Patent Application
20140175968
This non-provisional application claims priority under 35 U.S.C. §119(a) on Patent Application No. 2011-281416 filed in Japan on Dec. 22, 2011, the entire contents of which are hereby incorporated by reference.
This invention relates to a yttrium-cerium-aluminum garnet (sometimes referred to as YAG:Ce) phosphor for converting the wavelength of light from a light-emitting element, and a light-emitting device comprising the YAG:Ce phosphor. More particularly, it relates to a particulate YAG:Ce phosphor suited for constructing white light-emitting devices which are used to construct illuminating devices including general illuminating devices, backlight devices and headlamp devices.
Light-emitting diodes (LEDs) are the most efficient among currently available light sources. In particular, white LEDs find a rapidly expanding share in the market as the next-generation light source to replace incandescent lamps, fluorescent lamps, cold cathode fluorescent lamps (CCFL), and halogen lamps. The white LEDs are arrived at by combining a blue LED with a phosphor capable of emission upon blue light excitation. Typically, green or yellow phosphors are combined with blue LEDs to produce pseudo-white light. Suitable phosphors include Y3Al5O12:Ce, (Y,Gd)3(Al,Ga)5O12:Ce, (Y,Gd) 3Al5O12:Ce, Tb3Al5O12:Ce, CaGa2S4:Eu, (Sr, Ca, Ba) 2SiO4:Eu, and Ca-α-SiAlON:Eu.
Among these, the Y3Al5O12:Ce phosphor is most often used because it has a high emission efficiency upon blue light excitation. It is prepared, as disclosed in JP 3700502, for example, by dissolving rare earth elements Y and Ce in a proper stoichiometric ratio in an acid, coprecipitating the solution with oxalic acid, firing the coprecipitate into coprecipitate oxide, mixing it with aluminum oxide, and adding a fluoride (e.g., ammonium fluoride or barium fluoride) as flux thereto. The mixture is placed in a crucible and fired in air at 1,400° C. for 3 hours. The fired material is wet milled in a ball mill, washed, separated, dried, and finally sieved.
For the typical example of Y3Al5O12:Ce phosphor, it is described that its emission color can be shifted to the longer wavelength side by substituting gadolinium for part of yttrium. Undesirably, this substitution is at the sacrifice of the quantum efficiency of emission at room temperature and the emission performance at high temperature.
Patent Document 1: JP 3700502
An object of the invention is to provide a yttrium-cerium-aluminum garnet (YAG:Ce) phosphor which allows emission color to be shifted to the longer wavelength side without substituting gadolinium for part of yttrium and without sacrificing the emission performance at high temperature.
Regarding a yttrium-cerium-aluminum garnet phosphor consisting of crystalline grains as matrix phase, the inventors have found that if nanocrystalline grains having an average grain size of 5 to 20 nm and containing cerium in a higher concentration than the average cerium concentration of the matrix phase are dispersed in the crystalline grains, the phosphor is capable of producing emission color having a x value of 0.47 to 0.54 on the xy chromaticity coordinates when excited with 450 nm light. Also, the peak intensity of emission spectrum at a phosphor temperature of 80° C. is at least 93% of the peak intensity of emission spectrum at a phosphor temperature of 25° C. The invention is predicated on these findings.
In one aspect, the invention provides a yttrium-cerium-aluminum garnet phosphor having a crystallographic texture wherein the crystallographic texture is based on a matrix phase, and nanocrystalline grains having a grain size of 5 to 20 nm and containing cerium in a higher concentration than the cerium concentration of the matrix phase are dispersed in the crystallographic texture.
Typically, the phosphor produces emission color having a x value of 0.47 to 0.54 on the xy chromaticity coordinates when excited with 450 nm light.
Preferably, cerium is present in a concentration of 4 mol % to 15 mol % based on the sum of yttrium and cerium. Also preferably, the cerium concentration of the nanocrystalline grains is 1 to 20% by weight higher than the cerium concentration of the matrix phase.
In a preferred embodiment, the phosphor produces an emission spectrum when excited with 450 nm light, wherein the peak intensity of emission spectrum at a phosphor temperature of 80° C. is at least 93% of the peak intensity of emission spectrum at a phosphor temperature of 25° C.
In another aspect, the invention provides a light-emitting device comprising a light-emitting element for emitting light having a wavelength of 400 to 470 nm and the phosphor, defined above, for converting the wavelength of at least part of light from the light-emitting element.
In the YAG:Ce phosphor of the invention, nanocrystalline grains having a size of 5 to 20 nm and containing cerium in a higher concentration than the cerium concentration of the matrix phase are dispersed in the crystallographic texture. The emission color of the phosphor is shifted to the longer wavelength side than in the prior art phosphors. Since elements other than Y, Ce, and Al are excluded as the main component, the phosphor can maintain its satisfactory emission (or fluorescent) performance even at high temperature.
As used herein, the term “phosphor” refers to a fluorescent substance. The terms “particles” and “powder” are equivalent in that the powder is a grouping of particles.
The yttrium-cerium-aluminum garnet phosphor (including those having part of yttrium substituted by gadolinium; referred to as YAG:Ce phosphor, hereinafter) is one of the phosphors most commonly used to construct white LED owing to its chemical stability, high quantum efficiency, and high emission efficiency attributable to a good match with human visual sensitivity. Many of white LEDs using YAG:Ce phosphor are known as pseudo-white LED. Most of these LEDs use blue LED in combination with YAG:Ce phosphor of yellow emission.
While a choice is made from a variety of pseudo-white LEDs whose emission color has different color temperatures depending on a particular application or purpose, means for changing the color temperature of LED is most often by changing the emission color of YAG:Ce phosphor. In turn, the means for changing the emission color of YAG:Ce phosphor is most often by substituting gadolinium for part of yttrium in YAG:Ce phosphor to change the chromaticity of its fluorescent spectrum.
Specifically, the YAG:Ce phosphor is such that x value on the xy chromaticity coordinates increases as the concentration of cerium or activator in the phosphor increases. However, the method of Patent Document 1 is difficult to incorporate cerium beyond a certain concentration because the ionic radius of cerium is greater than the ionic radius of yttrium (notably, ionic radius Y3+=0.893 Å, Ce3+=1.034 Å). For this reason, the common approach taken to produce YAG:Ce phosphor having a high x value is to substitute gadolinium for part of yttrium.
However, the high x-value YAG:Ce phosphor obtained by substituting gadolinium for part of yttrium has the tendency that as the degree of substitution of gadolinium increases, the emission efficiency of the phosphor near room temperature lowers and the emission intensity at high temperature remarkably drops. The lowering of the emission efficiency of the phosphor leads to a lowering of the emission efficiency of the white LED. The drop of the emission intensity at high temperature allows the color of light emitted by an LED illuminating device to change depending on the LED chip temperature, environment temperature and the like. These properties are undesirable as the phosphor.
Making extensive investigations to improve a lowering of the emission performance at high temperature as found with the YAG:Ce phosphor having part of yttrium substituted by gadolinium while maintaining the shift of emission color to the longer wavelength side unchanged from that of the YAG:Ce phosphor having part of yttrium substituted by gadolinium, the inventors have arrived at the invention. The invention achieves this improvement by providing a YAG:Ce phosphor with the structure that nanocrystalline grains having an average grain size of 5 to 20 nm and containing cerium in a higher concentration than the cerium concentration of the matrix phase are dispersed in the crystallographic texture. The phosphor with this structure can achieve a chromaticity x value equivalent to that of the YAG:Ce phosphor having part of yttrium substituted by gadolinium, without incorporating gadolinium. Furthermore, the YAG:Ce phosphor of the invention exhibited excellent temperature performance in that when the emission peak intensity was measured by keeping it at temperatures of 25° C. and 80° C. and exciting with 450 nm light, the emission peak intensity at the phosphor temperature of 80° C. was at least 93% of the emission peak intensity at the phosphor temperature of 25° C.
Now the YAG:Ce phosphor of the invention will be described in detail.
The inventors actually prepared YAG:Ce phosphors using the method of Patent Document 1. Gadolinium-free YAG:Ce phosphors, when excited with 450 nm light, were difficult to produce emission color with a x value of at least 0.47. To manufacture YAG:Ce phosphors capable of producing emission color with a x value of at least 0.47, it was necessary to substitute gadolinium for part of yttrium.
With the method of Patent Document 1, cerium as an activator cannot be incorporated beyond a certain concentration, because the method relies on a solid-phase reaction where YAG:Ce phosphor forms through a relatively slow crystal growth process. There is a strong tendency that cerium having a large ionic radius is expelled out of the crystallographic texture of YAG:Ce phosphor (or excreted out of the phosphor composition).
Then, the inventors attempted to produce YAG:Ce phosphors by rapidly melting and solidifying a YAG:Ce phosphor composition to form particles without affording a sufficient time for cerium to be excreted out of the phosphor composition, and causing crystal growth at high temperature. When the chromaticity of the resulting YAG:Ce phosphors was measured, the x value increased as the concentration of charged cerium in the raw material increased, as shown in
The crystallographic texture of the YAG:Ce phosphor was analyzed under a transmission electron microscope (TEM), finding that nanocrystalline grains containing cerium in a higher concentration than the YAG:Ce crystalline matrix (referred to as “matrix phase,” hereinafter) are dispersed in the crystallographic texture. As used herein, the term “nanocrystalline grains,” also known as nanocrystals, refers to ultrafine crystal grains of nanometer order. The size of nanocrystalline grains is measured from TEM structural analysis, and given as a diameter of the minimum circle circumscribing a nanocrystalline grain under examination, for example.
The structure that nanocrystalline grains having a high cerium concentration are dispersed in the matrix phase was not observed in the YAG:Ce phosphors synthesized by the method of Patent Document 1. Also, even when YAG:Ce phosphors were synthesized by the same method as the invention, the distribution of nanocrystalline grains having a high cerium concentration in the matrix phase was not observed in those YAG:Ce phosphors wherein the concentration of charged cerium relative to the entire rare earth elements was up to 3 mol %. From these results, it was concluded that the distribution of nanocrystalline grains in the matrix phase is a characteristic structure obtained when a phosphor is synthesized according to the invention from the composition having a charged cerium concentration of at least 4 mol % relative to the entire charged rare earth elements. It is thus believed that by providing YAG:Ce phosphor with such a structure (crystallographic texture), YAG:Ce phosphor containing cerium in a high concentration of at least 4 mol % relative to the entire rare earth elements can be synthesized.
In the YAG:Ce phosphor of the invention, the size of cerium-rich nanocrystalline grains dispersed in the matrix phase varies with the composition thereof, especially the concentration of charged cerium relative to the entire rare earth elements, and other preparation conditions, and has a certain distribution. The size is typically in a range from 5 nm to 20 nm. If nanocrystalline grains are of too small size, the cerium concentration may not be so high. Also, if nanocrystalline grains are of too large size, it is difficult to maintain the crystalline phase in the YAG:Ce phosphor.
Preferably, the nanocrystalline grains having a high cerium concentration are distributed in the matrix phase as uniformly as possible.
The cerium concentration of the nanocrystalline grains (dispersed phase) and the matrix phase was measured by the energy-dispersive x-ray spectroscopy under transmission electron microscope (TEM-EDX), finding that the concentration of cerium contained in the nanocrystalline grains is higher than the concentration of cerium contained in the matrix phase. While the cerium concentration of the matrix phase is governed by the composition of the YAG:Ce phosphor, the nanocrystalline grains have a cerium concentration which is 1.01 to 3.00 times greater than that of the matrix phase as long as the composition is in the range of the invention. Differently stated, the cerium concentration of the nanocrystalline grains is 1 to 20% by weight higher than the cerium concentration of the matrix phase.
Although the nanocrystalline grain-forming mechanism is not well understood, the following is presumed. In the process of preparing a phosphor according to the invention, as an amorphous composition containing cerium in a large amount which is difficult to be introduced in essentially crystalline YAG:Ce alloys progressively crystallizes, cerium is excreted from the matrix phase everywhere throughout the crystallographic texture, and collects at micro-domains interspersed in the crystallographic texture. Consequently, nanocrystalline grains are formed as an alloy phase having a high cerium concentration dispersed throughout the crystallographic texture.
The YAG:Ce phosphor of the invention is represented by the compositional formula (1), for example.
YaCebAlcOd (1)
Herein a and b are preferably in the range: 0.04≦b/(a+b)≦0.15, more preferably 0.04≦b/(a+b)≦0.10. Specifically, the cerium concentration is controlled to 4 to 15 mol %, preferably 4 to 10 mol % based on the sum of yttrium and cerium. If b/(a+b) is less than 0.04, then an equivalent x value on the xy chromaticity coordinates may be obtainable by the prior art YAG:Ce synthesis method without resorting to the inventive method and without adding gadolinium. If b/(a+b) exceeds 0.15, then it may be difficult for the YAG:Ce phosphor to maintain the garnet phase. It is noted that in formula (1), a+b=3, 5.0≦c≦5.5, and 12≦d≦12.75.
The chromaticity of emission color of the phosphor can be adjusted by changing the cerium concentration (concentration of charged cerium relative to charged yttrium). As the cerium concentration increases from 4 mol % to 15 mol %, the x value of chromaticity increases. When excited with 450 nm light, the phosphor produces emission color having a x value of at least 0.47, specifically 0.47 to 0.54 on the xy chromaticity coordinates. It is noted that the resulting phosphor is free of a phase other than the garnet phase, for example, an alumina phase.
Described below is the temperature performance of the YAG:Ce phosphor of the invention. As used herein, the term “phosphor temperature” refers to the temperature of an ambient atmosphere surrounding the phosphor. YAG:Ce phosphors were prepared according to the invention so that they might produce emission color with a x value of 0.47 to 0.54. These phosphors produced an emission spectrum when excited with 450 nm light. The peak intensity (P80) of emission spectrum at a phosphor temperature of 80° C. was measured. Also the peak intensity (P25) of emission spectrum at a phosphor temperature of 25° C. was measured. The peak intensity ratio (P80/P25) was at least 93%.
Also empirically, phosphors having an equivalent x value to the inventive YAG:Ce phosphor were prepared by the method of Patent Document 1 and by substituting gadolinium for part of yttrium. For the phosphor having any x value, the peak intensity ratio (P80/P25) was inferior to (or lower than) that of the inventive YAG:Ce phosphor having an equivalent x value.
In the future, LED devices will become of larger size and higher power. Then the LED device generates more heat whereby the device is at a high temperature, giving rise to a problem that phosphor performance is degraded. The problem is overcome by the present invention providing a YAG:Ce phosphor having improved fluorescent performance at high temperature over the YAG:Ce phosphor prepared by the prior art method of substituting gadolinium for part of yttrium.
It is now described how to prepare a YAG:Ce phosphor. According to the invention, the YAG:Ce phosphor is prepared by rapidly melting and cooling a phosphor composition raw material to form a YAG:Ce phosphor composition in amorphous state, and treating it for crystallization.
The YAG:Ce phosphor composition in amorphous state resulting from quenching/solidification can contain cerium in a higher concentration than the Gd-free YAG:Ce phosphor which is prepared by the solid-phase method. This is because the YAG:Ce phosphor composition in amorphous state has a distance between atoms constituting the composition which is wider than in the crystal of the same composition. Then the composition containing much cerium ions having a greater ionic radius than yttrium ions does not possess the function to expel cerium ions out of the composition. The inventors have empirically confirmed that the YAG:Ce phosphor composition in amorphous state can contain cerium in a proportion of up to 15 mol % to substitute for part of yttrium.
The phosphor raw material is obtained by mixing yttrium, aluminum and cerium compounds which include oxides, hydroxides, organic acid salts, and mineral acid salts. Of these, oxides and hydroxides are preferable for cost and ease of handling. The raw material is in particulate form which preferably has as small a particle size as possible from the standpoint of obtaining phosphor particles of uniform composition. The compounds as the raw material have an average particle size of not greater than 1 μm. Yttrium, cerium and aluminum compounds are combined so as to provide a predetermined molar ratio of Y, Al and Ce to the phosphor composition. For example, the compounds are combined such that a cerium concentration is 4 to 15 mol % based on the entire rare earth elements, and a molar ratio of aluminum to the sum of yttrium and cerium is 5/3 to 5.5/3.
The raw material as mixed may be granulated into particles having a certain particle size which is dependent on the particle size of the final phosphor. For example, the raw material is granulated into particles having an average particle size of 5 to 100 μm, preferably 10 to 65 μm. Granulation techniques include tumbling granulation, spray drying, and dry pulverization/classification. A proper technique may be selected as long as the final phosphor of the desired particle size is available. A dispersant may be added for the purpose of improving the mixed state of the raw material prior to granulation. Further, a binder may be added for the purpose of facilitating binding of particles during granulation. In this case, the granulated powder is fired to remove the binder.
The phosphor raw material (or granulated powder) is melted in a high-temperature atmosphere and rapidly cooled, yielding the YAG:Ce phosphor composition in amorphous state. More specifically, the particles as granulated to an average particle size of 5 to 100 μm are melted in a high-temperature plasma. The melting temperature of the phosphor raw material may be at least 2,500° C., preferably at least 4,000° C., and more preferably at least 10,000° C. The cooling temperature may be around room temperature, and the atmosphere is preferably air or nitrogen atmosphere.
Immediately after exiting the plasma, the molten particles are rapidly cooled into spherical particles. The size of the outgoing spherical particles substantially corresponds to the size of the granulated particles. That is, spherical particles having an average particle size of 5 to 100 μm are recovered. The spherical particles thus recovered are less crystalline or amorphous (i.e., YAG:Ce phosphor composition in amorphous state).
The YAG:Ce phosphor composition in amorphous state is then heat treated, yielding a crystalline YAG:Ce phosphor. The temperature of heat treatment should preferably be 900 to 1,700° C., more preferably 1,200 to 1,650° C., and even more preferably 1,400 to 1,600° C. Temperatures below 900° C. are insufficient to promote crystal growth in particles, resulting in a phosphor having a low emission efficiency. Temperatures above 1,700° C. may cause particles to be fused together. The heat treatment atmosphere is preferably a reducing atmosphere, for example, an atmosphere of argon or nitrogen in admixture with hydrogen.
Prior to the heat treatment in a high-temperature atmosphere, cerium is distributed substantially uniform in the particle interior. After conversion of the particles to a highly crystalline YAG:Ce phosphor by the heat treatment in a high-temperature atmosphere, substantially the entirety of cerium is retained within the phosphor particles. Through the heat treatment step, nanocrystalline grains are formed in the matrix phase of YAG:Ce phosphor particles. Specifically, nanocrystalline grains are dispersed in the matrix phase of the YAG:Ce phosphor texture.
On X-ray diffraction (XRD) analysis, the phosphor thus obtained is identified to be yttrium-cerium-aluminum garnet.
The YAG:Ce phosphor of the invention is suited as a phosphor for converting the wavelength of light from a light-emitting element to construct a light-emitting device or light-emitting diode, especially as a phosphor to construct warm-color white LED. The particulate YAG:Ce phosphor of the invention is advantageously used in a light-emitting diode, and an illuminating device, backlight device or the like may be fabricated therefrom.
A further embodiment of the invention is a light-emitting device comprising the YAG:Ce phosphor defined as above and a light-emitting element for emitting light having a wavelength of 400 to 470 nm. They are coupled such that at least part of the light from the light-emitting element is wavelength converted (e.g., converted to white light) by the YAG:Ce phosphor. The particulate phosphor of the invention is suited for converting the wavelength of light from a light-emitting element to construct a light-emitting diode. The particulate phosphor of the invention is advantageously used in a light-emitting diode, and an illuminating device, backlight device or the like may be fabricated therefrom. Using the phosphor for wavelength conversion of part of light from blue LED, a warm-color white LED device which is not achievable with the prior art YAG:Ce garnet phosphor can be manufactured.
Examples are given below by way of illustration and not by way of limitation.
A yttrium oxide powder having a purity of 99.9 wt % and an average particle size of 1.0 μm, an aluminum oxide powder having a purity of 99.0 wt % and an average particle size of 0.5 μm, and a cerium oxide powder having a purity of 99.9 wt % and an average particle size of 0.2 μm were mixed to form 1,000 g of a powder mixture having a molar ratio of Y/Al/Ce=2.88/5.00/0.12. The powder mixture was combined with 1,500 g of deionized water, 10 g of ammonium polyacrylate, and 2 g of carboxymethyl cellulose, and milled in a ball mill for 6 hours. Using a two-fluid nozzle, the resulting slurry was granulated into particles having an average particle size of 15 μm. The particles were heat treated in air at 1,000° C. for 2 hours to burn out the organic matter.
An RF induction thermal plasma system was used. The particles were passed through the argon plasma where they were melted and then solidified, obtaining spherical particles. On qualitative analysis by X-ray diffractometer (XRD), the spherical particles were found to be amorphous composite.
The spherical particles were heat treated in 1 vol % hydrogen-containing argon gas at 1,350° C. for 5 hours, yielding phosphor particles.
With respect to this crystallographic texture, the cerium content was measured by EDX at a spot having a beam diameter of about 10 nm in the TEM images from three different fields of view as shown in
When excited with 450 nm light (i.e., light having a peak at wavelength 450 nm), the phosphor particles emitted light whose chromaticity had x=0.474 on the xy chromaticity coordinates as measured by chromaticity measuring system Model QE1100 (Otsuka Electronics Co., Ltd.).
Also, the phosphor was kept at a temperature of 25° C. or 80° C. by heating. The emission spectrum of the phosphor at the temperature of 25° C. or 80° C. upon excitation with 450 nm light was measured by a spectrometer Model FP6500 (JASCO Corp.). The peak intensities of these emission spectra were compared. Provided that the peak intensity at the phosphor temperature of 25° C. was 100, the peak intensity at the phosphor temperature of 80° C. was 97.5.
A yttrium oxide powder having a purity of 99.9 wt % and an average particle size of 1.0 μm, an aluminum oxide powder having a purity of 99.0 wt % and an average particle size of 0.5 μm, and a cerium oxide powder having a purity of 99.9 wt % and an average particle size of 0.2 μm were mixed to form 1,000 g of a powder mixture having a molar ratio of Y/Al/Ce=2.79/5.50/0.21. The powder mixture was combined with 1,500 g of deionized water, 10 g of ammonium polyacrylate, and 2 g of carboxymethyl cellulose, and milled in a ball mill for 6 hours. Using a spray drier, the resulting slurry was granulated into particles having an average particle size of 20 μm. The particles were heat treated in air at 1,500° C. for 2 hours to burn out the organic matter.
An RF induction thermal plasma system was used. The particles were passed through the argon plasma where they were melted and then solidified, obtaining spherical particles. On qualitative analysis by XRD, the spherical particles were found to be amorphous composite.
The spherical particles were heat treated in 1 vol % hydrogen-containing argon gas at 1,500° C. for 4 hours, yielding phosphor particles.
The crystallographic texture of these phosphor particles was observed under TEM. Nanocrystalline grains dispersed in the crystallographic texture (matrix phase) were seen. The nanocrystalline grains had a size of 5 to 10 nm.
When excited with 450 nm light, the phosphor particles emitted light whose chromaticity had x=0.501 on the xy chromaticity coordinates as measured by chromaticity measuring system Model QE1100 (Otsuka Electronics Co., Ltd.).
Also, the phosphor was kept at a temperature of 25° C. or 80° C. by heating. The emission spectrum of the phosphor at the temperature of 25° C. or 80° C. upon excitation with 450 nm light was measured as in Example 1. The peak intensities of these emission spectra were compared. Provided that the peak intensity at the phosphor temperature of 25° C. was 100, the peak intensity at the phosphor temperature of 80° C. was 93.7.
99.9 wt % pure yttrium nitrate, 99.0 wt % pure aluminum nitrate, and 99.9 wt % pure cerium nitrate were mixed in a molar ratio of Y/Al/Ce=2.85/5.30/0.15 and dissolved in water to form 10 L of a 0.25 mol/L solution. To the solution, 20 L of 0.5 mol/L aqueous ammonia was slowly added, obtaining about 2 kg of hydroxide mixture.
The hydroxide mixture was combined with 5,000 g of deionized water, 30 g of ammonium polyacrylate, and 50 g of carboxymethyl cellulose, and milled in a ball mill for 6 hours. Using a spray drier, the resulting slurry was granulated into particles having an average particle size of 20 μm. The particles were heat treated in air at 1,500° C. for 2 hours to burn out the organic matter.
An RF induction thermal plasma system was used. The particles were passed through the argon plasma where they were melted and then solidified, obtaining spherical particles. On qualitative analysis by XRD, the spherical particles were found to be amorphous composite.
The spherical particles were heat treated in 1 vol % hydrogen-containing argon gas at 1,500° C. for 4 hours, yielding phosphor particles.
The crystallographic texture of these phosphor particles was observed under TEM. Nanocrystalline grains dispersed in the crystallographic texture (matrix phase) were seen. The nanocrystalline grains had a size of 5 to 10 nm.
When excited with 450 nm light, the phosphor particles emitted light whose chromaticity had x=0.485 on the xy chromaticity coordinates as measured by chromaticity measuring system Model QE1100 (Otsuka Electronics Co., Ltd.).
Also, the phosphor was kept at a temperature of 25° C. or 80° C. by heating. The emission spectrum of the phosphor at the temperature of 25° C. or 80° C. upon excitation with 450 nm light was measured as in Example 1. The peak intensities of these emission spectra were compared. Provided that the peak intensity at the phosphor temperature of 25° C. was 100, the peak intensity at the phosphor temperature of 80° C. was 96.5.
A yttrium oxide powder having a purity of 99.9 wt % and an average particle size of 1.0 μm, an aluminum oxide powder having a purity of 99.0 wt % and an average particle size of 3.0 μm, and a cerium oxide powder having a purity of 99.9 wt % and an average particle size of 0.2 μm were mixed to form 1,000 g of a powder mixture having a molar ratio of Y/Al/Ce=2.85/5.00/0.15. To the powder mixture was added 200 g of barium fluoride as flux. After thorough mixing, the mixture was placed in an alumina crucible and heat treated in an atmosphere of 2 vol % hydrogen and 98 vol % argon at 1,400° C. for 4 hours. The fired product was washed with water, separated and dried, obtaining phosphor particles.
The phosphor particles were observed under an electron microscope. The particles were polyhedral, with crystal faces perceived.
The crystallographic texture of the phosphor particles was observed under TEM. As seen from
When excited with 450 nm light, the phosphor particles emitted light whose chromaticity had x=0.460 on the xy chromaticity coordinates. The x value was low although the raw material had the same composition as in Example 1.
A yttrium oxide powder having a purity of 99.9 wt % and an average particle size of 1.0 μm, a gadolinium oxide powder having a purity of 99.9 wt % and an average particle size of 1.0 μm, an aluminum oxide powder having a purity of 99.0 wt % and an average particle size of 3.0 μm, and a cerium oxide powder having a purity of 99.9 wt % and an average particle size of 0.2 μm were mixed to form 1,000 g of a powder mixture having a molar ratio of Y/Gd/Al/Ce=2.058/0.882/5.00/0.06. To the powder mixture was added 200 g of barium fluoride as flux. After thorough mixing, the mixture was placed in an alumina crucible and heat treated in an atmosphere of 2 vol % hydrogen and 98 vol % argon at 1,400° C. for 4 hours. The fired product was washed with water, separated and dried, obtaining phosphor particles.
The phosphor particles were observed under an electron microscope. The particles were polyhedral, with crystal faces perceived.
The crystallographic texture of the phosphor particles was observed under TEM. No nanocrystalline grains were observed in the crystallographic texture.
When excited with 450 nm light, the phosphor particles emitted light whose chromaticity had x=0.477 on the xy chromaticity coordinates, indicating a chromaticity approximately equal to Example 1.
Also, the phosphor was kept at a temperature of 25° C. or 80° C. by heating. The emission spectrum of the phosphor at the temperature of 25° C. or 80° C. upon excitation with 450 nm light was measured as in Example 1. The peak intensities of these emission spectra were compared. Provided that the peak intensity at the phosphor temperature of 25° C. was 100, the peak intensity at the phosphor temperature of 80° C. was 91.4.
A yttrium oxide powder having a purity of 99.9 wt % and an average particle size of 1.0 μm, a gadolinium oxide powder having a purity of 99.9 wt % and an average particle size of 1.0 μm, an aluminum oxide powder having a purity of 99.0 wt % and an average particle size of 3.0 μm, and a cerium oxide powder having a purity of 99.9 wt % and an average particle size of 0.2 μm were mixed to form 1,000 g of a powder mixture having a molar ratio of Y/Gd/Al/Ce=2.058/0.882/5.00/0.12. To the powder mixture was added 200 g of barium fluoride as flux. After thorough mixing, the mixture was placed in an alumina crucible and heat treated in an atmosphere of 2 vol % hydrogen and 98 vol % argon at 1,400° C. for 4 hours. The fired product was washed with water, separated and dried, obtaining phosphor particles.
The phosphor particles were observed under an electron microscope. The particles were polyhedral, with crystal faces perceived.
The crystallographic texture of the phosphor particles was observed under TEM. No nanocrystalline grains were observed in the crystallographic texture.
When excited with 450 nm light, the phosphor particles emitted light whose chromaticity had x=0.500 on the xy chromaticity coordinates, indicating a chromaticity approximately equal to Example 2.
Also, the phosphor was kept at a temperature of 25° C. or 80° C. by heating. The emission spectrum of the phosphor at the temperature of 25° C. or 80° C. upon excitation with 450 nm light was measured as in Example 1. The peak intensities of these emission spectra were compared. Provided that the peak intensity at the phosphor temperature of 25° C. was 100, the peak intensity at the phosphor temperature of 80° C. was 90.3.
Japanese Patent Application No. 2011-281416 is incorporated herein by reference.
Although some preferred embodiments have been described, many modifications and variations may be made thereto in light of the above teachings. It is therefore to be understood that the invention may be practiced otherwise than as specifically described without departing from the scope of the appended claims.
