phosphor compositions that may be configured to emit over a wide spectral range is the ability to pair a green or yellow version of the phosphor with an orange or red version of the same phosphor, and the silicon nitride family (Sr,Ba,Ca)2Si5N8:Eu is advantageously used in this situation as well. In this embodiment, a group B, green or yellow (Sr,Ba,Ca)2Si5N8:Eu phosphor is paired with a with a group A, orange or red (Sr,Ba,Ca)2Si5N8:Eu phosphor, such that the majority of the composition of this embodiment is (Sr,Ba,Ca)2Si5N8:Eu.
Smart phosphors may also be designed around (Sr,Ba,Ca)2Si5N8:Eu in its group A configuration, designated by orange (Sr,Ba,Ca)2Si5N8:Eu and red (Sr,Ba,Ca)2Si5N8:Eu. In one embodiment of the present invention, a smart phosphor is made by combining a group A, red (Sr,Ba,Ca)2Si5N8:Eu with a group B phosphor selected from the group consisting of a G-series silicate-based phosphor, a Y-series silicate-based phosphor, and a green SrSi2O2N2:Eu phosphor.
More general descriptions of the G-series and Y-series phosphors of the present embodiments will now be given. Phosphors of the G-series comprise silicate-based compounds having the formula (Sr,Al)x(Si,A2)(O,A3)2+x:Eu2+, where A1 is at least one divalent cation (a 2+ ion) including magnesium (Mg), calcium (Ca), barium (Ba), or zinc (Zn), or a combination of 1+ and 3+ cations, wherein the 1+ cations may include K, Na, and Li, and wherein the 3+ cations may include Cs, Y, Ce, Bi, and Li. The A1 cation(s) component may comprise a combination of some 2+ cations and a substantially equal number of 1+ and 3+ cations. A2 is a 3+, 4+, or 5+ cation, including at least one of boron (B), aluminum (Al), gallium (Ga), carbon (C), germanium (Ge), and phosphorus (P). A3 is a 1−, 2−, or 3− anion, including fluorine (F), chlorine (Cl), bromine (Br), nitrogen (N), and sulphur (S). The value of x is any integer or non-integer between 1.5 and 2.5, both inclusive. In one embodiment of the invention, x is not 2. The formula is written to indicate that the A1 cation replaces strontium (Sr); the A2 cation replaces silicon (Si), and the A3 anion replaces oxygen (O). In one embodiment of the present invention, A3 may be sulphur (S) and there may be little or no oxygen in the compound, such that the phosphor is substantially a sulfide rather than an oxide.
As taught by G. Blasse et al. in Philips Research Reports Vol. 23, No. 1, pp. 1-120, the crystal structure of a β-Ca2SiO4:Eu, Sr2SiO4:Eu, or Ba2SiO4:Eu composition, with Eu2+ at a concentration of 2 atomic percent, is K2SO4-like. Thus, it is contemplated that the present G-series green silicate phosphors have a similar host lattice.
The optical properties of these G-series phosphors may be controlled, among other methods, by adjusting the ratio of the A1 cation to strontium, where A1 may be an alkaline earth element or a transition metal element, or combinations thereof. For example, the wavelength position at which the peak emission occurs changes in a (Sr1-xBax)2SiO4 phosphor system from a green at 500 nm for x=1 (in other words, when the alkali metal content is 100 percent Ba) to a yellow at 580 nm when x=0 (100 percent Sr). The conversion efficiency from the same light source at 450 nm shows a continuous increase when the Ba increases from 0 to about 90 percent. The peak emission wavelength of 545 nm, obtained when x=0.3, is close to that of a YAG:Ce peak emission wavelength.
There are a variety of ways to include the A3 anion into the inventors' own G-series, green silicate-based phosphors. In one embodiment, a halogen is added to the phosphor composition during a liquid phase step of processing, such as that encountered during the sol-gel or co-precipitation processing methods. This liquid processing allows for mixing on a molecular level, such that the A3 anion is well dispersed within the composition prior to later crystallization steps (e.g., sintering). The present inventors have previously found that the A3 anion influences both emission intensity and peak wavelength. While not wishing to be bound by any particular theory, it is believed that the luminescence of these phosphors Eu doped silicate-based phosphors is due to of the Eu doped phosphors is due an electronic transition from 4f65d1 to 4f7 in the Eu activator. Emission wavelength depends on the crystal field splitting of the 5d level. With increasing crystal field strength, emission wavelengths increase. The luminescence peak energy of the 5d to 4f transition is affected the most by parameters that affect electron-electron repulsion in the crystal; in other words, the distance between Eu cations and its surrounding anions, and the average distance between cations and ions.
Liquid processing enables at least some of the A3 anions to replace the O2− anions of the host silicate, and to become incorporated into the crystal lattice. When the A3 anion is monovalent, as is the case with the halogens, then cation vacancies may be created in the crystal lattice in order to maintain electrical charge neutrality. Since vacancies at the cation positions reduce the average distance between cations and anions, the crystal field strength will be increased. Therefore, the peak of the emission curves will move to longer wavelengths as the halogen content increases, and as more cation vacancies are created. The emission wavelength is directly related to the energy gap between the ground and excited states of the electron in question, and this in turn is determined by the crystal field strength.
In the case of the present silicate-based phosphors, the fact that emission wavelength increases as a function of increasing halogen content (within a certain range of halogen content) is strong evidence of halogen incorporation into the host lattice, most likely substitutionally located on oxygen lattice sites. In one embodiment of the present invention, the A3 anion is fluorine or chlorine. Additional evidence of halogen incorporation into the lattice is provided by the data when phosphorus (P) is added to the composition, phosphorus being an A2 cation in at least the case of the G-series phosphors. Addition of phosphorus does not substantially change emission wavelength, and this is evidence, again, that the phosphorus behaves as a cation and therefore does not replace oxygen in the host crystal. Thus, phosphor addition does not appreciably change the host material's crystal field strength in the crystal field surrounding the Eu2+ ions, which consist essentially of oxygen sites.
Phosphors of the Y-series comprise silicate-based compounds having the formula A2SiO4:Eu2+D, wherein A is at least one of a divalent metal selected from the group consisting of Sr, Ca, Ba, Mg, Zn, and Cd, and D is a negatively charged ion, present in the phosphorin an amount ranging from about 0.01 to 20 mole percent. There may be more than one of the divalent metal A present in any one phosphor. According to the present embodiments, D may be a dopant ion selected from the group consisting of F, Cl, Br, and I, but D can also be an element such as N, S, P, As, and Sb. The silicate based phosphor is configured to absorb an excitation radiation having a wavelength ranging from about 280 to about 520 nm.
An exemplary Y-series phosphor configured to emit light having a wavelength ranging from about 460 to 590 nm has the composition (Sr1-x-yBaxCayEu0.02)2SiO4-zDz, where 0<x≦0.0, 0<y≦0.8, and 0<z≦0.2. An alternative formula for an exemplary Y-series phosphor is (Sr1-x-y-BaxMgyEu0.02)2SiO4-zDz, where 0<x≦1.0, 0<y≦0.2, and 0<z≦0.2. In an alternative embodiment the Y-series phosphor is (Sr1-x-yBaxMyEu0.02)2SiO4-zDz, where 0<x≦1.0, and M is one or more of Ca, Mg, An, and Cd. In this embodiment, the condition 0<y≦0.5 applies when M is Ca; 0<y≦1.0 when M is Mg, and 0<z≦0.5 when M is either Zn or Cd. In one embodiment, the dopant D is either F, or Cl, or both, and in this embodiment, at least some of the F or Cl replaces oxygen in the host crystal lattice.
Phosphors of the O-series comprise silicate-based compounds having the formula (Sr,A1)x(Si,A2)(O,A3)2+x:Eu2+, where A1 is at least one divalent cation (a 2+ ion) including magnesium (Mg), calcium (Ca), barium (Ba), or zinc (Zn), or a combination of 1+ and 3+ cations, A2 is a 3+, 4+, or 5+ cation, including at least one of boron (B), aluminum (Al), gallium (Ga), carbon (C), germanium (Ge), and phosphorus (P); and A3 is a 1−, 2−, or 3− anion, including fluorine (F), chlorine (Cl), bromine (Br); and x is any value between 2.5 and 3.5, inclusive. As with the G-series phosphors, the formula for the Y-series phosphors is written to indicate that the A1 cation replaces silicon (Si), and the A3 anion replaces oxygen (O).
Phosphors of these O-series, silicate-based phosphors may also be described in general by the formula (Sr1-xMx)yEuzSiO5, wherein M is at least one of a divalent alkaline earth metal selected from the group consisting of Ba, Mg, and Ca, but it may include other divalent elements as well, such as Zn. The values of x, y, and z follow the following relationships: 0<x≦0.5, 2.6<y<3.3, and 0.001<z≦0.5. The phosphor is configured to emit light having a wavelength greater than about 565 nm. In some embodiments, the O-series phosphor has the formula Sr3EuzSiO5. In alternative embodiments the phosphor could be (Ba0.05Mg0.O5Sr0.9)2.7EuzSiO5, or (Ba0.075Mg0.025Sr0.9)3EuzSiO5, or (Ba0.05Mg0.05Sr0.9)3EuzSiO5. In alternative embodiments the phosphor has the formula (MgxSr1-x)yEuzSiO5(CaxSr1-x)yEuzSiO5, and (BaxSr1-x)yEuzSiO5 wherein the values of x and y follow the rules 0<x≦1 and 2.6<y<3.3, and wherein the relationship between y and z is such that y+z is about equal to 3.
As taught by G Blasse et al. in Philips Research Reports Vol. 23, No. 1, pp. 1-120, the host lattice in a phosphor belonging to the system MeSiO5, where Me is either Ca, Sr, or Ba, has the crystal structure (or is related to the crystal structure) Cs3CoCl5. Thus, it is contemplated that the present O-series, orange silicate-based phosphors have a similar host lattice.
To describe the desired amount of activator content, the O-series phosphors may be represented in general by the formula (Sr1-xMx)yEuzSiO5, where the level of the europium activator is described by the “z” parameter, which may range from about 0.001<z<0.5. The effects of including a halogen into the O-series phosphors may be described by embodiments having the formula (M1-xEux)ySiO5H6z. In this embodiment, H is a halogen anion selected from the group consisting of F, Cl, and Br, and the amount of the halogen included in the composition is described again by the parameter “z.” Here, z ranges from 0<z<0.1.
According to the present embodiments, white LED-based illumination systems comprise a self-adjusting smart phosphor composition matched to a wide array of blue/UV emitting sources; a wider array than would have been possible with conventional phosphor packages. An example of a 5 mm range in excitation is from 452.5 nm to 457.5 nm, where the desired chromaticity of the illumination system may be maintained within the narrow range of x±0.01 and y±0.01. The variation of the product illumination on a CE diagram would vary from about 0.300±0.01 for the x value, and the 0.300±0.01 for the y value. Presently, at least 5 bins for every 2.5 nm variation in blue/UV excitation wavelength is required to sort those blue LED chips; and after that, another at least 5 bins in 5 different defined CIE regions would be required to satisfy present white LED needs. Current methods require that in each bin brightness and voltage have to be sorted, so at the end the LED packaging company has 168 bins.
In another embodiment a white LED wafer can be manufactured by coating the novel smart phosphor onto a blue/UV LED wafer containing an array (which may be thousands or more) of blue/UV LED chips whose peak emitting wavelength range is larger than 5 nm (again, using the exemplary range 452.5 nm to 457.5 nm). The CIE (x, y) value of an individual white LED chip produced from such a wafer may be controlled to within in a range of x+0.01 and y+0.01), again in the region of the CIE diagram of 0.300±0.01 for x and 0.300±0.01 for y. It is contemplated that the present technologies are applicable to situations where the variation in blue/UV is more than about 5 nm across the wafer, such as the 10 nm variation present in the industry today.
The present application claims benefit of and priority to U.S. Patent Application No. 60/837,178, titled “Two-phase yellow phosphor with self-adjusting emission wavelength,” filed Aug. 10, 2006, by inventors Yi-Qun Li and Yi Dong. U.S. Patent Application No. 60/837,178 is hereby incorporated by reference in its entirety.
| Number | Date | Country | |
|---|---|---|---|
| 60837178 | Aug 2006 | US |