TWI298348B - - Google Patents

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TWI298348B
TWI298348B TW95106939A TW95106939A TWI298348B TW I298348 B TWI298348 B TW I298348B TW 95106939 A TW95106939 A TW 95106939A TW 95106939 A TW95106939 A TW 95106939A TW I298348 B TWI298348 B TW I298348B
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powder
light
phosphor
temperature
heterojunction
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TW95106939A
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TW200734442A (en
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Naum Soschine
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1298348 * ▲ 九、發明說明: 【發明所屬之技術領域】 本發明係«於-種自光二極體之螢光粉及其製作方法,、 • 扣一種白光二極體之螢光粉,其色溫在Τ=12000〜25〇(ρκ 、 ' Ά小角度為發散度6 —12度角上,光強很高,此時異質奸 ' W導電觸點處於異質結背面之白光二極體之螢騎及其製作^ 法。 ’、 魯【先前技術】 現今由於半導體技術的進步,半導體照明技術得到了快速的 發展。主要表現在發明了各種細和讀來储所有的電真空燈 泡1在用於照明目的主要是生產白光二極體。在這些發光= 體中異質社要是氮化銦、氮化鎵,其波長小勝475⑽。藍色 或其它短波與螢光粉無機_粒相互侧,螢光粉細小的顆粒被 • 均句分佈到聚合薄膜上,聚合薄膜從異質結各個發光面將其圍 繞。短波光線穿透透明聚合物塗層達到塗於聚合物表面的榮光粉 顆粒層。這樣,就發生以下的物理現象: - 螢光粉顆粒使短波散射; - 螢光粉顆粒吸收光線; - 以螢光形式再次放射。 再-人發射的波長更長螢光粉輪射與最初的短波光線混合,形 成完整統一的光線,其顏色和色調近于標準白光,色溫在Τ=2800 1298348 ^ 鼻 -KKWK之間。以上三駐要現象的規律現在已經廣為認知 了。這樣最初的光線散射與螢光粉的分佈面積成正比,即,跟它 們的大小成正比。同時,光散射與發射到螢光粉顆粒光上的波長 成反比,這就造成了,由半導體異質結發射的短波會比它們發射 的長波散射強度更強。 第二個光學現象-螢光粉對光的吸收取決於物質能量區的能 量構造,能量區強烈的吸收初次發射的能量,這是由吸收系數值k > 決定的。吸收係數是根據穿透特定厚度材料後殘餘輻射幾兩測定 的。這種關係式為J=J0e-kd,其中J和J0分別是光通過厚度為d 鍍層的最後和初始強度。固體物質的強烈吸收與螢光粉物質能量 區的構造相關。如果該物質擁有禁區Eg的寬度超過2電子伏特, 那麼類似的物質對可見光的輻射吸收不是很強烈。在螢光粉材料 吸收係數相同的情況下,k=5000 CM-1螢光粉粒度直徑為(1=10 微米=1χ10·3釐米吸收超過50%的發射到螢光粉顆粒上的第一 > 次輻射光。 在初次短波輻射與螢光粉發生的相互作用過程中產生的第三 個光學現象是發螢光現象。被吸收的初次輻射能量激發位於螢光 粉顆粒中心的催化劑的内部能量水準。在激發内部水準之後,處 於執函數3d和4f的初始狀態的電子轉移到更為高能狀態的位 置’此時催化劑原子沒有離子化。這種狀態的被激發電子的生命 週期不長,一般為1 X KT3 — 1 X 10-6秒,此後被激發電子與處於 1298348 催化劑下層的小孔進行發射性再組合過程。此時催化劑中心螢光 化現象的特點是激發螢光粉主光線和它發射光線之間 的「池位 移」’還有1子輸出。如果初始值即「池位移」,一般等於δ=12〇_15〇 nm ’那麼量子輸出一般很少超過作〇 8。 發射光和激發光的能量之間的數量關係可以表示為W流fW 紐· λ絲/λ魏· γ。在w紐=110 mw/ mm2情況下,為了標準配置藍 光二極體和長波黃光螢光粉,等式W㈣=10x470/580x0.8=6.4 mW/mm ’這個等式表示螢光功率密度約為6 4mW/mm2,這保證 了發光一極體發光党度超過10000燭光/mm2。類似的白光發光二 極體用於作為發明類似用處的在1999年授予Shimizu等人之美國 專利第5,998,925號中有描述。與該專利相符合,在白光二極體的 二進位放射中使用鋁釔鈽螢光粉,其成分為Y3Al5〇i2.Ce,以細粉 末的形式塗在由氮化鎵氮化銦異質結表面。 根據前述專利資料其螢光粉末的顆粒粒度在〇」_1〇微米,比 如,以懸浮物的形式存在於二氧化矽氣溶膠或者環氧樹脂中在異 質結輕射表面形成很厚塗層。在直流電下發光二極體發射白光, 其色溫T=2800 —10000 °K,光強1〇 —15濁光,發光角度2Θ = 6°。儘管合成白光的光強值相當高,但是這個技術方案有眾所周 知的缺陷,即合成白光的不均勻性。這種現象反應在通過光學棱 鏡將發光二極體發光投射到光散射屏上時,會形成藍、藍-綠色和 頁-綠色同心圓。最大可此是,這種合成白光的散射成幾種組成色 1298348 1 4 办的現象疋m為異質結的初始藍絲射實際上很少被榮光粉散 射正因如此通過焦點平面而不偏離中心轴心。同時,榮光賴射 以自發光線的形式從每個螢光粉顆粒發射出來,這些光線在各個 角度都有這些不同角度的光線在發光二極體輸出棱鏡上聚焦很 μ弱。所以在巾心聚無自光的幾個組成顏色和初始的藍、黃榮 光輻射之間的比例關係即刻失衡。這樣在投射到白色榮幕上時就 丨產生色譜分散彩色圖像。類似圖像稱為效果「虹」現象。 前述美國第5,998,925號專利力圖修正各個發明層次上技術方 案的問題。此外,另一個美國第6351〇69 B1號專利(2/2〇〇2授予 Lowery等人),在此列為本發明之參考原型專利。根據這個專利, 為了排除不同光線的分散現象,在發光二極體螢光粉轉換輻射器 的成分中增加了這些分散性物質,如高分散的Si〇2或Ti〇2。由 於在螢光粉顆粒中存在大量上述物質顆粒初始的短波藍光輕射發 生多次散射。輻射的部分激發螢光粉顆粒長波光激發光,當輻射 其它在空間中有不同方向的部分,穿過光學棱鏡組成合成白光, 並在這種情況下沒有形成「熱點」(即更亮)之藍色亮點。發光二極 體合成白光的類似的各種色調更為廣泛,這些可以由眾多的美國 專利前案來證明,比如美國第6340824B1號專利,第6361192B1 號專利,第6501100B1號等專利,以及已經提交的美國第 2002/0084745A1號專利申請案。與所有這些專利相一致,都採用 非常細小分散螢光粉顆粒與光學分散劑顆粒相結合,比如Si〇2或 12983481298348 * ▲ IX. Description of the Invention: [Technical Field of the Invention] The present invention relates to a fluorescent powder of a self-photodiode and a method for producing the same, and a fluorescent powder of a white light diode, the color temperature thereof In Τ=12000~25〇(ρκ, ' Ά small angle is divergence 6-12 degree angle, the light intensity is very high, at this time heterogeneous 'W conductive contact is on the back of the heterojunction white light diode flash ride And its production ^ method. ', Lu [previous technology] Nowadays, due to the advancement of semiconductor technology, semiconductor lighting technology has been rapidly developed. It is mainly manifested in the invention of various fine and read to store all the electric vacuum light bulb 1 for lighting The main purpose is to produce white light diodes. In these luminescence = body, the heterogeneous society should be indium nitride or gallium nitride, and its wavelength is better than 475 (10). Blue or other short wave and phosphor powder inorganic _ grain side, the fluorescent powder is small The particles are distributed onto the polymeric film by a uniform sentence, and the polymeric film surrounds each of the light-emitting surfaces of the heterojunction. The short-wave light penetrates the transparent polymer coating to reach the layer of luminescent powder particles coated on the polymer surface. Physical phenomena: - Fluorescent powder particles cause short-wave scattering; - Fluorescent powder particles absorb light; - Re-radiate in the form of fluorescence. - Human-emitting wavelengths longer. Fluorescent powders are mixed with the original short-wave light to form Complete and uniform light, its color and hue are close to standard white light, and the color temperature is between Τ=2800 1298348 ^ nose-KKWK. The law of the above three resident phenomena is now widely recognized. Thus the initial light scattering and phosphor powder The distribution area is proportional to, that is, proportional to their size. At the same time, the light scattering is inversely proportional to the wavelength of the light emitted onto the phosphor particles, which causes the short waves emitted by the semiconductor heterojunction to be emitted compared to them. The long-wave scattering intensity is stronger. The second optical phenomenon - the absorption of light by the phosphor depends on the energy structure of the energy region of the material, and the energy region strongly absorbs the energy emitted for the first time, which is determined by the absorption coefficient value k >. The absorption coefficient is determined according to the residual radiation after passing through a specific thickness of material. This relationship is J=J0e-kd, where J and J0 are the last of the light passing through the thickness of d plating. Initial strength. The strong absorption of solid matter is related to the structure of the energy region of the phosphor material. If the material has a width of the forbidden zone Eg exceeding 2 electron volts, the similar material absorbs visible light radiation is not very strong. In the case where the absorption coefficients are the same, the particle size diameter of k = 5000 CM-1 phosphor powder is (1 = 10 μm = 1 χ 10 · 3 cm and absorbs more than 50% of the first > secondary radiation emitted onto the phosphor particles. The third optical phenomenon that occurs during the interaction between the initial short-wave radiation and the phosphor is the fluorescing phenomenon. The absorbed primary radiant energy excites the internal energy level of the catalyst at the center of the phosphor particle. After the level, the electrons in the initial state of the functions 3d and 4f are transferred to the position of the more energetic state 'At this time, the catalyst atoms are not ionized. The life cycle of the excited electrons in this state is not long, generally 1 X KT3 - 1 X 10-6 seconds, after which the excited electrons are recombined with the small holes in the lower layer of the 1298348 catalyst. At this time, the phosphorescence phenomenon of the catalyst center is characterized by exciting the "pool shift" between the chief ray of the phosphor powder and the light it emits, and a sub-output. If the initial value is "pool displacement", which is generally equal to δ = 12 〇 _15 〇 nm ′ then the quantum output generally rarely exceeds 〇 8. The quantitative relationship between the energy of the emitted light and the excitation light can be expressed as W-flow fW New λ 丝 / λ Wei · γ. In the case of wNEW = 1010 mw/mm2, for standard configuration of blue diode and long-wave yellow phosphor, the equation W (four) = 10 x 470 / 580 x 0.8 = 6.4 mW / mm ' This equation indicates that the fluorescence power density is about 6 4mW/mm2, which guarantees that the luminous one-pole luminous party exceeds 10,000 candelas/mm2. A similar white light-emitting diode is described in U.S. Patent No. 5,998,925, issued to Shimizu et al. In accordance with the patent, an aluminum bismuth phosphor is used in the binary radiation of the white light diode, and its composition is Y3Al5〇i2.Ce, which is applied as a fine powder on the surface of the gallium nitride indium nitride heterojunction. . According to the aforementioned patent data, the particle size of the phosphor powder is in the range of 〇 〇 〇 micrometers, for example, in the form of a suspension in the cerium oxide aerosol or epoxy resin to form a very thick coating on the light-emitting surface of the heterojunction. Under direct current, the light-emitting diode emits white light, and its color temperature is T=2800-10000 °K, the light intensity is 1〇15, and the light-emitting angle is 2Θ=6°. Although the intensity of the synthesized white light is quite high, this technical solution has a well-known defect that the white light is not uniform. This phenomenon reflects the formation of blue, blue-green and page-green concentric circles when the light-emitting diodes are projected onto the light-scattering screen by optical prisms. The maximum is that the scattering of this synthetic white light into several constituent colors 1298348 1 4 The phenomenon of 疋m is the initial blue filament of the heterojunction is actually rarely scattered by the glory powder. Therefore, the focus plane is not deviated from the center. Axis. At the same time, the glare beam is emitted from each of the phosphor particles in the form of self-illuminating lines, which have different angles of light at various angles that are very weakly focused on the output prism of the LED. Therefore, the proportional relationship between several constituent colors of the towel core and the initial blue and yellow radiance is immediately unbalanced. This produces a chromatographically dispersive color image when projected onto a white glory. A similar image is called the effect "rain" phenomenon. The aforementioned U.S. Patent No. 5,998,925 seeks to revise the technical solutions at various inventive levels. In addition, another U.S. Patent No. 6,351,69 B1 (2,2,2, issued to Lowery et al.) is incorporated herein by reference. According to this patent, in order to eliminate the dispersion of different light rays, these dispersing substances such as highly dispersed Si〇2 or Ti〇2 are added to the composition of the light-emitting diode phosphor conversion radiator. Since the presence of a large amount of the above-mentioned substance particles in the phosphor powder particles, the initial short-wave blue light emission causes multiple scattering. The part of the radiation excites the long-wavelength excitation light of the fluorescent powder particles. When radiating other parts with different directions in space, the optical prisms are combined to form a white light, and in this case, no "hot spots" (ie, brighter) are formed. Blue highlights. Light-emitting diodes synthesize white light in a variety of similar shades, which can be demonstrated by numerous US patents, such as U.S. Patent No. 6,340,824 B1, U.S. Patent No. 6,361,192 B1, No. 6,501,100 B1, and U.S. Patent Application No. 2002/0084745A1. Consistent with all of these patents, very finely dispersed phosphor particles are combined with optical dispersant particles such as Si〇2 or 1298348.

Ti〇2或A!N,這樣可以使白光無色調截面達到非常穩定,色溫 T=2800 —6000°K。類似結構發光的光強可以達到κ 15_16燭 光。儘管類似的儀器被大量運用,但是它們有著嚴重的缺陷:這 • 些結構的小角度光強非常低。這樣即使通過使用特殊棱鏡可以從 ' 異質結表面產生光強燭光的白光,這對於在特殊信號設備, 比如鐵路L號4上使用結構斋也是不夠的。這種發光二極體與大 φ 角度光學結構結合的設計不能使光流值達到Φ^2-4流明,這樣當 然是不足以用來作為經濟照明的,誠屬美中不足之處。 【發明内容】 為解決上述習知技術之缺點,本發明之主要目的係提供一種 白光發光二極體之螢光粉,其在GaN•應異質結的基礎上設計白 光二極體’該設計會有很高的甚至非常高的白光小角度光強數 值’具體會是公4〇濁光。 # P本么月之另目的在於創建發光結構,該結構可以保障複製 白光和先前給定的光色調。㈣的這些色調可能屬於暖白光,冷 白光,月光白。 表、> ^發日月之另一目的在基於祕__異質結創建全白光流量的 么光結構’比如㈣流明。類似的發光元件可以用於生產特種發 光源。 盆為達上述之目的’本發明之—種白光發光二極體之榮光粉, -係由氮化鎵氮化銦半導體異f結而成,魏射波長小於㈣ 1298348 nm ,’褒備由乳备鑄基,鋪催化的多棱面大粒度分散榮光粉,其 光碏轉換器通用方程式為Gd3-x-y-zYxLuyCezAlp〇q,其中該化學指 數變動如下·· L〇<x<2.6, 0.0001 取0.5, 〇 〇购成5, 4^:3曰 -q=4.5+1.5*p,區別在於該螢光粉為大顆粒分散的單晶,多棱主要 : 是六面體形,六面體有兩個相互平行的基面,由12___, • 這些邊相互成9〇 -150。角,螢光粉顆粒内切圓的半徑在6 _ 12 籲 微米之間,兩個基面的高度距離在4-10微米之間,同時這種多 棱顆粒直接與異質結鋪正面和四個端面進行光學接觸,並覆蓋 異質結光表面20 - 85%面積,發光表面與螢光粉顆粒轉換發出 的波長λ超過560nm的長波光一起構成合成白光,其色溫在 卜12_ - 2500〇K之間,在小角度為發散度6 —12度角上, 光強很高,此時異質結的導電觸點處於異質結背面。 為達上述之目的’本發明之—種白光二極體螢絲之製作方 鲁法’其包括下列步驟:先枰取如下⑽,^^及Αΐ2〇3 氧化物若干4 ;取联干濃度之Ce_3)3水雜;將秤取之氧化 物王數加入Ce(NG3)3水溶液巾’並狀充分混合;將充分混合之 尺容液置人)t、箱巾乾㉖’得混合粉末;在混合粉末内添加若干量 之NajO4、KsSO4和邱〇4粉末後充分混合,再將混合粉末放入 石央坩辦;將;5糾細^麟離職之氣餘雜巾,以特定 速度升溫至第-溫度,並以此溫度鋪第—_後私等速度升 /嚴至第一/置度,以此溫度保持第二時間後再以等速度升溫至第三 !298348 1 他度,以此溫度保持第三時間後再以等速度降溫至室溫取出;將 取出之粉末用硝酸和磷酸清洗未反應之物質,然後用大量清水重 複清洗至中性為止;以及將清洗後之粉末置入烘箱中乾燥,乾燦 後即得螢光粉產品。 【實施方式】 簡單闡述本發明之物理學實質。首先提出兩個圖表(請參照表 _1和备2),其中展示了光通過螢光粉塗層到異質結表面的情形。 這種情況下,表_1給出了由標準分散分佈和大小的螢光粉顆粒製 成的塗層。從表_1得出結論,塗層是由單個大粒徑的螢光粉及其 燒結物構成並且在填充厚度上是不均⑽。縣之間的空間由許 常細小的螢光粉顆粒覆蓋,這種情況下,由於螢光粉小顆粒可以 在高度上職迭加,這樣就構成了鮮塗層高度微米。由細 小螢光粉末構成的類似厚度的塗層位於沒有規則形狀的大顆粒骜 光粉顆粒或顆粒燒結物表。由於在原型中使用的螢光粉顆粒的高 度分散性,所以不能在攝影或光學轉換時對其進行精確聚焦。顯 然,類似的散射的擴散性是細小顆粒發射的螢光的特性。被標準 螢光粉覆蓋的異質結的自由表面部分不會超過5或職,這嚴重 限制了異質結初始短波輻射輸出。 給定的初始藍光和螢光粉長波光_互義平均〇· G5:〇· 95 - 0.1:0.9決定了合成白光的顏色,合成白光在標準原型設計 中處於暖白光區域,顏色座標在泛〇 35於〇 37至犯Ti〇2 or A!N, which makes the white light-free cross section very stable, and the color temperature T=2800-6000°K. The light intensity of a similar structure can reach κ 15_16 candle. Although similar instruments are used in large numbers, they have serious drawbacks: These structures have very low light intensity at small angles. Thus, even by using a special prism, it is possible to generate a white light of a strong candle from the surface of the heterojunction, which is not enough for the use of a structural fast on a special signal device such as the railway L number 4. The combination of such a light-emitting diode with a large φ angle optical structure does not allow the optical flow value to reach Φ^2-4 lumens, which is of course insufficient for economical illumination, and is a drawback. SUMMARY OF THE INVENTION In order to solve the above disadvantages of the prior art, the main object of the present invention is to provide a white light emitting diode phosphor powder, which is designed with a white light diode based on a GaN heterojunction. There is a very high or even very high white light small angle light intensity value 'specifically it will be public 4 turbid light. The other purpose of #P本月月 is to create a light-emitting structure that guarantees the reproduction of white light and the previously given light tones. (4) These shades may belong to warm white light, cool white light, and moonlight white. Table, > ^ Another purpose of the sun and the moon is to create a white light flow based on the secret __ heterojunction, such as (four) lumens. Similar illuminating elements can be used to produce special light sources. The pot is the glory powder of the white light-emitting diode of the present invention, which is formed by an indium-bonded indium nitride semiconductor, and the wavelength of the Wei-ray is less than (4) 1298348 nm, 'prepared by milk Prepared base, catalyzed multi-faceted large-grain dispersion glory powder, the general formula of the pupil converter is Gd3-xy-zYxLuyCezAlp〇q, wherein the chemical index changes as follows: · L〇 < x < 2.6, 0.0001 0.5, 〇〇 purchased into 5, 4^: 3曰-q=4.5+1.5*p, the difference is that the phosphor powder is a single crystal dispersed by a large particle, and the multi-edge is mainly: a hexahedron, a hexahedron has two The mutually parallel base faces are 12___, • these sides are 9〇-150 to each other. The radius of the inscribed circle of the fluorinated powder particles is between 6 _ 12 and the height of the two bases is between 4 and 10 microns, and the multi-edge particles are directly bonded to the front and four The end face is optically contacted and covers 20 - 85% of the area of the heterojunction light surface, and the light-emitting surface and the long-wavelength light of the wavelength λ exceeding 560 nm converted by the phosphor powder particles constitute a synthetic white light, and the color temperature thereof is between 12 and 2500 〇K. At a small angle of divergence of 6-12 degrees, the light intensity is high, and the conductive contacts of the heterojunction are at the back of the heterojunction. For the purpose of the above-mentioned 'the white light-emitting diode filament of the present invention', the method of the invention includes the following steps: first taking the following (10), ^^ and Αΐ2〇3 oxides 4; taking the dry concentration Ce_3)3 water miscellaneous; the number of oxides taken from the scale is added to the Ce(NG3)3 aqueous solution towel and mixed well; the well-mixed tolerant liquid is placed in the human) t, the box towel is dried 26' to obtain a mixed powder; Add a certain amount of NajO4, KsSO4 and Qiuqi 4 powder to the mixed powder, mix well, and then put the mixed powder into the Shiyang 坩 ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; - Temperature, and spread the temperature at this temperature - _ after the private speed rise / strict to the first / set, the temperature is maintained for the second time and then warmed to the third at the same speed! 298348 1 other degrees, this temperature After the third time, the temperature is lowered to room temperature and taken out at a constant speed; the unreacted material is washed with nitric acid and phosphoric acid, and then washed repeatedly to neutral with a large amount of water; and the washed powder is placed in an oven. Dry, dry, and then get the fluorescent powder product. [Embodiment] The physical essence of the present invention will be briefly explained. First, two charts (see Table _1 and Preparation 2) are presented, which show how light is applied to the surface of the heterojunction through the phosphor powder. In this case, Table_1 gives a coating made of phosphor powder particles of standard dispersion distribution and size. From Table_1, it was concluded that the coating consisted of a single large particle size phosphor and its sinter and was uneven in fill thickness (10). The space between the counties is covered by very small fluorescent powder particles. In this case, since the small particles of the phosphor powder can be superimposed on the height, the thickness of the fresh coating layer is micrometer. A coating of similar thickness consisting of fine phosphor powder is located in a large particle size powder particle or particle sintered form having no regular shape. Due to the high degree of dispersion of the phosphor particles used in the prototype, it is not possible to precisely focus it during photographic or optical conversion. Obviously, the diffusivity of similar scattering is characteristic of the fluorescence emitted by fine particles. The free surface portion of the heterojunction covered by the standard phosphor does not exceed 5 or the position, which severely limits the initial short-wave radiation output of the heterojunction. Given initial blue and luminescent powder long-wavelength _ 互 〇 〇 · G5: 〇 · 95 - 0.1: 0.9 determines the color of synthetic white light, synthetic white light in the standard prototype design in the warm white light area, color coordinates in the ubiquitous 35 Yu 〇37 to commit

11 1298348 之間。在_情況下,即可以實縣要是自光帶有暖色,但已知 的由鬲分散螢光粉小顆粒塗層製成的發光二極體設計還有重要的 缺陷。 由螢光粉顆粒和以銦和鎵的異質結為基礎,使用建議本發明 中的高分散螢光粉的大容量棱形顆粒的螢光粉塗層看上去是完全 不一樣的’在塗層上可以看到大粒的、板狀—塔形顆粒,覆蓋在 異質結的輻射面。螢光粉顆粒的外切直徑平均在6_12微米或更 大。本發明巾使用大顆粒分散螢光_絕大多數顆粒擁有是棱 形,多數六面體形狀。棱面光環,沒有明顯的粗糙不平,所以來 自晶體的輻射主要是小角度一般不超過衫2〇。,根據方程式 cp=arctg(ni/n2),得出,這裏ηι是空氣折射係數,m是榮光粉材 料折射係數雛縣錢綠射由平㈣棱面和顆 粒正面表面形成’財常明亮、沒有散射的光學綺和反射形式。 因為如此,大顆粒螢光粉發射的螢光光線在方向上非常接近輸出 棱鏡的光學軸心’該軸心將來自螢絲層的輻射引出,在這=情 況下’長波光線很好的脫離二極體表面,在很小的發散度上形成 藍光(短波)和黃光(長波)級的均色光束。這樣在^二極體 中就沒有大量以分散#jTi〇2顆粒或者無規則粉狀榮光 存在散射光h ’這樣就消除了二極體機射的多次擴散性散^ 現象。 在多倍電子賴鏡下,本發明制放大圓倍_催化的紹— 12 1298348 ::基的早個大顆粒螢光粉顆粒圖像。圖像顯示,顆粒為六面體 柱,棱面兩邊都為梯形棱面,梯形棱面相互之間以9〇 —⑽。 每^交Γ互平行的_棱面分別與梯形棱面相交,分別組成 ^顆軸正絲面。主錢絲紅是騎料絲,被激發 $化丨心«結_波光線也是通過這録面發射出來。再 ^曰出’每也可以從表_2直觀的看出,每個規則單晶顆粒的背面 =:光!度與異質結發射面直接光學接觸。在形成大顆粒 乙:層…廷些表面之間可能會有部分很稀薄透明聚合物 2早讀軌下的絲_衫辟,㈣輻射和蘇赫也 不會消失。 β魏則螢光粉覆蓋異質表面的部分,可以從表_2得出,可能 ^不樣的’比如,20-85%的異質結輻射表面被螢光粉顆粒覆 :相應地20-85%的短波藍光僅僅穿透規則晶體的松疏層形成 口光。這種短波光功率可以用兩個等式來表示:Wb=(w⑹ 〜γ)γΒ(ΐ Sy)fc,其中第—個被加部分是通過松疏孔的初始藍光, 弟二個被加數表示了沒有被規則螢光粉吸收的藍光部分。這種情 =乘積αιγ)-龍以質結额=射所需轉,γΒ_異質結外 心子輕射輸出,Sy-異質被規則螢光粉覆蓋的部分,螢光粉對 初始藍光輻射吸收係數為RB。 每個螢光粉雕將初始激發藍光轉換成黃色魏,成功獲得藍光 相當的大神分’料WPKUy)YB(卜&>λΒ/λ♦,⑽符號符合 1298348 { ► 螢光粉光輕射等量流明數值的時候,其中補充指數、和、表示 半導體異質結和螢光粉最大光譜波長。 被集中到棱鏡外部,二極體的合成白光的強度非常大。這個 . 數值在光學上被稱為光強,一般用J=d<D/d〇)表示並按凱德拉測量 • (燭光)’到達被精確測量的光發散角(根據光強在特定輻射角度的 " 一半衰弱值)。 又 • 纟此過財本發明得知,所使_三極難縣強非常高。 ^表-1中列出了與相應顏色座標對應絲強數值。應該指出本發 明所使用的二極體光強超過商業標準光強4一5倍。如果對標準的: =體=試驗二極體進行輻射輪㈣度數位對比,那麼在光強上的 區別疋· J/J3T=l〇9. 25/12. ο X 6Vi〇2=109· 25/12 X 36/100=3. 6。 表〜1Between 11 1298348. In the case of _, it can be that the county has a warm color from the light, but the known light-emitting diode design made of the 鬲 dispersed fluorescent powder small particle coating has important defects. Based on the phosphor powder particles and the heterojunction of indium and gallium, the phosphor powder coating using the large-capacity prismatic particles suggesting the highly dispersed phosphor powder of the present invention appears to be completely different in the coating. Large, plate-tower-shaped particles can be seen covering the radiating surface of the heterojunction. The outer diameter of the phosphor particles is on average 6 to 12 microns or larger. The inventive towel uses large particles to disperse the fluorescing - most particles possess a prismatic, mostly hexahedral shape. The prismatic aura has no obvious roughness, so the radiation from the crystal is mainly small angles generally not exceeding 2 inches. According to the equation cp=arctg(ni/n2), it is concluded that ηι is the air refractive index, m is the refractive index of the glory powder material, and the young green money is formed by the flat (four) facet and the front surface of the particle. The optical enthalpy and reflection form of the scattering. Because of this, the fluorescent light emitted by the large particle phosphor is very close in the direction of the optical axis of the output prism. The axis extracts the radiation from the filament layer. In this case, the long-wave light is well separated. The surface of the polar body forms a blue (short wave) and yellow (long wave) level uniform light beam with a small divergence. Thus, in the ^ diode, there is not a large amount of scattered #jTi〇2 particles or random powdery glory, and scattered light h' eliminates the phenomenon of multiple diffusion of the diode. Under the multiple electron spectroscopy, the present invention produces a magnified circle-catalyzed image of the early large particle phosphor powder particles of the base 12 12298348. The image shows that the particles are hexahedral columns, and the sides of the facet are trapezoidal facets, and the trapezoidal facets are 9〇(10). The _ facets that are parallel to each other intersect with the trapezoidal facets to form a positive axis of the axis. The main money silk red is riding the wire, which is excited. The 丨 丨 heart « knot _ wave light is also emitted through this recording surface. Further, it can be seen from Table 2 that the back side of each regular single crystal particle =: light degree is directly in optical contact with the heterojunction emitting surface. In the formation of large particles B: layer ... between the surface of some of the surface may be very thin transparent polymer 2 under the early reading of the wire - shirt, (four) radiation and Sukh will not disappear. The part of β-Wei fluorescent powder covering the heterogeneous surface can be obtained from Table_2, which may be different. For example, 20-85% of the heterojunction radiation surface is covered by the phosphor powder: correspondingly 20-85% of the short wave The blue light only penetrates the loose layer of the regular crystal to form the mouth light. This short-wavelength optical power can be expressed by two equations: Wb=(w(6) ~γ)γΒ(ΐ Sy)fc, where the first added portion is the initial blue light through the loose hole, and the second is added. Indicates the portion of the blue light that is not absorbed by the regular phosphor. This kind of emotion = product αιγ) - dragon with mass balance = shot required to turn, γ Β _ heterojunction outer core light shot output, Sy-heterogeneous part covered by regular phosphor powder, fluorescent powder for initial blue light radiation absorption coefficient For RB. Each fluorescent powder carving converts the initial excitation blue light into yellow Wei, and successfully obtains the blue light equivalent of the big god 'WPKUy' YB (Bu &>λΒ/λ♦, (10) symbol conforms to 1298348 { ► Fluorescent powder light shot When the lumen value is equal, the index, sum, and the semiconductor heterojunction and the maximum spectral wavelength of the phosphor are added. The concentration of the synthesized white light of the diode is very large. This value is optically called For light intensity, generally denoted by J=d<D/d〇) and according to Kadella measurement • (candle light)' to reach the accurately measured light divergence angle (according to the light intensity at a specific radiation angle " half weak value) . In addition, this invention has been known to have a very high level of strength. ^ Table-1 lists the wire strength values corresponding to the corresponding color coordinates. It should be noted that the intensity of the diode used in the present invention exceeds the commercial standard light intensity by a factor of four to five. If the standard: = body = test diode is irradiated (four) degree digital comparison, then the difference in light intensity 疋 J / J3T = l 〇 9. 25 / 12. ο X 6Vi 〇 2 = 109 · 25 /12 X 36/100=3. 6. Table 1

12983481298348

28 598 4 92.75 0.25 0.2 99 286 5 105.27 0.30 0.3 63 051 6 89.43 0.25 0.2 37 141 7 81.83 0.29 0.2 01 758 8 89. 03 0.27 0.2 95 600 9 109. 25 0.25 0.2 48 169 10 95. 28 0.30 0.2 10 921 11 12.0 0.30 0.3 晶體電流40mA 0 異質結的面積 12 81.18 0. 32 0.3 S=0. 2x0. 3 mm2 69 395 輻射角度 13 84. 88 0. 35 0.3 2Θ=10°商業規 48 799 格28 598 4 92.75 0.25 0.2 99 286 5 105.27 0.30 0.3 63 051 6 89.43 0.25 0.2 37 141 7 81.83 0.29 0.2 01 758 8 89. 03 0.27 0.2 95 600 9 109. 25 0.25 0.2 48 169 10 95. 28 0.30 0.2 10 921 11 12.0 0.30 0.3 crystal current 40 mA 0 area of heterojunction 12 81.18 0. 32 0.3 S=0. 2x0. 3 mm2 69 395 radiation angle 13 84. 88 0. 35 0.3 2Θ=10° commercial gauge 48 799 grid

15 129834815 1298348

、知用大驗螢光粉後,二極體在光強上的大幅度提高可能是 因為採用新的發光二極體設計結構。 本發明所_發光二極體光強上的巨大優勢在於是異質結是 直角平行六面體各個面的比例是1:1:〇· i到1:2:〇· 12,而以基礎 面與異質結輻射©接朗大縣螢光粉的高與齡投射内切半徑 的比例是1:3 —1:1,在高度為最佳的6-8微米的情況下,如 此保證了在初始藍光和第二次發射的黃-橙黃合献巾由於和色 座標 x=0 ’ 2548 y=0,2169 至 χ=〇,363 y=0,351 大量均勻混合, 所以;又有發生玉間上的光分離(選擇)並形成光的短波中心區。 在結構上發光二極體的主要是氮化銦,氮化鎵基與單晶SiC 或藍寶石底板上構成的異質結。在平面圖上異質結是長方形邊的 比例為1:2到1:1· 5並在異質結長方形最小一面的外延薄膜厚 度疋0· 1 — 0· 12幾何尺寸。異質結導電引線可以有幾種設計方 1298348 案,在本發明中係採用分級接觸設計,正負極處於外延薄板一面。 在這種情況下,對於InN層和p—觸點之間有一個特殊面,從n—層After knowing that the fluorescent powder is used, the significant increase in the light intensity of the diode may be due to the new light-emitting diode design. The great advantage of the light intensity of the light-emitting diode of the present invention is that the heterojunction is a ratio of each surface of the rectangular parallelepiped is 1:1: 〇·i to 1:2: 〇·12, and the base surface and Heterojunction radiation © the ratio of the high-intensity projection inscribed radius of the granitic powder of Langda County is 1:3 -1:1, which guarantees the initial blue light in the case of the best height of 6-8 microns. And the second-launched yellow-orange-yellow towel is uniformly mixed due to the color coordinates x=0 ' 2548 y=0, 2169 to χ=〇, 363 y=0,351, so there is a jade between The light separates (selects) and forms a short-wave center region of the light. The structure of the light-emitting diode is mainly a heterojunction composed of indium nitride, gallium nitride based and single crystal SiC or sapphire substrate. In the plan view, the heterojunction is a rectangular side with a ratio of 1:2 to 1:1·5 and a thickness of the epitaxial film on the smallest side of the heterojunction rectangle 疋0·1 — 0·12 geometry. Heterojunction conductive leads can be found in several designs 1298348. In the present invention, a graded contact design is used, with the positive and negative electrodes on one side of the epitaxial sheet. In this case, there is a special face between the InN layer and the p-contact, from the n-layer

GaN外延20-40微米。上電極直接和氮化鎵層接觸。此刻,螢光粉 顆粒覆蓋GaN異質結外部表面,並位於環繞異質結端平面的接觸 級上。 在本發明中,異質結輻射表面面積為2〇〇χ3〇〇微米可能覆蓋 有300 — 750單個大顆粒螢光粉,其截面(或顆粒内切圓)直 徑在6 — 24微米之間,這時每個規則顆粒的高度不超過6 一 8 微米。 必須指出的是,直接與異質結輻射表面接觸的榮光粉顆粒, 在螢光粉層相對於異質結輕射平面的各個方向上沒有形成多層覆 蓋,這肯定會反應在光結構輸出強度上。 合成白光光譜由兩個主要波段構成,兩者強度_取決於異質結 輻射表面㈣絲絲接_覆蓋練度。根據合成光計算出的 顏色座標值在X在G.28 - 0.42之間變動,隨著Q 3〇 — 0.44之間變動。必須指出的是,在已知變動範圍内有已知的合成 白光方案’比如冷自光、暖自光,能量囉的白色。 螢光粉是立體晶體結構。與已知的化合物表巾資料通用分子 ' 才目付&在過私中’我們瞭解,所有螢光粉顆粒擁有Pnm 空間群的域晶聽構,這與已知化合物表#料通用公式祕心 相符合:Ce,係屬於礦物型化合物。根據本發明之資料,榮光粉GaN is epitaxially 20-40 microns. The upper electrode is in direct contact with the gallium nitride layer. At this point, the phosphor particles cover the outer surface of the GaN heterojunction and are located at the level of contact around the plane of the heterojunction junction. In the present invention, the heterojunction radiation surface area of 2 〇〇χ 3 〇〇 micrometer may cover 300 - 750 single large particle fluoresce powder, the cross section (or granule inscribed circle) diameter is between 6 - 24 microns, then The height of each regular particle does not exceed 6 to 8 microns. It must be pointed out that the glare powder particles that are in direct contact with the heterojunction radiation surface do not form a multi-layer coating in all directions of the phosphor layer relative to the heterojunction light-emitting plane, which will certainly be reflected in the light structure output intensity. The synthetic white light spectrum consists of two main bands, the intensity of which depends on the heterojunction radiation surface (4) wire bonding _ coverage training. The color coordinate value calculated from the synthesized light varies between X and G.28 - 0.42, and varies with Q 3〇 - 0.44. It must be pointed out that there are known synthetic white light schemes within known variations, such as cold self-light, warm self-light, and energy white. Fluorescent powder is a three-dimensional crystal structure. With the known compound tablecloth data, the general molecule 'has been paid & in the private" 'we understand that all the phosphor powder particles have the domain crystal structure of the Pnm space group, which is related to the known compound table. Consistent: Ce, is a mineral compound. According to the information of the present invention, glory powder

17 1298348 物質的晶體格柵參數在a=12.1A — 12·21Α之間變動。這種變動 取決於螢光粉成份中的並部分替換螢光基本的釔離子的Gd離子 數量。這種陽離子節點中的γ+3離子被稀土 Gd+3替換是同價替換, 不需要通過往物質晶體格栅中導入補償物質進行其它補償變化。 往螢光粉物質晶體柵格中加入Gd離子可以提高螢光粉晶體的折射 係數,從原來的初始成分為YALOaCe的初始值η=ι· 92,提高到 新的成分〇(1^15〇12心的11=1.99-2.00。在螢光粉成分中一定量 的紀離子被錄離子無變化替換之後螢光粉物質的折射係數也會達 到很南的值。 通過向螢光粉成分中加入鐺、離子可以增強其黃綠色彩,這同 時還加強了螢光粉對氮化鎵氮化銦異質結的初次輻射的大量吸 收。如螢光粉顆粒與充滿氮化Ga_In-N的異質接平面之間有光學 接觸那麼輻射輸出角,即接近1〇。。螢光粉物質折射 增長指數從η=1·92到η=2·0,使異質結外表面直接輸出角度降 低’但同時異f結錢絲雜之間的光學細區的輻射輸出增 大。螢光粉輻射穿過異質結,提高了發光二極體總的光輸出。 這種補充輻射由於通過使用Frenel棱鏡而消除,這使得螢光 可以聚焦。為了將來自螢光粉顆粒的紐成形,最後加入有機聚 合物特殊分散介質,折射係數為V吐45_155。這種有機聚合物 塗層可起光收集ϋ作用,這樣螢光粉顆粒表面光輸出角度可以增 大到φ-45。’這可以提高螢光粉輻射收集到達8〇_9〇。並在實際上17 1298348 The crystal grid parameter of a substance varies between a = 12.1A and 12.21Α. This variation depends on the amount of Gd ions in the phosphor component that partially replaces the fluorescent base ions. The replacement of the γ+3 ion in the cation node by the rare earth Gd+3 is a parity replacement, and there is no need to perform other compensation changes by introducing a compensation substance into the material crystal grid. Adding Gd ions to the crystal lattice of the phosphor powder material can increase the refractive index of the phosphor powder crystal, and increase the initial composition of the original YAROACe from η=ι·92 to the new composition (1^15〇12). The heart's 11=1.99-2.00. After a certain amount of ion in the phosphor component is replaced by the recorded ion without change, the refractive index of the phosphor powder material will reach a very south value. By adding 铛 to the phosphor component The ions can enhance the yellow-green color, which also enhances the large absorption of the primary radiation of the gallium nitride indium nitride heterojunction by the phosphor powder, such as the phosphor particles and the heterojunction plane filled with the nitrided Ga_In-N. The optical output angle is then close to 1 〇. The refractive index of the phosphor powder is from η=1·92 to η=2·0, which reduces the direct output angle of the outer surface of the heterojunction 'but at the same time The radiation output of the optical fine area between the money filaments increases. The phosphor powder radiates through the heterojunction, increasing the total light output of the light-emitting diode. This supplementary radiation is eliminated by using the Frenel prism, which makes the firefly Light can be focused. In order to be from Firefly The formation of the powder particles is finally formed by adding a special dispersion medium of the organic polymer, and the refractive index is V_45_155. The organic polymer coating can act as a light collecting enthalpy, so that the surface light output angle of the phosphor powder particles can be increased to φ- 45. 'This can increase the collection of fluorescent powder radiation to reach 8〇_9〇. And in fact

18 1298348 沒有光學損失。 數在發^巾同萌_ ’觀所錢絲齡平面的螢光總 18 ’此時所有的平面和棱面發射均句螢光。激發螢光 :=?_子輪出很好的被藍光吸收。根據本發明之測量大 •化與杰八二0/°(甚至更高)°顯然’更高的量子輸出與螢光粉的 予刀相符,螢光粉中有相當部分的紀被乳和鑄替換。對於這 •材料縣特點S激發光學波長反射係數關係曲線有更小 二曰曰體形式的絲材料在光學上是透_,岭的黃綠色正如 X月中展7F的樣’是由螢光粉成分中吸收波段的催化劑離子 決定的。 在加入IL離子和_子過程中發生的螢光粉矩陣内部晶體場 的變化不僅僅提高了螢光粉物質的折射係數,同時也增強了其吸 收I曰此日守,在榮光粉材料吸收波譜和異質結輕射發生最佳的 • 光學匹配,以異質結輕射的半寬度為入〇,5=35 -45 !1111。榮光粉中加 的矣曰離子使其吸收波譜擴展到短波區域,因此為了激發榮光粉 知用更為合適的短波發光二極體,與波長為λ=45〇脑相比。這樣, 在本發明中使用了短波Ga-InN發光二極體,波長λ=445肺或更 短這些一極體與本發明之螢光粉的結合保證了很高的光流值和 光輸出。 如上所述,已知的工業用的螢光粉,比如日本和美國公司生 產的系列螢光粉不能滿足本發明的需要,這樣螢光粉顆粒是破碎18 1298348 No optical loss. The number of the radiant light in the plane of the hair 同 ’ ‘ 所 钱 钱 钱 钱 钱 钱 钱 此时 此时 此时 此时 此时 此时 此时 此时 此时 所有 所有 所有 所有 所有 所有 所有 所有 所有Excitation of fluorescence: =?_ The sub-round is well absorbed by the blue light. According to the measurement of the present invention, it is clear that the higher quantum output is consistent with the phosphor powder, and a considerable portion of the phosphor powder is cast and cast. replace. For this material county characteristic S excitation optical wavelength reflection coefficient relationship curve has a smaller diterpene form of the silk material is optically transparent _, ridge yellow green as X month in the exhibition 7F sample is made of fluorescent powder The composition of the absorption band of the catalyst ion is determined. The change in the crystal field inside the phosphor powder matrix that occurs during the addition of IL ions and _ sub-processes not only increases the refractive index of the phosphor powder material, but also enhances its absorption. This is the absorption spectrum of the glory powder material. The best optical matching with a heterojunction light shot, with a half-width of the heterojunction light shot, 5=35 -45 !1111. The strontium ions added to the glory powder extend the absorption spectrum to the short-wavelength region, so a more suitable short-wavelength light-emitting diode is known for exciting the glory powder, compared with the wavelength λ=45 camphor. Thus, in the present invention, a short-wave Ga-InN light-emitting diode is used, and the combination of the wavelength of λ = 445 lungs or shorter and the phosphor of the present invention ensures a high optical flow value and light output. As described above, known industrial phosphor powders, such as a series of phosphor powders produced by companies in Japan and the United States, do not satisfy the needs of the present invention, so that the phosphor powder particles are broken.

19 1298348 的,不具備自然的晶體多棱’其中包括大量平行平面,異質結短 波輕射從—面應通過這些平面被吸收,長波螢光從另-面穿過。 此^ ’對工業級的螢光粉進行的電子顯微鏡研究表明,它們表面 覆盍大量弧坑、彎曲及痕跡,鱗螢絲財的,卫業生產的最 後工序是球賴械粉碎滾H螢絲表面品肢根據反射係 數值R來檢測的。螢光粉稱量(〜觸毫克)將其在光源A下曝 光直到將8G%投制其表_光線反㈣去。如果對本發明的榮 光粉進行類似測試,那麼其反射係數下降至55%。在少量榮光粉 稱:!:光線反應係數區別會更明顯。 重要的是由於絲表面光散射現象雜螢光粉量子輸出是不 一樣的。這樣,對於鮮工#產品來說螢光量子輸出不會超過 咬5〇%,本發明之有規則晶體多棱面的螢光粉的量子輸出值 ° _的區別的-個可能的原因就是’本發明採用的發光 二極體含有帶棱㈣光粉,從自己12_16 (一般14)表面的量子輸 出超過85%,㈣粉化學成分的化學方程式為:u LuyCezAlpOq,其中的化學指數變動如下··〗〇<χ<2 6, 〇.〇_鱗5, 0.0撕⑽5, 4.7姐3,㈣訊々,保證了 ^光粉強烈的長波黃-橙黃發光,波長在平均U=53()〜595邮, 最大半寬度λ〇,5=110〜130mn,並隨著螢光粉中Gd離子含量的增 加而提高。 本發明中_還注意到上述陽離子對螢光粉性能的影響。首 20 1298348 先,釔離子保證對螢光粉晶體格柵主要催化離子ce+3八面體形式 包園。釔和鈽陽離子在幾何形狀上的區別不是很大(τγ=〇·97Α Tc’l.〇4A) ’正因如此遵循了形成固態溶液主要結晶學原理。釓離 子TGd=0.95A的引入提高了晶體内電場梯度,如此可以大幅度提高 Ce離子内光照發光。鐺離子是非常小的(Tlu=〇85A)半徑,可以 穩定螢光粉晶體格栅並可能降低其在向鋁_釔_釓中引入催化大顆 粒離子鈽Ce+3的過程中產生的機械強度。 I 螢光粉顆粒缺乏機械強度同時伴隨得到它們自然的多棱面, 因為眾所周知,組成複雜化合物的成分的幾何尺寸的非補償性同 日π疋伴其晶體或者微晶體表面深斷口、斷層突起或凹口。複 雜化合物晶體形狀必定伴隨脆性、降低的顯微硬度、酸洗劑中的 快速溶解等等。 在本發明中,催化離子Ce+3的能量配置有兩個主要標準2Fi/2 和兮於,都是Ce+3離子主要電場分解狀態牝…、6)。被激發的 離子狀悲項5d(5s25p6)產生蜆化的項%,位於螢光粉電介質 Gd3-x-y-zYxLuyCezAlpOq禁區導電區底部〜〇·9電子伏特處。%可 月匕刀解冰留在離能量水準最低的位置超過2·6電子伏特,並在傳 導區鈍化,因此實際上並沒有發生Ce+3狀態的下層4f電子位移, 因而,並沒有產生用於激發的補充能量消耗。19 1298348, does not have a natural crystal polygon ‘which includes a large number of parallel planes, the heterojunction short-wave light from the surface should be absorbed through these planes, long-wave fluorescence from the other side. This electron microscopy study of industrial grade phosphor powders shows that they have a large number of craters, bends and traces on the surface, and the scales are flamboyant. The final process of Weiye production is the ball smashing and rolling H-ray. The surface product is detected based on the reflection coefficient value R. Fluorescent powder weighing (~ touch milligrams) exposes it to light source A until 8G% is applied to the table _light counter (four). If the glare powder of the present invention is similarly tested, its reflection coefficient is reduced to 55%. In a small amount of glory powder said:!: The difference in light response coefficient will be more obvious. What is important is that the quantum output of the phosphor powder is different due to the light scattering phenomenon on the silk surface. Thus, for the Xiangong# product, the fluorescence quantum output does not exceed 5咬%, and the quantum output value of the regular crystal polygonal surface of the present invention has a difference of - _ the possible reason is 'this The light-emitting diode used in the invention contains a ribbed (four) light powder, and the quantum output from the surface of itself 12_16 (general 14) exceeds 85%. (4) The chemical formula of the chemical composition of the powder is: u LuyCezAlpOq, wherein the chemical index changes as follows. 〇<χ<2 6, 〇.〇_scale 5, 0.0 tear (10)5, 4.7 sister 3, (four) 々, guarantees the strong long-wave yellow-orange luminescence of the light powder, the wavelength is on the average U=53()~595 The maximum half width λ〇, 5=110~130mn, increases with the increase of Gd ion content in the phosphor powder. In the present invention, the influence of the above cations on the properties of the phosphor powder is also noted. First 20 1298348 First, the cesium ion guarantees the main catalytic ion ce+3 octahedral form of the fluorescent powder crystal grid. The difference in geometry between the ruthenium and osmium cations is not very large (τ γ = 〇 · 97 Α Tc'l. 〇 4A) ‘the reason why the main crystallographic principle of forming a solid solution is followed. The introduction of the cesium ion TGd=0.95A increases the electric field gradient in the crystal, which can greatly improve the illumination in the Ce ion. The erbium ion is a very small (Tlu=〇85A) radius, which stabilizes the phosphor powder crystal grid and may reduce its mechanical strength during the introduction of catalytic large particle ions 钸Ce+3 into aluminum_钇_釓. . I. Fluorescent powder particles lack mechanical strength and are accompanied by their natural polygonal faces, as it is well known that the geometrical dimensions of the constituents of complex compounds are uncompensated with the same day π疋 with deep fractures of the crystal or microcrystal surface, fault protrusions or Notch. The crystal shape of the complex compound must be accompanied by brittleness, reduced microhardness, rapid dissolution in the pickling agent, and the like. In the present invention, the energy configuration of the catalytic ion Ce+3 has two main criteria, 2Fi/2 and 兮, which are the main electric field decomposition states of Ce+3 ions 、..., 6). The excited ionic sadness 5d (5s25p6) produces a % of deuteration, which is located at the bottom of the conductive region of the fluorescent powder dielectric Gd3-x-y-zYxLuyCezAlpOq, which is ~ 〇·9 eV. % can be used to release ice from the lowest energy level above 2·6 eV, and passivated in the conduction zone, so there is actually no electron displacement of the lower layer 4f in the Ce+3 state. Therefore, it does not produce Supplemental energy consumption for excitation.

Ce離子狀31¾2和2d之間的主要能量轉換需要激發量子 hV=2·7電子伏的能量消耗,這符合被吸收光的波長λ=457ηιη。此 21 1298348 1 n 時電子池位移實際上是可能性最小地,因為發射光波長在2姑5/2 位移等於卜525削。類似由於發散光波長引起的12%的低值電子 池位移是螢光發光中_魏象。在本發明之顧巾已知主要 波長為入=457贈的被吸收的光可能會因為向榮光粉成分中加入 Lu+3離子發生短波位移,錢絲中Lu+3離子含量_最佳值的 時候波長為λ,譲。在螢光粉基質中加入Gd+3軒可以將吸收 ,長提高λ=477ηη!。該水準〜〇.4電子伏的寬度對2〇主要激發狀 Μχ生的發光過财影響。這個水準的寬度位於距離物質傳導區 〇.9電子伏的位置,造成輕射量子波長上的極大差異。在這種情況 下短波波長在λ=51〇 — 565聰之間,而長波最高可以達到 λ=680^700 nm,發光最大波長可以達到λ=59〇腿。正如上面顯示 的Ce離子發光狀態上的能量多樣性使得它實際上是再現可見光 譜中黃、撥黃、紅、甚至深紅區域唯—必需的。這是使用半導體 異質結和螢光粉來製造最佳白光組合光學結構所需要的。的確, 如果異質結短波光譜最大值在1445 nm __ 475腿之間,即, △—3〇nm,那螢光粉再次輻射發光光譜最大值可達到心65 nm,這 滿足了為了獲得平衡白光的對黃、橙黃和紅光輻射的必需條件。 本發明注意到主要催化劑Ce+3離子的濃度對螢光粉發光光譜 性能有影響。如果引入Ce+3離子濃度最低並處於〇尬碰〇2之 間’那麼_$光粉發光光譜半紐為^11()11111。_螢光粉成 刀中的Ce+3離子劑量增大’當含量z=〇〇5時,輻射光譜半寬度增 22 1298348 加到 Δ=120ηιη,如 ζ=0·1,那麼 Δ=130ηιη。 本發明還注意到引入的釓、錆離子對螢光粉發射光譜半寬度 增加的影響,輻射半寬度Δλ〇,5=135-141 nm,在螢光粉格柵中的小 - 顆粒陽離子Gd+3和Y+3濃度最高的情況下。 * 本發明還注意到螢光粉發射光譜中的變化。在往Y離子中加 1.5原子里的肉色榮光粉顆粒就具備了黃—撥黃色。如果將 修 浪度提高到x=2·0,那麼螢光粉顆粒將擁有穩定的黃光。螢光粉中 Y離子含量的持續增加到:^2.4伴隨著在反射光譜出現綠色。從 所有資料可以得出,螢光粉成分中氧化稀土元素與氧化銘的比例 2化學方程式成分_區別在等於3 — 5。類_提高氧化㈣含 里可以得到更為完善的大顆粒多棱螢光粉顆粒。 八本發雜上可崎$,騎光雛有對於類似晶體 螢光粉完 全不—樣喃粒成分。表·2中為用於推薦儀器的該螢光粉顆粒大 • *規格與市場上標準螢光粉規格對比。 用於發光二極體.螢光粉分散指標 表-2The main energy conversion between the Ce ions 313⁄42 and 2d requires excitation of the energy consumption of the quantum hV = 2. 7 electron volts, which corresponds to the wavelength of the absorbed light λ = 457 ηιη. This 21 1298348 1 n time electron cell displacement is actually the least likely, because the wavelength of the emitted light is 2 5 5 displacement equal to 525 525. A 12% low-value cell shift similar to that due to the divergent wavelength is a luminescence. In the present invention, it is known that the absorbed light of the main wavelength of 457 is likely to be due to the short-wave displacement of the Lu+3 ion added to the glory composition, and the Lu+3 ion content in the Qiansi _ optimal value. The wavelength is λ, 譲. Adding Gd+3 Xuan to the phosphor powder matrix can increase the absorption and increase the length by λ=477ηη!. The level of ~ 〇. 4 electron volts has a large effect on the luminescence of the 2 〇 main stimuli. The width of this level is located at a distance of 电子.9 eV from the material conduction zone, causing a large difference in the quantum wavelength of the light shot. In this case, the short-wavelength wavelength is between λ=51〇—565, and the long wave can reach λ=680^700 nm, and the maximum wavelength of the luminescence can reach λ=59〇. As shown above, the energy diversity of the Ce ion illuminating state makes it practically necessary to reproduce the yellow, yellow, red, and even deep red regions in the visible spectrum. This is required for the fabrication of optimal white light combining optical structures using semiconductor heterojunctions and phosphors. Indeed, if the maximum value of the short-wavelength spectrum of the heterojunction is between 1445 nm __ 475 legs, ie Δ - 3 〇 nm, then the maximum radiance of the luminescent powder can reach 65 nm, which satisfies the goal of achieving balanced white light. Necessary conditions for yellow, orange and red radiation. The present invention notes that the concentration of the primary catalyst Ce+3 ions has an effect on the luminescence spectral properties of the phosphor. If the Ce+3 ion concentration is the lowest and is between the 〇2, then the _$ light luminescence spectrum half is ^11()11111. The amount of Ce+3 ion in the fluorochemical forming knife increases. When the content z=〇〇5, the half-width of the radiation spectrum increases by 22 1298348 and is added to Δ=120ηιη, such as ζ=0·1, then Δ=130ηιη. The present invention also notes the effect of the introduced ruthenium and osmium ions on the increase in the half-width of the emission spectrum of the phosphor powder, the radiation half-width Δλ〇, 5=135-141 nm, and the small-particle cation Gd+ in the phosphor powder grid. 3 and the highest concentration of Y+3. * The present invention also notes changes in the emission spectrum of the phosphor. In the addition of 1.5 atoms to the Y ion, the flesh-colored glory powder particles have a yellow-yellow yellow color. If the repair wave is increased to x=2·0, the phosphor particles will have a stable yellow light. The Y ion content in the phosphor powder continues to increase to: ^2.4 accompanied by a green color in the reflectance spectrum. From all the data, it can be concluded that the ratio of oxidized rare earth elements to oxidized in the phosphor powder composition is 2 different from the chemical equation component _. Class _ Improve oxidation (4) contains more perfect large-particle multi-angle phosphor particles. Eight copies of the miscellaneous can be found on the $, the riding light has a similar crystal fluorescein powder is completely non-like granules. In Table 2, the phosphor powder particles used for the recommended instrument are large. * The specifications are compared with the standard phosphor powder specifications on the market. For light-emitting diodes. Fluorescent powder dispersion indicators Table-2

23 129834823 1298348

應當指出,用於本發明的螢光粉顆粒的表面比率比日本和美 國標準螢光粉小。較小的表面積無疑可以極大的降低來自異質钟It should be noted that the surface ratio of the phosphor powder used in the present invention is smaller than that of Japanese and American standard phosphor powder. The smaller surface area can undoubtedly greatly reduce the heterogeneous clock

的初始光的散射。同時指出螢光粉顆粒的尺寸分佈級差曲線差別 很大。本發明的螢光粉的分散數值與日本公司的螢光粉相同但比 美國Am.Tech同類產品小很多。 6.如申請專利範圍第丨項所述之螢光粉,其中該長波之特定波長係 超過560nm。 此外,本發明之螢光粉其異質結是直角平行六面體各個邊的 比例是1:1:0.1 - 1:2:0.12,此時,以基面和異質結髮光面相交的 多棱螢光粉顆粒的高度和顆粒内切圓半徑比例為1:3 一丨:丨,其言 度值為6 — 8微米,使在合成光中有初次放射藍光和再次放射 的黃、撥黃光的存在,當它們與色座標(在x=〇 28 y=〇 3() x=Q 42 y=〇.44之間)進行大容量的均勻混合時,避免了由於散射光過多形 成光混合不均勻的現象。 此外,本發明之螢光粉其單晶螢光粉微粒具有立體晶體結 構,當主要異質結折射係數和螢光粉顆粒物質折射係數比例在 2·8·1·8 3.2:2.0之間時’晶體拇格參數在&=12.1。八至a=i2 2°α 之間,主要都是沿著平面方向(m),使發光輸出角度在8 —Μ 度之間,並可能使用Frenel棱鏡對總光輻射進行補充對焦。其中該The scattering of the initial light. At the same time, it is pointed out that the size distribution curve of the phosphor powder particles is very different. The dispersion value of the phosphor powder of the present invention is the same as that of the Japanese company's phosphor powder but much smaller than that of the American Am. Tech. 6. The phosphor of claim 2, wherein the specific wavelength of the long wave exceeds 560 nm. Further, the phosphor powder of the present invention has a heterojunction in which the ratio of each side of the rectangular parallelepiped is 1:1:0.1 - 1:2:0.12, and at this time, the polygonal surface intersecting the light-emitting surface of the heterojunction The ratio of the height of the phosphor powder particles to the radius of the inscribed circle of the particles is 1:3. 丨: 丨, the value of which is 6-8 μm, so that there is a primary blue light in the synthesized light and a yellow and yellow light that is radiated again. The existence of large-capacity uniform mixing when they are compared with the color coordinates (between x=〇28 y=〇3() x=Q 42 y=〇.44), avoiding the formation of light mixing due to excessive scattered light. Uniform phenomenon. In addition, the phosphor powder of the present invention has a three-dimensional crystal structure, and when the ratio of the refractive index of the main heterojunction to the refractive index of the phosphor powder is between 2·8·1·8 3.2:2.0' The crystal thumbgness parameter is & = 12.1. Between eight and a=i2 2°α, mainly along the plane direction (m), the illumination output angle is between 8 and Μ, and the Frenel prism may be used to supplement the total optical radiation. Which should

24 1298348 棱鏡的第一個平面距離螢光粉微粒發光基面100 一2〇〇微米,中 間填充透明聚合物填充物,折射係數在n=142 一 η=1·55之間。 此外,本發明之螢光粉其大顆粒多棱面顆粒從所有14個相互 連接平面發光,量子輸出為6〇 一 95%,當螢光粉的化學方程式為 Gd3_x_y_zYx LuyCezAlp〇c^,可使該螢光粉的強烈的黃-撥黃色長波 光,波長在Xmax=530— 595nm之間,最大光譜半寬度為、产11〇 一 130 nm之間,隨著螢光粉化學組分中Gd離子劑量的增長而增 大。其中該化學指數變動如下·· 10<χ<26,〇〇〇〇1取〇5, 0.0001 幺ZS0.5,4.7幺Ζ幺5.3,q=4.5+1.5*p之間變動。 此外,本發明亦揭露白光二極體之螢光粉的製造方法,本發 明之螢光粉的製作是通過所謂的陶制流程圖進行的,以下列述九 種螢光粉的備制方法。請參照圖1,其繪示根據本發明第一實施例 之螢光粉之製作方法之流程示意圖。如圖所示,本發明第一實施 例之螢光粉製造方法包括下列步驟:先秤取如下Gd2〇3,, LU2〇3及Al2〇3氧化物若干量(步驟i);取用若干濃度之Ce(N〇3)3 水溶液(步驟2);將秤取之氧化物全數加入Ce(N〇3)3水溶液中, 並使之充分混合(步驟3);將充分混合之水溶液置入烘箱中乾燥, 得混合粉末(步驟4);在混合粉末内添加若干量之Na2S〇4、 寺LUSO4:^末後充分混合’再將混合粉末放入石英掛銷中(步驟 5);將石英坩鍋放置於游離仰3之氣氛保護爐中,以特定速度升溫 至第一溫度,並以此溫度保持第一時間後再以等速度升溫至第二24 1298348 The first plane of the prism is 100 to 2 μm from the luminescent base of the phosphor powder, filled with a transparent polymer filler, and the refractive index is between n=142 and η=1·55. In addition, the phosphor powder of the present invention has large particle polyhedral particles emitting light from all 14 interconnected planes, and the quantum output is 6〇95%. When the chemical formula of the phosphor powder is Gd3_x_y_zYx LuyCezAlp〇c^, the The intense yellow-picked yellow long-wavelength of the phosphor powder, with a wavelength between Xmax=530-595nm and a maximum spectral half-width of between 11〇130 nm, with the Gd ion dose in the chemical composition of the phosphor powder The increase in growth. The chemical index changes as follows: · 10 < χ < 26, 〇〇〇〇 1 takes 〇 5, 0.0001 幺 ZS0.5, 4.7 幺Ζ幺 5.3, q = 4.5 + 1.5 * p varies. Further, the present invention also discloses a method for producing a phosphor of a white light diode. The production of the phosphor powder of the present invention is carried out by a so-called ceramic flow chart, and the following nine kinds of phosphor powder preparation methods are described. Referring to FIG. 1, a schematic flow chart of a method for fabricating a phosphor powder according to a first embodiment of the present invention is shown. As shown in the figure, the method for manufacturing a phosphor powder according to a first embodiment of the present invention comprises the steps of: first weighing the following Gd2〇3, LU2〇3 and Al2〇3 oxides (step i); taking a concentration Ce(N〇3)3 aqueous solution (step 2); add the scaled oxides to the Ce(N〇3)3 aqueous solution and mix them thoroughly (step 3); place the well mixed aqueous solution in the oven Drying, mixing powder (Step 4); adding a certain amount of Na2S〇4, Temple LUSO4: after the end of the mixed powder, thoroughly mixing ', then putting the mixed powder into the quartz hanging pin (Step 5); Placed in an atmosphere protection furnace of free elevation 3, and heated to a first temperature at a specific speed, and maintained at the same temperature for a first time and then heated to a second speed at a constant speed.

25 1298348 、度以此度保持第二時間後再以等速度升溫至第三溫度,以 此溫度保持第三時間後再以等速度降溫至室溫取出(步驟6);將取 出之粉末用硝酸和磷酸清洗未反應之物質,然後用大量清水重複 清洗至中性為止(步驟7);以及將清洗後之粉末置入烘箱中乾燥, 乾餘後即得螢光粉產品(步驟8)。 於步驟 1 中,該 Gd203 為 17.2g,Y2〇3 為 271g,Lu2〇3 為 59.7g25 1298348, the degree is maintained for the second time and then warmed to the third temperature at the same speed, the temperature is maintained for the third time and then cooled to room temperature at the same speed (step 6); the powder to be taken out is nitric acid The unreacted material is washed with phosphoric acid, and then repeatedly washed with a large amount of water until neutral (step 7); and the washed powder is placed in an oven to be dried, and after drying, the phosphor powder product is obtained (step 8). In step 1, the Gd203 is 17.2g, the Y2〇3 is 271g, and the Lu2〇3 is 59.7g.

而八丨2〇3為26〇g。 於步驟2中’該Ce(N〇3)3水溶液中含有〇·ι μ之Ce(N03>。 於步驟4中,該充分混合之水溶液係置入12〇〇c之烘箱中乾 燥,得混合粉末。 於步驟5中’在混合粉末内係添加24克之ΝΜ〇4、12克ΜΑ 和4克LijO4粉末後充分混合,再將混合粉末放入5〇〇毫升的石 央掛銷中。 於步驟6中,麟離NH3之成份為%112=3:卜且以5。〇分鐘 速度升溫至4默之第-溫度,以此溫度保持一小時(即第—日^里) 贿以5。0分鐘賴躲至之$二溫度,贿溫度保持三 小日守(即第二時間)後再以5。〇分鐘速度升溫至i獅。C之第三溫 度,以此溫度保持四小時(即第三時間)後再以50C/分鐘速度降= 室溫取出。 於步驟7巾’該植之_為1:卜和猶之關亦為1:1清 洗未反應之物質,織狀量清水重複清絲巾性為止。’月 26 1298348 於步驟8中,該烘箱之溫度為i2〇°C。 請參照圖2,其繪示根據本發明第二實施例之螢光粉之製作方 法之流程示意圖。如圖所示,本發明第二實施例之螢光粉製造方 法包括下列步驟:先秤取氧化物如TGd2〇3_34.4g ’ Y2O3 -249g, WO3 - 59.7g ’ Al2〇3 —260g (步驟 1);取用 Ce(N03)3 水溶液,水溶 液中含有0·1 M(莫耳)之Ce(N〇3)3 (步驟幻;將秤取之氧化物全數 > 加入Ce(N〇3)3水溶液中,並使之充分混合(步驟3);將充分混合 之水溶液置入烘箱中乾燥,得混合粉末(步驟4);在混合粉末内添 加右干1之NajO4、KjO4和Li2S04·粉末後充分混合,再將混合 粉末放入石英坩鍋中(步驟5);將500毫升的石英坩鍋放置於游離 NH3(N2:H2=3:1)之氣氛保護爐中,以5°C/分鐘速度升溫至450°C, 以此溫度保持一小時後再以5〇c/分鐘速度升溫至12〇〇〇c,以此溫 度保持三小時後再以5cC/分鐘速度升溫至15〇〇〇c,以此溫度保持 • 四小時後再以5°C/分鐘速度降溫至室溫取出(步驟6);將取出之粉 末用硝酸(比例1:1)和璘酸(1:1)清洗未反應之物質,然後用大量清 水重複清洗至中性為止(步驟7);以及將清洗後之粉末置入 T-120°C的烘箱中乾燥,乾燥後得最中之螢光粉產品(步驟8)。 以上根據本發明較佳實施例所製造之螢光粉之化學式如表_3 所示。表-3中列出螢光粉的主要光譜和發光指標。 表-3 推薦螢光粉的成分 晶體 Xmax,納 量子輸 相j 的主 米 出η% 亮 要大 度, 27 1298348 小 (微 米), h x 1 xk -------- % Gd〇 > 2^2' 4L110»3Ce〇»1AI5' 10x1 545 85 80 l〇12’15 2x12 Gd〇 * 4Y2 * 2Lu〇 * 3Ce〇 * 1AI5 > 12x1 '—---- 550 95 95 l〇12 Ί5 2x12 Gd〇,6丫2,2Lu〇,3Ce〇,1AI5, 10x1 ' —---- 555 100 100 l〇12’ 15 0x10 Gdi ’ 〇Yi ’ gLu。,iCe〇,1AI5, 8x10 〜—____ 565 100 92 l〇12,15 xl2 Gdi ’ 3Y1 ’ 6Lu〇,〇5Ce〇,05AI5, 10x8 575 94 90 l〇12,15 xl2 Gdi ’ 4Y1,5LU0,〇5Ce〇 ’ 05 AI5, 10x8 595 90 86 l〇12’ 15 xl2 Gdi,4Y1,5L110 ’ ogCe。,02AI5, 10x1 592 88 84 2〇12'3 0x14 Gdi * 4Y1 · 3L110» 2Cg〇 > 1AI5 > 10x1 590 86 87 2〇12’3 0x14 Gdi · 1Y1 * 5LU0 . 3sCe〇 · 05 10x1 570 94 91 AI5 2〇12 3 0x12 Y3 Al5〇i2Ce(標準) lx6x 550 80 75~~ 3 ----And gossip 2〇3 is 26〇g. In step 2, the Ce(N〇3)3 aqueous solution contains 〇·ι μ of Ce (N03>. In step 4, the well-mixed aqueous solution is placed in an oven of 12 〇〇c to be dried to obtain a mixture. Powder. In step 5, add 24 g of ΝΜ〇4, 12 g ΜΑ and 4 g of LijO4 powder to the mixed powder, mix well, and then put the mixed powder into a 5 〇〇 ml stone pin. In 6, the composition of the lining from NH3 is %112=3: and the temperature is raised to 5. The temperature of the 默 minute is increased to the temperature of 4 mils, and the temperature is maintained for one hour (ie, the first day). Minutes to hide the $ two temperature, the bribe temperature to keep three small days (ie the second time) and then heat up to 5. Lions. The third temperature of C, this temperature for four hours (ie the first After three times), take the speed drop at 50C/min = take it out at room temperature. In step 7, the towel's _ is 1: Bu and Juzhiguan is also 1:1 clean unreacted material, and the amount of water is repeated.丝261298348 In step 8, the temperature of the oven is i2 〇 ° C. Please refer to FIG. 2, which illustrates the production of luminescent powder according to the second embodiment of the present invention. Schematic diagram of the method. As shown in the figure, the method for producing a phosphor powder according to a second embodiment of the present invention comprises the following steps: first weighing an oxide such as TGd2〇3_34.4g 'Y2O3-249g, WO3-59.7g 'Al2〇3 - 260g (Step 1); take Ce(N03)3 aqueous solution, containing 0.1 M (mole) of Ce(N〇3)3 in the aqueous solution (step magic; add the full oxide of the scale) to Ce (N〇3)3 aqueous solution, and thoroughly mixed (step 3); the well-mixed aqueous solution is placed in an oven to dry, to obtain a mixed powder (step 4); add right dry 1 NajO4, KjO4 in the mixed powder After thoroughly mixing with Li2S04· powder, put the mixed powder into a quartz crucible (step 5); place 500 ml of quartz crucible in an atmosphere protection furnace with free NH3 (N2:H2=3:1) to The temperature was raised to 450 ° C at a rate of 5 ° C / min. After maintaining this temperature for one hour, the temperature was raised to 12 ° C at a rate of 5 ° C / min. The temperature was maintained for three hours and then increased to 5 c C / min. 15〇〇〇c, keep at this temperature • After four hours, cool down to room temperature at 5 ° C / min (step 6); remove the powder with nitric acid ( Example 1:1) Wash unreacted material with tannic acid (1:1), then repeat washing with neutral water to neutral (step 7); and place the washed powder in an oven at T-120 °C. After drying and drying, the most fluorescent powder product is obtained (step 8). The chemical formula of the phosphor powder manufactured according to the preferred embodiment of the present invention is shown in Table _3. The phosphor powder is listed in Table-3. Main spectrum and luminescence index. Table-3 Recommended composition of crystal powder Xmax, nanometer quantum phase j main η% bright, 27 1298348 small (micron), hx 1 xk ------ -- % Gd〇> 2^2' 4L110»3Ce〇»1AI5' 10x1 545 85 80 l〇12'15 2x12 Gd〇* 4Y2 * 2Lu〇* 3Ce〇* 1AI5 > 12x1 '----- 550 95 95 l〇12 Ί5 2x12 Gd〇,6丫2,2Lu〇,3Ce〇,1AI5, 10x1 '——---- 555 100 100 l〇12' 15 0x10 Gdi ' 〇Yi ' gLu. ,iCe〇,1AI5, 8x10 ~—____ 565 100 92 l〇12,15 xl2 Gdi ' 3Y1 ' 6Lu〇,〇5Ce〇,05AI5, 10x8 575 94 90 l〇12,15 xl2 Gdi ' 4Y1,5LU0,〇5Ce 〇' 05 AI5, 10x8 595 90 86 l〇12' 15 xl2 Gdi, 4Y1, 5L110 ' ogCe. , 02AI5, 10x1 592 88 84 2〇12'3 0x14 Gdi * 4Y1 · 3L110» 2Cg〇> 1AI5 > 10x1 590 86 87 2〇12'3 0x14 Gdi · 1Y1 * 5LU0 . 3sCe〇· 05 10x1 570 94 91 AI5 2〇12 3 0x12 Y3 Al5〇i2Ce (standard) lx6x 550 80 75~~ 3 ----

本發明中使用的螢光粉為鋁-釓〜釔〜镥榴,其螢光粉顆粒具有 大顆粒夕棱面形態,為了自身使用需要採用榮光粉聚合物層的改 型工藝。首先,必須使用精細的機械攪拌來配置螢光粉懸浮物; 取佳方式是使用超聲波槽來進賴拌操作。第二,合理地提高懸 子物二螢絲顆粒,辰度。據本發明之資料,螢光粉顆粒最佳含量 750/0 為 0· 001-〇· 002 毫升。 28 1298348 在本發明中亦對製作的白光二極體的工作壽命進行了系列測 4 °測試包括連續工作1000小時的發光二極體光強I ( mCd)測The phosphor powder used in the present invention is aluminum-niobium-tantalum-niobium, and the phosphor powder particles have a large particle-shaped prism face shape, and a modification process of the glory powder polymer layer is required for self-use. First, fine mechanical agitation must be used to configure the phosphor suspension; a preferred method is to use an ultrasonic bath for the mixing operation. Second, reasonably improve the particles of the two filaments of the suspension. According to the information of the present invention, the optimum content of the fluorescent powder particles is 750/0, which is 0·001-〇·002 ml. 28 1298348 In the present invention, the working life of the produced white light diode is also measured in series. The 4 ° test includes the luminous intensity I (mCd) measurement of the LED for 1000 hours of continuous operation.

1°發光二極體直流電穩定在20毫安培,供電電壓為U 〜3· 20-3.28 V。製作了 25個採用大顆粒螢光粉的發光二極體,作 為對比標準是採用日本公司N螢光粉25個發光二極體。測試結果 見表〜4。 表〜4 藍光 發光 二極 體樣 品 ι〇 τη mCd 平均值 Ιδ〇〇,mCd 平均值 I loooJ mCd 平均值 11000/ Io, °/o 大顆 粒螢 光粉 320 324.1 332· 2 103.76 日亞 標準 螢光 粉 320 291.2 259.2 81.0 因為U工作可以連續工作1〇〇〇小時,所以認為儀器的光強可能 會因為發光二極體工作電壓降低而改變的假設是不存在的。 這種用大顆粒多棱螢光粉製成的白光發光二極體的亮度增長 的物理事實是先前沒有注意_,需要深人細_研究。勿庸置 疑的是該螢光粉顆粒具有與眾不同的不尋常的特性。 综上所述,每顆規格為〇· 2x0· 3微米的GafHnN晶體異質結 29 1298348 表面都從各個輻射面覆蓋大顆粒多棱微晶為主的懸浮物發出的光 流為4 — 6流明,異質結的工作電流為j=2〇mA。16個串連在發 射矩陣上的發光二極體,所需電流J=800 mA,光流為F=98-120 流明,這保證光輸出達到η=22-28流明/伏,因此,確可改善習知 白光二極體及其螢光粉製作方法之缺點。 雖然本發明已以較佳實施例揭露如上,然其並非用以限定本The 1° LED is stable at 20 mA and the supply voltage is U 〜3·20-3.28 V. Twenty-five light-emitting diodes using large-particle phosphor powder were produced, and as a comparison standard, 25 light-emitting diodes of Japanese company N phosphor powder were used. Test results See Table ~4. Table ~4 Blue Light Emitting Diode Sample ι〇τη mCd Average Ιδ〇〇, mCd Average I loooJ mCd Average 11000/ Io, °/o Large Particle Fluorescent Powder 320 324.1 332· 2 103.76 Nichia Standard Fluorescence Powder 320 291.2 259.2 81.0 Since U can work continuously for 1 hour, it is assumed that the light intensity of the instrument may change due to the reduced operating voltage of the LED. The physical fact that the brightness of white light-emitting diodes made of large-particle polygonal phosphors has increased is not previously noted, and requires deep research. It is undoubted that the phosphor particles have unusual characteristics that are distinctive. In summary, each of the GafHnN crystal heterojunctions 29 1298348 with a size of 〇·2x0·3 microns has an optical flow of 4-6 lumens from a suspension of large particles of polycrystalline microcrystals covered by each radiation surface. The operating current of the heterojunction is j=2〇mA. 16 LEDs connected in series on the emission matrix, the required current J = 800 mA, the optical flow is F = 98-120 lumens, which ensures that the light output reaches η = 22-28 lumens / volt, so it is true Improve the shortcomings of the conventional white light diode and its fluorescent powder manufacturing method. Although the present invention has been disclosed above in the preferred embodiments, it is not intended to limit the present invention.

發明,任何熟習此技藝者,在不脫離本發明之精神和範圍内,當 可作少許之更動與潤飾,因此本發明之保護範圍當視後附之申請 專利範圍所界定者為準。 【圖式簡單說明】 圖1為-示意圖’其綠示根據本發明第一實施例之螢光粉之 製作方法之流程示意圖。 圖2為-示意圖’其緣示根據本發明第二實施例之榮光粉之 製作方法之流程示意圖。 表-1示出由標準分散分佈和大小的榮光粉顆粒製成的塗層。 表-2 +為驗減儀_錄糖雛別、規減市場上標 準螢光粉規格對比。 表-3示出本發明之九種螢光粉之化學式。 體 表_4為對比標準是_曰本公司N榮光粉25個發 測試結果。 【主要元件符號說明】 30 1298348 步驟1 :先秤取如下Gd2〇3 ’ ΙΟ3,ΜΑ及从〇3氧化物若 干量; 步驟2 :取用若干濃度之Ce(N03)3水溶液; 步驟3 :將秤取之氡化物全數加入Ce(N〇3)3水溶液中並使 之充分混合; 步驟4 :將充分混合之水溶液置入烘箱中乾燥,得混合粉末; 步驟5:在混合粉末内添加若干量之卿〇4、]^〇4和Li2S04· 粉末後充分混合,再將混合粉末放入石英坩鋼中; 步驟6 ··將石英掛鋼放置於游離之氣氛保護爐中,以特定 速度升狐至$ /皿度,並以此溫度保持第一時間後再以等速度升 溫至第二溫度,以此溫度保持第二時間後再以等速度升溫至第三 /皿度’以此’皿度保持第三時間後再轉速度降溫至室溫取出; 步驟7 :將取出之粉末用硝酸和磷酸清洗未反應之物質,然後 .肖大量清水重複清洗至巾性為止;以及 步驟8 ·將清洗後之粉末置入供箱中乾燥,乾燥後即得榮光粉 產品。 ’The invention is to be understood as being limited by the scope of the appended claims. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a schematic view showing the flow of a method for producing a phosphor according to a first embodiment of the present invention. Fig. 2 is a schematic view showing the flow of a method for producing a glazing powder according to a second embodiment of the present invention. Table-1 shows the coatings made from phoenix powder particles of standard dispersion distribution and size. Table-2 + is the comparison of the specifications of the fluorescent powder in the market. Table-3 shows the chemical formulas of the nine kinds of phosphors of the present invention. The surface standard _4 is the comparison standard is _ 曰 曰 N N N N N N N N [Main component symbol description] 30 1298348 Step 1: First weigh the following Gd2〇3 ' ΙΟ3, ΜΑ and a certain amount of 〇3 oxide; Step 2: Take several concentrations of Ce(N03)3 aqueous solution; Step 3: The weighed compound is added to the Ce(N〇3)3 aqueous solution and mixed thoroughly; Step 4: The well-mixed aqueous solution is placed in an oven to be dried to obtain a mixed powder; Step 5: Adding a certain amount to the mixed powder After the powder 4,]^〇4 and Li2S04· powder, mix well, then put the mixed powder into the quartz steel; Step 6 · Place the quartz steel in a free atmosphere protection furnace to raise the fox at a specific speed To $ / dish degree, and to maintain the first time at this temperature, then increase the temperature to the second temperature at the same speed, and then maintain the temperature for the second time and then increase the temperature to the third / dish degree at the same speed. After the third time, the temperature is further reduced to room temperature and taken out; Step 7: The unreacted material is washed with nitric acid and phosphoric acid, and then washed with a large amount of water to the towel; and step 8 · after cleaning The powder is placed in a box for drying and drying Powder product is obtained after glory. ’

Claims (1)

1298348 十、申請專利範園·· 1· -種白光二極體之螢絲,其係由氮化鎵及氮化銦半導體 異質結而成,其具有若干輻射波長,且裝備有由乳也轉基,飾催 化的多棱面絲度分散縣粉,其光_彻通財程式為 Gd3_x_y_zYxLuyCezAlp〇q ’其中’該光譜轉換器通用方程式之化學指 : 1.0<χ<2.6, 0.0001<y<〇.5 , 〇.〇〇〇ι<ζ<〇 5,4 ?<z<5 3 , q=4.5+1.5V該料粉為大麵分散的單晶,且多棱主要是1 •體形’該六面體有兩個相互平行的基面,由12條梯形邊構成,、這 些邊相互成—夾角,同時該多棱顆粒直接與異質結幸畐射正面和四 個端面進行光學接觸,並覆蓋異質結光表面若干面積,發光表面 與螢光粉顆粒轉換發出的特定波長的長波光一起構 為發嫩上纖高’且該異陶導觀點處於異 β r二=請專利細第1斯叙㈣二㈣之料粉,其中該 ©輻射波長係小於470 nm。 3·如申料觸圍第丨彻述之縣粉,^ 150。。 H申請專利範圍第1項所述之榮光粉,其中該多棱顆粒直接 與異貝、.,。輪射正面和四個端面進行光學接觸,並覆蓋該異質 表面20 —85%面積。 、 5·如申請專·_蘭狀_,其 長係超過560nm。 收 32 1298348 6.如申請專利範圍第1項所述之螢光粉,其中該螢光粉顆粒内 切圓的半徑在6 —12微米之間,兩個基面的高度距離在4一1〇微米 之間。 7·如申請專利範圍第1項所述之螢光粉,其中該合成白光之色 溫在Τ=12000-2500οΚ之間,且在發散度為6 —12度角上,具很 高之光強。 _ / 8·如申請專利範圍第1項所述之螢光粉,其中該異質結是直角 平行六面體各個邊的比例是1:1:〇1 一 1:2:〇12,此時,以基面和 貝、、、Ό磋光面相父的多棱螢光粉顆粒的高度和顆粒内切圓半徑比 例為1:3 - 1:1,其高度值為6 — 8微米,使在合成光中有初次 放射藍光和再次放射的黃、橙黃光的存在,當它們與色座標、在 χ=〇·28 y=a30 xKU2 y=0 44之間)進行大容量的均勻混合時,避 免了由於散射光過多形成光混合不均勻的現象。 鳙 9·如申明專利縫第8項所述之螢光粉,其單晶榮光粉微粒具 有立體晶體結構’當主要異f結折㈣數和螢输麵物質折射 係數比例在2.8:1.8 - 3.2:2.0之間時,晶體柵格參數在a=121〇A •2 A之間,主要都是沿著平面方向(in),使發光輸出 角度在8 -16度之間,並可能使用於㈣破鏡對總光輻射進行補 充對焦。 瓜如申請專利範圍第9項所述之螢光粉,其中該棱鏡的第一 個平面距離螢光粉微粒發絲面1〇〇 -200微米,中間填充透明 33 1298348 m 合物填充物’折射係數在η=1·42 一 n=:i M之間。 11.如申请專利範圍第8項所述之螢光粉,其大顆粒多棱面顆 粒從所有14個相互連接平面發光,量子輸出為6〇 一 95%,當螢光 粉的化學方程式為Gd3.x.y_zYx LuyCezAlpCMf,可使該螢光粉的強 烈的頁橙育色長波光,波長在入_=53〇一 595 nm之間,最大光 譜半寬度為‘HO - 130啦之間,隨著榮光粉化學組分中況 離子劑量的增長而增大。 % 12·如申請專利範圍第11項所述之榮光粉,其中該化學指數變 動如下:1·0<χ<2·6,0._奶〇.5 , 〇·_㈤〇 5,4 7如 3, q=4.5+1.5*p之間變動。 13· -種白光二極體之螢光粉之製作方法,其包括下列步驟: 先秤取如下Gd203,γ2〇3,lU2〇3及八12〇3氧化物若干量; 取用若干濃度之Ce(N03)3水溶液; 儀 將秤取之氧化物全數加入Ce(N〇3)3水溶液中,並使之充分混 合; 將充分混合之水驗置讀箱中絲,得混合粉末,· 、在混合粉末内添加若干量之他卿哪机㈣粉末後充 分混合,再將混合粉末放入石英坩銷中,· 將石英賴放胁_贿3之氣氛賴射,崎 至第-溫度’並以此溫度保持第—時間後再以等速度升溫^第: 溫度,以此溫度保持第二_後再轉速奸溫至第』度,二 34 1298348 此/皿度保持第三時再以等速度降溫至室溫取出; 將取出之粉末用硝酸和磷酸清洗未 清水重複清洗至中性為止, ·以及反應之物質,然後用大量 =清洗後之粉末置人烘射_,乾燥餅得蘇粉產品。 R如申請專利範園第13項所述之製作方法,其中該⑽為 •2g ’ YA為271g ’ Lu2〇3為59.78而八12〇3為2卿。 、15.如申請專利範圍第13項所述之製作方法,其中該Ce(N〇^ 水溶液中含有〇· 1M之Ce(N03)3。 16.如申料種圍第13衡叙製作方法,財該充分混合 之水溶液係置入120V之烘箱中乾燥,得混合粉末。 m 17·如申請專利細第13項所狀製作方法,射該混合粉末 内係添加24克之施风、12克以〇4和4克Li2S〇4粉末後充分混 合,再將混合粉末放入500毫升的石英坩鍋中。 18·如申請專利範圍第13項所述之製作方法,其中該游離Nh3 之成份為Ν2:Η2=3··1 ;該特定速度係^c/分鐘速度;該第一溫度係 400°C ;該第一時間係一小時;該第二溫度係12〇〇〇c ;該第二時間 係三小時;該第三溫度係15〇〇〇c ;以及該第三時間係四小時。 19.如申請專利範圍第13項所述之製作方法,其中該硝酸之比 例為1:1,而礙酸之比例亦為1:1。 351298348 X. Patent application Fan Park····· A kind of white light diode filament, which is made of heterojunction of gallium nitride and indium nitride semiconductor, which has several radiation wavelengths and is equipped with milk. The base is decorated with a catalyzed polyhedral filament dispersing county powder, and its light_cutting code is Gd3_x_y_zYxLuyCezAlp〇q 'where the chemical of the general equation of the spectral converter is: 1.0<χ<2.6, 0.0001<y< 〇.5 , 〇.〇〇〇ι<ζ<〇5,4 ?<z<5 3 , q=4.5+1.5V The powder is a large-surface dispersed single crystal, and the multi-edge is mainly 1 • body shape 'The hexahedron has two mutually parallel bases, consisting of 12 trapezoidal edges, which are at an angle to each other, and the polygonal particles are in direct optical contact with the front side and the four end faces of the heterojunction. And covering a certain area of the surface of the heterojunction light, the light-emitting surface is combined with the long-wavelength light of a specific wavelength converted by the phosphor powder particles to form a high-fibre high-- and the viewpoint of the different ceramic guide is in different β r two = please patent fine 1 The material of Si (4) 2 (4), wherein the wavelength of the radiation is less than 470 nm. 3. If the application is in contact with the second grade of the county, ^ 150. . H claims the glory powder described in the first item of the patent scope, wherein the multi-edge particles are directly related to the bismuth, . The front side of the wheel is in optical contact with the four end faces and covers 20 to 85% of the area of the heterogeneous surface. 5) If you apply for a special _ blue _, the length is more than 560nm. The fluorinated powder according to claim 1, wherein the radius of the inscribed circle of the phosphor powder is between 6 and 12 microns, and the height of the two bases is 4 to 1〇. Between microns. 7. The phosphor powder according to claim 1, wherein the color temperature of the synthetic white light is between Τ=12000-2500οΚ and has a high light intensity at a divergence angle of 6-12 degrees. _ / 8. The phosphor powder according to claim 1, wherein the heterojunction is a ratio of each side of a rectangular parallelepiped of 1:1: 〇1 to 1:2: 〇12, at this time, The ratio of the height of the polygonal prism powder and the radius of the inscribed circle of the granules of the base surface and the shells, and Ό are 1:3 - 1:1, and the height value is 6-8 μm, so that the synthesis In the light, there is the presence of yellow and orange light that emits blue light for the first time and re-radiation. When they are mixed with the color coordinates, between χ=〇·28 y=a30 xKU2 y=0 44), large-volume uniform mixing is avoided. Excessive light mixing results in uneven light mixing.鳙9·If the fluorescent powder described in Item 8 of the patented seam, the single crystal glory powder particles have a three-dimensional crystal structure 'when the main heterogeneous f-fold (four) number and the refractive index of the fluttering surface material are in the ratio of 2.8:1.8 - 3.2 Between 2.0, the crystal grid parameters are between a=121〇A •2 A, mainly along the plane direction (in), so that the illumination output angle is between 8 and 16 degrees, and may be used in (4) The mirror is used to supplement the total light radiation. The phosphor powder according to claim 9, wherein the first plane of the prism is 1 〇〇-200 μm from the hairline surface of the phosphor powder, and the intermediate filled transparent 33 1298348 m compound filler 'refracting The coefficient is between η=1·42 and n=:i M . 11. The phosphor powder according to claim 8, wherein the large particle polygonal particles emit light from all 14 interconnected planes, and the quantum output is 6〇95%, when the chemical formula of the fluorescent powder is Gd3. .x.y_zYx LuyCezAlpCMf, which can make the fluorescent powder have strong orange-colored long-wavelength light with a wavelength between _=53〇-595 nm and a maximum spectral half-width of between 'HO-130'. The amount of ion in the chemical composition of glory powder increases. %12·If the glory powder described in claim 11 of the patent scope, the chemical index changes as follows: 1·0<χ<2·6,0._奶〇.5, 〇·_(5)〇5,4 7 3, q=4.5+1.5*p changes. 13· a method for producing a white light diode phosphor powder, comprising the following steps: first weighing the following Gd203, γ2〇3, lU2〇3 and 八12〇3 oxide; taking a certain concentration of Ce (N03)3 aqueous solution; the meter will add the whole amount of oxide to the Ce(N〇3)3 aqueous solution and mix it thoroughly; the fully mixed water will be placed in the reading box to obtain the mixed powder, ·, Add a certain amount of the powder to the mixed powder and mix it thoroughly, then mix the powder into the quartz crucible, and put the quartz 放 _ _ _ 3 3 3 3 3 3 3 3 3 3 3 3 3 This temperature is maintained at the same time and then warmed up at the same speed. ^: Temperature, the temperature is kept at the second _ and then the temperature is tempered to the first degree, two 34 1298348. This / dish is kept at the third time and then cooled at the same speed. The mixture is taken out at room temperature; the removed powder is washed with nitric acid and phosphoric acid, and the washing is repeated until neutral, and the reacted material is then sprayed with a large amount of the powder after washing, and the dried cake is dried. R is the production method described in claim 13 of the patent application, wherein the (10) is • 2g YA is 271g ‘Lu2〇3 is 59.78 and 八12〇3 is 2 qing. 15. The method according to claim 13, wherein the Ce (N〇^ aqueous solution contains Ce(N03)3 of 〇·1M. 16. The well-mixed aqueous solution is placed in a 120V oven to be dried to obtain a mixed powder. m 17·If the preparation method of the patent item 13 is applied, the mixed powder is added with 24 g of the wind and 12 g of the crucible. 4 and 4 g of Li2S〇4 powder are thoroughly mixed, and then the mixed powder is placed in a 500 ml quartz crucible. 18. The production method according to claim 13, wherein the free Nh3 component is Ν2: Η2=3··1; the specific speed is ^c/min speed; the first temperature is 400 ° C; the first time is one hour; the second temperature is 12 〇〇〇c; the second time is Three hours; the third temperature is 15 〇〇〇c; and the third time is four hours. 19. The method according to claim 13, wherein the ratio of nitric acid is 1:1, and The acid ratio is also 1:1. 35
TW095106939A 2006-03-02 2006-03-02 Fluorescent powder for white light diode and manufacturing method thereof TW200734442A (en)

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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TWI404240B (en) * 2009-02-06 2013-08-01 Everlight Electronics Co Ltd Colorful light-emitting apparatus

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
TWI404240B (en) * 2009-02-06 2013-08-01 Everlight Electronics Co Ltd Colorful light-emitting apparatus

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