TW201022411A - Warm white light emitting diode using gadolinium lutetium cerium as substrate and phosphor powder thereof - Google Patents

Warm white light emitting diode using gadolinium lutetium cerium as substrate and phosphor powder thereof Download PDF

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TW201022411A
TW201022411A TW097148201A TW97148201A TW201022411A TW 201022411 A TW201022411 A TW 201022411A TW 097148201 A TW097148201 A TW 097148201A TW 97148201 A TW97148201 A TW 97148201A TW 201022411 A TW201022411 A TW 201022411A
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phosphor powder
light
powder
emitting diode
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TW097148201A
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TWI390016B (en
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Naum Soshchin
wei-hong Luo
qi-rui Cai
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wei-hong Luo
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    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
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Abstract

The present invention discloses a phosphor powder taking gadolinium lutetium cerium as substrates, the characterized in that: F.sup.-1 ions and N.sup.-3 ions are added into the phosphor powder to replace a portion of the oxygen ions in the garnet lattice, wherein the stoichiometric formula is: (Gd.sub.1-x-yLu.sub.xCe.sub.y).sub.3Al.sub.5O.sub.12-zF.sub.z/2N.sub.z/2. The phosphor powder can irradiate in the scope of orange-red spectrum after the phosphor powder is excited by an indium gallium nitride (InGaN) semiconductor heterostructure shortwave. Additionally, this invention also discloses a warm-white-light emitting diode that adopts the phosphor powder having gadolinium lutetium cerium as substrates. When the semiconductor heterostructure having the wavelength lambda that is equal to 420-500 nm is radiatively excited, the maximum emitting of the phosphor powder in the orange-red spectrum is that lambda is greater than 575 nm, the half wave width is greater than 135 nm, and the color rendering index Ra is equal to 80.

Description

201022411 九、發明說明: 【發明所屬之技術領域】 本發明係有關於一種以乳轉鈽為基質的暖白光發光二極體及 其螢光粉,尤指一種可結合不同的新型固態光源,以及#InGaN 氮化物異質結為基質且含有大量奈米級結構的異質結之以乳錄錦 為基質的暖白光發光二極體及其螢光粉。 【先前技術】 具有Ja3d石權石結構空間組的發光材料在2〇世紀六十年代已 被廣泛採用在核能及鐳射物理中;初次石榴石合成的學術報告是由 ❹美國的工程師 H Yooder及M.Kettle(請參照 Amer. Mineralogist 1952 V36N6P15〜98)第一次提出含有Y3Al5〇i2成份的單晶人工石榴 石’將此命名為纪鋁石榴石(YAG)。 該項工作中已指出’ YAG的化學成份晶格結構與天然礦物 Crossulara-Ca3Al2Si3012 以及 spessartine_Mn3Al2Si3〇i_差別,201022411 IX. Description of the Invention: [Technical Field] The present invention relates to a warm white light emitting diode based on a milk transition and a fluorescent powder thereof, and more particularly to a novel solid state light source which can be combined with different #InGaN Nitride Heterojunction is a matrix and contains a large number of nano-structured heterojunctions. The warm white light-emitting diodes and their phosphors are based on the milk record. [Prior Art] Luminescent materials with Ja3d stone structure space group have been widely used in nuclear energy and laser physics in the 1960s; the first report of garnet synthesis was made by American engineers H Yooder and M. .Kettle (please refer to Amer. Mineralogist 1952 V36N6P15~98) for the first time to propose a single crystal artificial garnet containing Y3Al5〇i2, which is named as yttrium aluminum garnet (YAG). It has been pointed out in this work that the chemical composition lattice structure of YAG differs from the natural minerals Crossulara-Ca3Al2Si3012 and spessartine_Mn3Al2Si3〇i_.

JooderH.J首次非常明確的確定間隔組屬於J1〇3d人工石榴石。同 樣晶格參數a^l2.01±〇.2A與天然的石榴石a~ 1186A相比更大。採 用大尺寸的Y+3與Mn+2—起,這種材料其計量式可以寫成 A3B2(B〇4)3 ’其中A型離子(稀土元素,如鈣、鐵等等),具有十二 面體的配位,其配價數κυ=8,B型離子(矽及部分鋁)具有其配價 KU=4,部分的Α1+3離子具有八面體,配價κυ=6。For the first time, JooderH.J made it very clear that the spacer group belongs to the J1〇3d artificial garnet. The same lattice parameter a^l2.01±〇.2A is larger than the natural garnet a~1186A. Using large-size Y+3 and Mn+2, the metering of this material can be written as A3B2(B〇4)3 'where A-type ions (rare earth elements such as calcium, iron, etc.) have twelve sides The coordination of the body, its valence number κ υ = 8, B type ion (矽 and part of aluminum) has its valence KU = 4, part of the Α 1 + 3 ion has octahedron, the price κ υ = 6.

Yo^era先生創先打開了新型的合成可能,這不僅僅是傳統的 石榴石晶體。長期以來關注的往往是市場漂亮的紅寶石,開發新 的工f結晶成為重要的發展方向,該技術理念在2G世紀已經產 生,高技術與鐳射相結合。 在此必須指出,產生於2〇世紀6〇年代的固態鐳射比紅寶石 Al203.Cr更加有效,一種以單晶為主的YAG_請參照】Mr. Yo^era pioneered the new synthetic possibilities, which are more than just traditional garnet crystals. The long-term concern is often the market's beautiful ruby. The development of new workmanship has become an important development direction. This technical concept has been produced in the 2G century, combining high technology with laser. It must be pointed out here that the solid-state laser produced in the 1960s is more effective than the ruby Al203.Cr, a YAG_ based on single crystal.

Applyphysicsl%2,33卷,第 8 頁 2519,同-雜諸 1963,V34,P3063, 201022411Applyphysicsl%2, Volume 33, page 8 2519, Tong-Mizhi 1963, V34, P3063, 201022411

同-雜諸^切娜^在這-年’第一篇石權石成份从⑽㈣ 專利誕生(請參照Charvat之英國GB1055 〇99專利、Niels〇n J WThe same - miscellaneous ^ Chenna ^ in this - year's first stone stone composition from (10) (four) patent was born (please refer to Charvat's British GB1055 〇99 patent, Niels〇n J W

Bell實驗室之美國US2,979,413專利及BallmanA.之美國us 3,050,407 專利)。 源自含斂的YAG:Nd(請參照Baiiman人之美國us 3,050,407 專利)石榴石成份,其區別在於高效、高透光性及抗熱性,對於製 備更大尺寸的鐳射元件可靠的加工辦法。 於此同時,根據物理學和材料學分析運用原理,實現了“合成” 石榴石(YAG:Nd)。根據不同稀土離子(〇6丨1^1〇^)石榴石的合成 ❹導致擴大了這獨有材料的應用,在1966年詳細的研究運用了有關 在YAG:Ce的順磁共振’公佈於H.Lewis(請參照Journal Apply physics Vol.37N2, P739),其主要結論就是在單晶體形式中採用鈽 為激活劑,同樣顆粒以粉末及含鈽的黃色石榴石粉末形態出現(黃 寶石在珠寶市場是珍貴罕見的)。 對於創造寬頻帶石榴石螢光粉我們有一個技術解決方案。具 有優先權的是荷蘭的著名物理學家G.Blasse在1967年4月29曰 及ABRille在有關陰極射線管的專利(請參照荷蘭N1 67〇6〇95專利) 中。在製造螢光屏中採用了新型的螢光粉(Y,Ce)3Al5012。這五項專 利在不同的國家備受保護’指出G.Blass及A.Brill在此項工作的重 要性。 荷蘭皇家菲利普(Phillips)公司之BlasseG於其美國、英國、 德國及比利時之【Cerium-Activated Yttrium Aluminate Phosphor】 專利(請參照US3,564,322專利,GB1174518專利,DE1764218專利 及Be714420專利)中開闢了新型的彩色影像螢幕的發展,具有輻 射λ=470〜720nm的寬頻帶螢光粉(Y,Ce)3Al5012,最大輻射光譜 、狀=55〇11111。允許透明的多色晝面以及幻燈片建立在電致發光產 生可見光譜次能帶顯示藍色、天藍色、黃色及紅色,對於更多的 6 201022411 顏色平衡以及建立正確的白光發光,有關所提的添加的石榴石螢 光粉’及添加第一種早以熟知的CaaA^SiO^Ce(石權石)螢光粉, 結合兩種材料所製成的寬頻帶輻射,彩色圖像品質具有可複製性 (请參照 BlassGA.Brill JP Apply physics Lett 1967,Vol 11,P53 ) 〇 YAG:Ce螢光粉的公開有創始人GBlasse在當時發表的學術論 文【Luminescent material】(請參照 GBlasse Uuminescentmaterial】U.S. Patent No. 2,979,413 to Bell Laboratories and U.S. Patent No. 3,050,407 to Ballman A. It is derived from the garnet composition of YAG:Nd (refer to the US patent US 3,050,407 of the Baiiman), which differs in high efficiency, high light transmission and heat resistance, and is a reliable method for preparing larger-sized laser components. At the same time, the "synthetic" garnet (YAG: Nd) was realized according to the principles of physics and material analysis. According to the synthesis of different rare earth ions (〇6丨1^1〇^) garnet, the application of this unique material has been expanded. In 1966, detailed research applied to the paramagnetic resonance of YAG:Ce was published in H. .Lewis (please refer to Journal Apply physics Vol. 37N2, P739), the main conclusion is that helium is used as an activator in the single crystal form, and the same particles appear in the form of powder and yellow garnet powder containing yttrium (the topaz is in the jewelry market). Precious and rare). We have a technical solution for creating broadband garnet phosphors. The priority is the Dutch physicist G. Blasse in April 29, 1967 and ABRille in the patent on cathode ray tubes (please refer to the Netherlands N1 67〇6〇95 patent). A new type of phosphor powder (Y, Ce) 3Al5012 is used in the manufacture of fluorescent screens. These five patents are protected in different countries, pointing out the importance of G.Blass and A.Brill in this work. BlasseG of the Royal Phillips of the Netherlands has developed a new type of patented Cerium-Activated Yttrium Aluminate Phosphor (see US3,564,322, GB1174518, DE1764218 and Be714420) in the United States, United Kingdom, Germany and Belgium. The development of the color image screen has a wide-band phosphor powder (Y, Ce) 3Al5012 with a radiation of λ=470~720 nm, and the maximum radiation spectrum, shape = 55〇11111. Allows transparent multi-color enamels and slides to be built on electroluminescence to produce visible spectrum sub-bands showing blue, sky blue, yellow and red, for more 6 201022411 color balances and to establish the correct white light luminescence, Addition of garnet fluorescing powder' and the addition of the first well-known CaaA^SiO^Ce (Shiquanshi) fluorescing powder, combined with two materials to produce broadband radiation, color image quality is reproducible (Please refer to BlassGA.Brill JP Apply physics Lett 1967, Vol 11, P53) 〇YAG: Ce Fluorescent Powder is published by the founder GBlasse at the time published in the academic paper [Luminescent material] (please refer to GBlasse Uuminescentmaterial)

Amstepdam-.Berliu,1994)’以及在日本的螢光粉手冊中也曾記載(請 參照 Phosphors Handbook,lst Edition,1987)。 主要的YAG:Ce材料的出現對於核子物理及閃爍器非常有 _ 效,其非常短時間餘輝(t/lxHT7秒)允許檢測非常高能量輻射。 這樣的樣本’發光組份(Y,Ce)3A15〇i2以及相近類比的組份,猶 如等’在【螢光粉手冊】(請參照Handb〇〇k〇f Phosphors)及在各種工程學校的教學參考書申均可找到。 在這一犄間有關複合材料(及二元組)裝置,以GaP GaAS為主 在紅外線光譜領域有強烈輻射,利用反司托克榮光粉將眼睛看不 見的輻射轉換成可見的紅光魏光或藍光輻射。其相關專利的描 述请參照美國US3,882,215專利、加拿大CA9〇〇62〇專利及 CA900620A 專利。 建立以GaN為基質的新型氮化物材料擬定其發光二極體在短 波次能帶輻射的可見光譜區域(紅外光、紫外光及藍光)。這一材 料在蘇聯工程師B.C阿布拉墨夫邮.她_)所獲准之蘇聯 CCCP635,813 專利中(請參照 B C Ablam〇vCCCp635813 專利) ^出利用司托克螢光粉將GaN結構的部分初級輻射轉換為長波輕 射’構成不同的顏色的白光。 在1994年日本的物理學豕中村修一(s Nakamura)提出了源 ^化銦、氮化鎵的異質結(即ρ·Ν接面)結構,可提升效能(請參 …、s. Naka聰a. Blue laser. Springer Verlag,Beriin,而)。之後沒 201022411 多久,在1995年“Nichia”公司出色的物理學家運用合成了白光發 光二極體。利用寬頻帶螢光粉Y3Al5012:Ce(請參照US3,564,322專 利、GB 1174518專利、DE1764218專利及Be714420專利)以及發 光一極體的合成結構(請參照US 3,564,322專利,GB 1174518專 利,DE1764218 專利及 Be714420 專利)(Grodriewicz W. Uitert W/Light 之 CA 900620 專利、Pankove 之 DE 2444107 專利及 B.CAblamov之CCCP 635813專利)。該理念根據17世紀牛頓的 互補色原理,結合兩種互補色,創造白光輻射。他們根據已知的 材料、結構,以及物理原理申請了專利(請參照S.Nakamura. Blue laserDiode. Springer Verlag,Berlin,1997)。而在熟知的 N5988925 專 利中,仍然存在著下列缺點:1.儀器的發光效率水準不高,對於色 int大於5000K時為1〇〜12流明/瓦特;2.第一部分異質結inN_GaN 異質結的藍光輻射對視覺有不利影響;以及3.運用以固態類型 (Y’Gd.CehAlsOu為基質的單一材料上,不可能複製出暖白發光。 在建立暖白光發光二極體上,因缺乏單組份石榴石結構發光 材料,故長時間受到限制,以单組成份(Gd,Ce)3Al5〇12嘗試建立相 似的發光一極體尚無定論(請參照S.Nakamura. Blue laser Diode q SPringerVerlag,Berlin,1997),此外在一系列的研發工作中從採用 GdsAlsO^開始,這樣單個的螢光粉,在AedredF A所發表之文 章(請參照 Aedred RATrans Brit Ceram Soc .1959.vol 58N4p 199-210)中被否認。 在採用YsAlsOhCe及CaAlSiN^Eu雙組份結構螢光粉來製作 具有暖紅色發光的發光二極體(請參照RyowatT之美國專利申請 案 US2008283801A,2008/11/20 及 Soshchin N 之中國專利申請^ CN 2008 1016492,11.05.2008)中同時對於曾提出的多種石榴^結' 構來獲取暖白發光,中國專利申請案CN20081016492與本發明°有 關,這裡,本發明中引用了相關資料,很可能是因為複雜的技術、 201022411 發光技術參數的不足,迄今為止尚未用 【發明内容】 麟ί缺點,本發明之-目的係提供-種以 乳蟀卹馮丞貝的杈白先發光二極體, 結結構區域中創建具有高發光材料,本中質 x>58〇nm的區域具有撥紅色輕射。 m的疋在 參 φ 為解決上述習知技術之缺點,本發 ===,極體,其可建立非= 二解為 為達上述之目的,本發明之一種以釓鑄鈽為基質 絲f、,其雜在於··雜絲養成份巾添加F·1離 A 子,取代部分石榴石晶格中的氧離子,其化學計量式 1 lyU^CeyhAlsO^-zFz^Nz^ ’該螢光粉經由一氮化鋼鎵 中feGaN )半導體異質結短波激發後可輻射在撥紅色光譜區域賴 為達上述之目的,本發明之一種以釓镥鈽為基質的暖白光發 —二極體,其係以一氮化銦鎵(InGaN)異質結為基質,且具有一 =光轉換器,其可將第一級的藍光輻射發光轉換轉變為暖白光, 、=在於:該發光轉換器的螢光粉顆粒組份如上所述,與有機石夕 相連接,以厚度均勻的形式分佈在該異質結的輕射表面及 ϋ射棱面。 為達上述之目的,本發明之一種以釓鍀鈽為基質螢光粉之製 備=法,用以製備如上所述之螢光粉,其包括熱處理爐料自最初 t ^化材料,其特徵在於:該熱處理是在還原氣體,分三個溫度 階段熱處理,第一溫度階段及11〇〇。〇第二溫度階段T>1250°C, 201022411 第二溫度階段T>133Gt,總時間超過t=12小時,隨後將產品冷 部並用礦物^溶液進行魏,在其表面職薄的細驗叫。 為使貴審查委員能進—步瞭解本發明之結構、特徵及其目 的,兹附關式及較佳具體實關之詳細制如後。 八 【實施方式】 首先,本發明之目的在於消除上述習知石榴石榮光粉的缺 flit 了達觀個目標,本發明之贼麟為基f螢光粉係以I ()縛(Lu)飾(Ce)為基質,其特徵在於:該螢光粉材 Ο F曰-1離子及N-3離子,取代部分石榴石晶格中的氧離子,其化學^ 置式為:啊士私从队-心如’該螢光粉經由一氮化 中 (InGaN )半導體#質結短波激發後可輻射在撥紅色光譜區域範圍 其中’該化學計量式之計量參數值為χ=〇 〇〇〇1〜〇 3 ; y=0.001 〜0.08 ; ζ=〇.〇〇〇ι〜〇 5 原子分率。 其中,該橙紅色光譜區域範圍中最大光譜波長為 ^^=57511111,其主波長々58〇nm。Amstepdam-.Berliu, 1994)' and also in the Fluorescent Powder Handbook in Japan (please refer to Phosphors Handbook, lst Edition, 1987). The emergence of the main YAG:Ce material is very effective for nuclear physics and scintillators, and its very short afterglow (t/lxHT7 sec) allows the detection of very high energy radiation. Such a sample 'light-emitting component (Y, Ce) 3A15〇i2 and similar analog components are like 'in the fluorescent powder manual' (please refer to Handb〇〇k〇f Phosphors) and teaching in various engineering schools. Reference books can be found. In this case, the composite (and two-group) device, with GaP GaAS as the main radiation in the infrared spectrum, uses anti-Stoke glory to convert the invisible radiation into visible red light. Or blue radiation. For a description of related patents, please refer to US Patent No. 3,882,215, Canadian CA9〇〇62〇 patent and CA900620A patent. A novel nitride material based on GaN is established to define the visible region (infrared light, ultraviolet light and blue light) of the light-emitting diode in the short-wavelength energy band. This material was obtained from the Soviet engineer BC Abramoff. She obtained the franchise of the Soviet CCCP 635, 813 patent (please refer to BC Ablam〇vCCCp635813 patent) ^Using Stoke Fluorescent Powder to Partial Primary Radiation of GaN Structure Converted to long-wave light shots 'white light that makes up different colors. In 1994, Japan's physics 豕 Nakamura proposed a heterojunction (ie, ρ·Ν junction) structure of indium and gallium nitride, which can improve performance (please refer to..., s. Naka Cong a) Blue laser. Springer Verlag, Beriin, and). After that, there was no 201022411. In 1995, the excellent physicist of "Nichia" company used the synthesis of white light emitting diodes. A wide-band phosphor powder Y3Al5012:Ce (refer to US Pat. No. 3,564,322, GB 1174518, DE1764218, and Be714420) and a composite structure of a light-emitting body (refer to US Pat. No. 3,564,322, GB 1174518, DE1764218, and Be714420). Patent) (CA 900620 patent of Grodriewicz W. Uitert W/Light, DE 2444107 patent of Pankove and CCCP 635813 patent of B. CAblamov). This concept combines two complementary colors to create white light radiation based on the 17th century Newton's complementary color principle. They applied for patents based on known materials, structures, and physical principles (see S. Nakamura. Blue laser Diode. Springer Verlag, Berlin, 1997). However, in the well-known N5988925 patent, the following disadvantages still exist: 1. The luminous efficiency of the instrument is not high, 1 〇 12 12 watts/watt for color int greater than 5000 K; 2. Blue light of the first partial heterojunction inN_GaN heterojunction Radiation has an adverse effect on vision; and 3. On a single material with a solid-state type (Y'Gd.CehAlsOu), it is impossible to replicate warm white light. In the establishment of a warm white light-emitting diode, due to the lack of a single component The garnet structure luminescent material has been limited for a long time, and it is inconclusive to try to establish a similar luminescent body with a single component (Gd, Ce) 3Al5 〇 12 (please refer to S. Nakamura. Blue laser Diode q SPringerVerlag, Berlin, 1997), in addition to the use of GdsAlsO^ in a series of research and development work, such a single fluorescent powder, in the article published by AedredF A (please refer to Aedred RATrans Brit Ceram Soc. 1959.vol 58N4p 199-210) Densification. In the use of YsAlsOhCe and CaAlSiN^Eu two-component structured phosphors to produce a light-emitting diode with warm red light (see US Patent Application No. US2008283801A, 2008/11/20, by Ryowat T). And the Chinese patent application of Soshchin N (CN 2008 1016492, 11.05.2008) and the various pomegranate structures proposed at the same time to obtain warm white light, Chinese patent application CN20081016492 relates to the invention, here, in the present invention Citing the relevant information, it is probably because of the complicated technology, the lack of illuminating technical parameters of 201022411, so far has not been used [invention content] Lin 缺点 shortcomings, the purpose of the present invention is to provide - a kind of 蟀 蟀 丞 丞 丞 先In the light-emitting diode, a region having a high luminescent material is formed in the junction structure region, and the region of the medium-mass x > 58 〇 nm has a red light shot. The 疋 in the reference φ is to solve the above-mentioned shortcomings of the prior art, the present invention == =, a polar body, which can establish a non-second solution for the purpose of the above, one of the inventions is a sputum cast sputum as a matrix filament f, and the hybrid 在于 杂 丝 丝 丝 丝 丝 丝 丝 丝 丝, replacing some of the oxygen ions in the garnet lattice, the stoichiometric formula 1 lyU^CeyhAlsO^-zFz^Nz^ 'The phosphor powder is excited by a short-wave excitation of a heterojunction of a gallium nitride gallium) Red spectral region In order to achieve the above object, a ruthenium-based warm white light-diode of the present invention is based on an indium gallium nitride (InGaN) heterojunction and has a = optical converter. The first stage of blue light luminescence conversion can be converted into warm white light, and =: the luminescent powder particle component of the luminescence converter is connected to the organic stone as described above, and distributed in the thickness uniformity The light-emitting surface of the knot and the radiant facet. In order to achieve the above object, the present invention relates to a preparation method of a fluorene-based phosphor powder for preparing a phosphor powder as described above, which comprises heat-treating a charge from an initial material, which is characterized by: The heat treatment is a heat treatment in a reducing temperature in three temperature stages, a first temperature stage and 11 Torr. 〇Second temperature stage T>1250°C, 201022411 The second temperature stage T>133Gt, the total time exceeds t=12 hours, and then the cold part of the product is used to carry out the Wei with the mineral solution, and the thinness of the surface is called. In order to enable the review committee to further understand the structure, features and objectives of the present invention, the detailed details of the attached and better specific implementations are as follows. [Embodiment] Firstly, the object of the present invention is to eliminate the lack of flit of the above-mentioned conventional garnet glory powder, and to achieve the goal of the present invention, the thief-based fluorescent powder of the present invention is decorated with I () (Lu) Ce) is a matrix, characterized in that the fluorescent powder ΟF曰-1 ion and N-3 ion replace the oxygen ion in a part of the garnet lattice, and the chemical formula is: sage private team-heart For example, the fluorescent powder can be radiated in the range of the red spectral region after being excited by a short-wavelength of an indium nitride (InGaN) semiconductor. The measurement parameter value of the stoichiometric formula is χ=〇〇〇〇1~〇3. y=0.001 ~0.08 ; ζ=〇.〇〇〇ι~〇5 Atomic fraction. The maximum spectral wavelength in the orange-red spectral region range is ^^=57511111, and its dominant wavelength is 〇58〇nm.

其中’該此與轉之間的原子分率比3〇〇:1〜5:1時,最佳的原 子分率比20:1〜1〇:卜激活劑成份…自〇 〇〇5〜〇 〇8原子分率。,、 其中,該陰離子晶格中的氧離子、rl離子及N.3離子 分率βΜΝ-^ο.οοο^〜〇.25。 ’ 其中,該亂嘗κι及引入原子分率[f-1mn-1]=0001〜〇〇〇5 時’其最大輕射光谱在λ=582ηιη,引入的原子分率 [卩-1]’1]:。^〜0.1時,最大輻射光譜位移至λ=585ηιη。 其中’該螢光粉之色座標值Sx+y>0.82時,其輻射波長值 λ=585〜600nm。 其中,該螢光粉之發光激發光譜位於波長間隔自 λ=420〜500nm,主要是改變釓與镥之間的含量。 201022411 其中’該縣粉之光触大輻射辭波寬^ =135〜138nm。 其中’該螢光粉以超分散顆粒形式製成,且該螢光粉顆粒形 狀呈橢圓形狀’中位線直徑為d5〇=2微米。 以下將簡單闡述-下本發明所提出的解決方案。首先指出, 在本發明所提出的螢光粉中缺乏主要材料成份如:紀;第二、榮光 粉具有,石=立方晶格類型。對於石權石晶格材料及附屬的 lc3d-0 η,、第二、在螢光粉的主要成份中缺乏釔,因此它不屬於 YAG榮光私,第四、有關螢光粉的晶格參數數值的產生方法採用 春:種匕學結構:部分Gd+3被同價態Lu+3⑨Ce+3所替 檑如^㈣、将,二價態$ 〇-2被一價態的氟離子F_1以及三 f iiWi,本發明所提出的螢絲_轉&+3離子作為 、虫县λ^>420 '辰08原子分率,保證短波異質結InGaN材料在 Γ吸收,發光材料分佈在藍色、綠色、橘色以 及、·工色了見7U區域’最大光譜具有^=582肺。 構的ίΐ的_械份巾缺植軒γ+3,目此石權石結 :h光譜輻射料寬,自㈣⑻〜細細或更多; 於100分、;,二大於13〇nm_的半波寬;3.餘暉時間非常短,小 ❹主要-欠G的位銘愈η>0.90的高量子輻射輸出;以及5.波長方面 主要久此帶的位移與主要的激發帶有關。 本發明所提出縣粉的發光性能 =劑光為像這樣的⑽ _連結4f-5d内ί的電頻帶擴散’相關的過渡範圍 激發ΪΪ根對:二::中’主要的c,3輻射 Ce+3雜;沾μ 具有垂直對稱相對於垂直的主要曲線。 及麵識具有聰及2F7/2(激發水準)、2D5/2 u本狀t) ’提升螢光粉的晶格靜電場,Ce+3短波長鋪 11 201022411 位移’當降低晶格靜電場力所引發的Ce+3輻射長波長位移。 吾人在發明過程工作中曾經表示,對於位在輻射光譜帶Ce+3 的機構,首先,主要的最大輻射光譜依附於陽離子晶格螢光粉, 具有自乱離子Gd+3與鑄離子Lu+3之間比率的關係。 其次,螢光粉輻射光譜的結構成份中,異價態替換部分,二 價態的〇_2被—價_氟離子F1以及三價態的Ν·3取代。 通構所構成的光學影響,在本發明中 通過刀析h圖的方法來進行闡述。光譜 ❹ 波長λ~參-二 ❿Among them, the atomic ratio between this and the rotation is 3〇〇: 1~5:1, the best atomic ratio is 20:1~1〇: Bu activator composition...from 〇〇〇5~〇 〇 8 atomic fraction. , wherein, the oxygen ion, the rl ion, and the N.3 ion fraction in the anion lattice are βΜΝ-^ο.οοο^~〇.25. ' Among them, the tampering κι and the introduction of the atomic fraction [f-1mn-1]=0001~〇〇〇5' its maximum light spectrum is at λ=582ηιη, the introduced atomic fraction [卩-1]'1 ]:. When ^~0.1, the maximum radiation spectrum shifts to λ=585ηιη. Wherein the color coordinate value Sx+y> 0.82 of the phosphor powder has a radiation wavelength value of λ = 585 to 600 nm. Wherein, the luminescent excitation spectrum of the phosphor powder is located at a wavelength interval from λ=420 to 500 nm, mainly changing the content between lanthanum and cerium. 201022411 where 'the county's powder light touches the large radiation wave width ^ = 135~138nm. Wherein the phosphor powder is formed in the form of ultra-disperse particles, and the phosphor powder particles have an elliptical shape in shape, and the median diameter is d5 〇 = 2 μm. The solution proposed by the present invention will be briefly explained below. It is first pointed out that in the phosphor powder proposed by the present invention, the main material components are absent; the second, the glory powder has a stone = cubic lattice type. For Shiquanshi lattice material and its attached lc3d-0 η, and second, lack of antimony in the main components of the phosphor powder, it does not belong to YAG Rongguang, and fourth, the lattice parameter value of the phosphor powder. The method of production uses spring: species dropout structure: part of Gd+3 is replaced by the same valence state Lu+39Ce+3 such as ^(4), will, the divalent state $〇-2 is a monovalent fluoride ion F_1 and three f iiWi, the proposed filament_turn & +3 ion as the atomic fraction of worm λ ^ > 420 'chen 08, ensuring that the short-wave heterojunction InGaN material is absorbed in the yttrium, and the luminescent material is distributed in blue, The green, orange, and work colors are seen in the 7U area. The maximum spectrum has ^=582 lungs. ΐ ΐ ΐ 械 械 缺 植 γ γ γ γ + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + Half-wave width; 3. The afterglow time is very short, the small ❹ is mainly - the high quantum radiation output of the y = y > y = 0.90; and 5. The wavelength is mainly related to the main excitation band. The luminescence property of the county powder proposed by the present invention = the light of the agent is such that (10) _ linkage 4f-5d within the electric frequency band diffusion 'related transition range excitation ΪΪ root pair: two:: medium 'main c, 3 radiation Ce +3 miscellaneous; dip μ has a vertical curve with respect to vertical. And face with Cong and 2F7/2 (excitation level), 2D5/2 u this shape t) 'Raining the electrostatic field of the phosphor powder, Ce+3 short wavelength shop 11 201022411 Displacement' when reducing the electrostatic field force of the lattice The long wavelength shift of the Ce+3 radiation induced. In the process of the invention process, we have stated that for the mechanism of the Ce+3 in the radiation spectrum, first, the main maximum radiation spectrum is attached to the cationic lattice phosphor powder, with self-interesting ions Gd+3 and casting ions Lu+3. The relationship between the ratios. Secondly, among the structural components of the fluorescent powder radiation spectrum, the heterovalent substitution portion, the divalent 〇_2 is replaced by the valence-fluoride ion F1 and the trivalent Ν·3. The optical influence of the structure is explained in the present invention by a method of analyzing the h-picture. Spectral ❹ wavelength λ~ --二二

光譜 半波 寬 λ〇. 5, nm 136, 6 136, 1 136,4 136, 5 136, 7 583 發光 亮度Spectral Half-wave width λ〇. 5, nm 136, 6 136, 1 136,4 136, 5 136, 7 583 Luminance Brightness

色溫 K 21281 21002 19691 1 9051 18397 3229 3310 3278 3203 3406 137, 〇 138, 5 21729 3300 ^ί^^!Α15〇1,.5ι 的光:C1〜圖8,其中圖1緣示 的曰丁意圖,圖2繪示表i中樣本2榮光粉的光譜示意圖;圖3 138, 6 20227 20302 3127 3396 12 201022411 表1中樣本3螢光粉的光譜示意圖;圖4繪示表1中樣本4 =粉的光譜示意圖;圖5繪示表丨中樣本5螢光粉的光譜示意 =,圖6繪示表!中樣本6螢光粉的光譜示意圖;圖7緣示表】 中樣本7螢光粉的光講示意圖;圖叫示表丨中樣本8螢光粉的 光譜示意圖。 …由上述之表1中,吾人發現:1.用Γ1及Ν'3替代氧離子,螢 2的最大輻射光譜改齡2.9nm ; 2.最大光譜輻㈣波寬,變化 有在Δ=2ηΐη;3.發光亮度在替換的Γ1及N-3濃度增長的改變下, ,19ίΚ^位中,或更多,高出1G%;以及4.螢光粉的色 >皿減少在ΔΤ=279Κ。 本發明所提㈣螢紐優勢,其特徵在於:在Gd離子及Lu =子的原子比率自嫌1〜5:1時,最佳比彳狀2Q:1〜1():1及以μ ς激,劑’比率為0.005〜0 08原子分率。本發明所提出的榮光粉 =個特徵包括:在陰離子晶格巾氧離子被rl離子及ν_3離子所 取代’數量自[FlMN-3]=0.00005〜0.25原子分率。 在表1巾的域資料組纽發敝成的方法,指&本發明 =的^粉(樣本”具有最大光譜I,9震時的原子分率比 中替換少量&離子,有_«_晶格科 個重要反映波長位移轉變。 疋 ^原子分率增加時,γ原子分率 加了螢光粉的發絲度。 &增 Μ 射實質差別出自其他稀土離子的輻射,例如 ’在f_軌道的内部離子與表面相互制約,通^ 出i的可軒祕5d—辦卿式,可以 這個次能帶在,發光好的波似,nm產生 13 201022411 以下現象:ce+3-〇-2+發光量子—cf v〇-2_^e+3(4F5/2_5D)。 含強烈的吸收光’離子激發返回觸、來的初始狀態,釋放的 量子發光差異在越)〜7〇nm,因此Ce+3的最大輕射光譜在石梅石 立方晶格類型的次能帶上自530〜590mn。在含有整體Ce+3離子中 的輻射轉移,吾人發現最大輻射在立方結構Gd3Al5〇i2自 λ^=580〜585nm,適於橙紅色可見光譜區域。 吾人在發明過程中發現,指出對於色座標值增長至 (】x+y)>0.82日^· ’主波長的輕射自λ=58〇〜595腿不同的輕射光譜 最大數值及主波長的賴射對稱。 吾人同樣指出對於增加氟離子Fl以及Ν-3離子來替換σ 大光譜輻射半波寬增加。 、 联 这疋本發明峨峻絲主要崎勢,其概在於 域的所有整體數值的演色指數Ra>74。 匚 法:ί!?亦揭示一種以釓鑄鈽為基質螢光粉之製備方 ί二二!: 之以釓雜基質螢光粉,首先秤取所需 ❹ ,皿至切靴,保持2〜5小時,然後再以5t/min溫 5 «(Ν2:Η2=ί:5) 持溫速率升⑽職,保 粉狀:出光乾禍中取出並研磨至 一夕酸輪Si=中酸洗,並在營光粉粉末表面塗上 ―,那麼像這樣的:具 14 201022411 盲孔,如果螢光粉的粉末非常細小,d5〇<2微米,那麼會增加光的 散射’在第一次半導體異質結輻射激發時發光亮度降低。 、,“上所述’平均粒控為d5〇=2.00土0.5微米,本發明所提出的螢 ,粉具有高發光亮度,計算螢光粉其他化學成份的關係標準,這 是因為’在文獻中缺乏釓石榴石發光螢光粉的資料,因此利用固 溶體(YoaGdomCeo.oAAlAa螢光粉為基準來比較。 ❹ ❹ 根據其化學成分(Gd/Lu的相互關係),及替換在四面體A1〇 中,氧離子的氟離子F1和氮離子Ν'3引入數量,吾人已經取得^ 光党度水準在72〜76.5%的螢光粉樣本,具有最大輻射光譜 =56lnm ’主要發歧在黃色的可見光譜領域,本發明所提出 光粉發光亮度高於75%,發光亮度非常高。 蛍 實施本㈣之缝_絲賤_之製備絲之一較佳 先秤取如下原物料Color temperature K 21281 21002 19691 1 9051 18397 3229 3310 3278 3203 3406 137, 〇138, 5 21729 3300 ^ί^^!Α15〇1,.5ι Light: C1~Fig. 8, in which Figure 1 shows the intention of Kenting, 2 is a schematic diagram showing the spectrum of the sample 2 glory in Table i; FIG. 3 138, 6 20227 20302 3127 3396 12 201022411 Schematic diagram of the sample 3 phosphor powder in Table 1; FIG. 4 shows the sample 4 in Table 1 = powder Schematic diagram of the spectrum; Figure 5 shows the spectral representation of the sample 5 phosphor in the surface = =, Figure 6 shows the table! Schematic diagram of the spectrum of the sample 6 phosphor powder; Figure 7 shows the schematic diagram of the sample 7 fluorescent powder; the diagram is called the spectrum of the sample 8 fluorescent powder. ... From the above Table 1, we found: 1. Replace the oxygen ions with Γ1 and Ν'3, the maximum radiation spectrum of fluorescein 2 is 2.9nm; 2. The maximum spectral radiance (four) wave width, the change is Δ=2ηΐη; 3. The illuminance of the luminescence is changed by the change of the concentration of Γ1 and N-3, and in the 19 Κ Κ ^ position, or more, 1 G% higher; and 4. The color of the phosphor powder is reduced by Δ Τ = 279 Κ. The invention has the advantages of (4) the highlight, which is characterized in that: when the atomic ratio of Gd ion and Lu = sub is suspected to be 1~5:1, the optimal ratio is 2Q: 1~1():1 and μμ The ratio of the agent is 0.005 to 0 08 atomic percentage. The glare powder proposed by the present invention includes a feature in which the oxygen ions are replaced by rl ions and ν_3 ions in an anion lattice, and the amount is from [FlMN-3] = 0.00005 to 0.25 atomic fraction. In the method of Table 1 of the domain data group, the method refers to & the invention = powder (sample) has the largest spectrum I, 9 atomic ratio of the earthquake when replacing a small amount of & ion, there is _« _ Lattice is an important reflection of the wavelength shift. When the atomic fraction is increased, the gamma atomic fraction is increased by the fluorescence of the phosphor. & Μ Μ 实质 实质 实质 实质 实质 实质 实质 实质 实质 实质 实质 实质 实质The internal ion and surface of the f_ orbit are mutually restricted, and the yin secret 5d----------------------------------------------------------------------------------------------------------------------------------------------- -2+ luminescence quantum-cf v〇-2_^e+3(4F5/2_5D). Contains strong absorption light 'ion excitation returns to the initial state of the touch, the quantum luminescence difference released is ~7〇nm, Therefore, the maximum light spectrum of Ce+3 is from 530~590mn in the sub-band of the pumice cubic lattice type. In the radiation transfer containing the whole Ce+3 ion, we found that the maximum radiation is in the cubic structure Gd3Al5〇i2 λ^=580~585nm, suitable for the orange-red visible spectrum region. I found in the process of invention, pointed out The color coordinate value is increased to (]x+y)>0.82 day^· 'The light wavelength of the dominant wavelength is different from the maximum value of the light-radiance spectrum and the dominant wavelength of the λ=58〇~595 legs. I also pointed out that Increasing the fluoride ion Fl and Ν-3 ions to replace the λ large-spectrum radiation half-wave width increase. 联 疋 疋 疋 疋 主要 主要 主要 主要 主要 主要 主要 主要 主要 主要 主要 主要 主要 主要 主要 主要 主要 主要 主要 主要 主要 主要 主要 主要 主要 主要 主要 主要 主要 主要 主要 主要 主要 主要 主要 主要: ί!? Also reveals a preparation of fluorinated powder based on enamel cast enamel. ί 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二 二, then 5 t / min temperature 5 « (Ν 2: Η 2 = ί: 5) holding temperature rate (10) position, powder: the light out of the dry disaster and grinding to the overnight acid wheel Si = medium pickling, and The surface of the camping powder powder is coated with ―, like this: with 14 201022411 blind holes, if the powder of the phosphor powder is very small, d5 〇 < 2 microns, then it will increase the scattering of light 'in the first semiconductor heterojunction When the radiation is excited, the luminance of the light is lowered. The above-mentioned average particle control is d5〇=2.00 soil 0.5 micrometer, which is proposed by the present invention. The firefly, the powder has a high luminous brightness, and the relationship standard of other chemical components of the fluorescent powder is calculated. This is because the material of the garnet luminescent phosphor is lacking in the literature, so the solid solution (YoaGdomCeo.oAAlAa fluorescent light is utilized). Powder is used as a benchmark to compare. ❹ ❹ According to its chemical composition (Gd/Lu correlation), and replacement in tetrahedral A1〇, the ion number of fluoride ion F1 and nitrogen ion Ν'3 introduced by oxygen ion, we have obtained ^ light The party level is 72~76.5% of the phosphor powder sample, with the largest radiation spectrum = 56lnm 'mainly in the yellow visible spectrum field, the proposed light powder brightness is higher than 75%, and the brightness is very high.实施 One of the preparations for the implementation of the seam of this (4) _ silk 贱 _ is preferred to weigh the following raw materials

Gd203: 48.95 g Al2〇3 : 25.5 gGd203: 48.95 g Al2〇3 : 25.5 g

Lu203 : 4.18 g A1F3.3H20 : 0.92 gLu203 : 4.18 g A1F3.3H20 : 0.92 g

Ce02 :1.55 g AIN : 〇.82 g 將以上原物料充分混和後放入300ml的翁 職入電射域,以π論糾 持4小時’然後再以5〇C/min的升溫速率升溫至 j 5小時’此時加入弱還原氣體(n2:H2=95:5)為仅·厲匕’保持 5°C/min的升溫速率升溫至Τ=ι42οχ:,伴#4、€乳體,然後再以 卻到室溫。 你待4小時’然後自然冷 將掛堝從電爐中取出,然後將螢光粉從 粉狀,用0.1M的HN〇3強酸中酸洗,並在取出並研磨至 50nm的矽酸鋅ZnO.Si〇2薄膜。根據以上會粉粉末表面塗上 為表1中的樣品1。 Μ所製作的樣品即 15 201022411 w ^ 卜田ίϊ明亦揭示—種以氣錄鈽為基質之暖白光發光二極 ^ Γ所述之以為基f螢光粉,該發光二極Ce02 : 1.55 g AIN : 〇.82 g The above raw materials are thoroughly mixed and placed in a 300ml Wengeng electric field, which is held for 4 hours by π theory and then heated to j 5 at a heating rate of 5〇C/min. At this time, add a weak reducing gas (n2:H2=95:5) to the temperature increase rate of 5 °C/min to Τ=ι42οχ:, with #4, €乳, then But to the room temperature. You stay for 4 hours' then naturally remove the hanging from the electric furnace, then the powder is powdered, pickled with 0.1M HN〇3 strong acid, and removed and ground to 50nm zinc ZnO. Si〇2 film. According to the above powder powder surface, the sample 1 in Table 1 was applied. The sample produced by Μ is 15 201022411 w ^ 卜田 ϊ ϊ 亦 亦 亦 亦 亦 亦 亦 亦 亦 亦 亦 亦 亦 亦 亦 亦 亦 亦 亦 亦 亦 亦 亦 亦 暖 暖 暖 暖 暖 暖 暖 暖 暖 暖 暖 暖 暖 暖 暖 暖 暖 暖 暖

體I構她於本發明之申請人在中國專利⑽咖侧AI am the applicant of the present invention in the Chinese patent (10) coffee side A

(請參照上述專利之說明書及圖式,在此不再贅述),安置 石Al2〇3或單晶石夕的導熱基底上,填充有榮光粉轉換層J :隼:ΓΖ:)通常位於圓錐形的蓄光器中,蓄光器將所有 f集到的先引向發光二極體透鏡蓋上,匯出向外_。位於(Please refer to the specification and drawings of the above patents, and will not be described here.) The heat-conducting substrate on which the stone Al2〇3 or single crystal stone is placed is filled with a glory conversion layer J: 隼:ΓΖ:) usually located in a conical shape In the refractory device, the accumulator leads all the f-collected first to the illuminating diode lens cover and retracts outward. lie in

體異質結發光轉換層的表面或棱面,組成自 錄鈽為基質勞光粉顆粒與聚合物相混和,對發光二 吕^見有的石夕酸鹽(有機石夕)合成物折射率可達n=i65~H 升?ί轉換器的外部輻射輸出。以上之半導體 开徠:炎昭、、、t底、畜光器發光轉換器及發光二極體透鏡蓋等 ⑽011()4曝椒_書峨,在此不再 在本發明所提出的以⑽錦為基質之發光二極體中,係以氮 ϊϊί質結為基礎,其發光表面與側面覆蓋著厚度為16〇〜200微 米的發光轉換層。發光轉換層均勻的厚度保證了高均勻度的光及 ⑩,人在發明的過程中看到,對於榮光粉顆粒ί與聚合 〜爲。螢絲顆粒的重量比在6%時所合成的白 非吊_色溫τ>麵0Κ,在增加螢光粉的重量比時,整 輕射顏色為橙黃色調,螢光粉的最佳的重量比 發光二極體的發光亮度以及其高演色性。 k確保了 本發明所指出的以此縳鈽為基質之發光二極體的優勢,其特 徵在於UnGaN IU匕物異質結為基質的半導體 所 立的發光轉換層,將第-級的藍光輻射發光轉換轉建 光,特徵在於:該發光轉換器是由如上所述之 & 組份,與有機石夕聚合物相混和’以厚度均勾的形式分 16 201022411 的輻射表面及輻射棱面,螢光粉顆粒的的重量比6〜70〇/〇。 這裡還應當指出’本發明所提出的以釓錄鈽為基質之發光二 極體採用異質結輻射激發位移在更長的波長更寬,與標準相比 (λ=450〜465nm),本發明所提出的以釓鑄鈽為基質之發光二極體具 有異質結輻射區域自λ=420〜485nm,及必須要強調的是標準的石 權石螢光粉(Yo.wGdo.^Ceo.oAAlsOi2沒有像這樣寬的激發波長。 這樣的高發光亮度異質結需要發光非常高的飽和色及其高量 子輸出所述的發光二極體的色溫2500〜4500K,暖白光的色座標為The surface or the facet of the bulk heterojunction luminescence conversion layer is composed of a self-recorded ruthenium matrix powder mixed with a polymer, and the refractive index of the luminescent acid compound Up to n=i65~H liter? The external radiant output of the converter. The above semiconductor development: Yan Zhao,,, t bottom, animal light luminescence converter and light-emitting diode lens cover, etc. (10) 011 () 4 exposure pepper _ book 峨, here is no longer proposed in the present invention (10) In the light-emitting diode of the substrate, the light-emitting surface and the side surface are covered with a luminescence conversion layer having a thickness of 16 〇 to 200 μm. The uniform thickness of the luminescence conversion layer ensures high uniformity of light and 10, which is seen in the process of the invention, for glory powder particles and polymerization ~. When the weight ratio of the filament particles is 6%, the white non-hanging color temperature τ> surface 0Κ, when increasing the weight ratio of the phosphor powder, the whole light color is orange-yellow, and the optimal weight ratio of the phosphor powder The luminance of the light-emitting diode and its high color rendering. k ensures the advantages of the light-emitting diode of the substrate as indicated by the present invention, characterized in that the UnGaN IU dopant heterojunction is a semiconductor-based luminescence conversion layer, and the first-order blue radiant luminescence Converting and reconstructing light, characterized in that: the illuminating converter is composed of the & component as described above, and is mixed with the organic stone polymer, and is fused to the radiation surface and the radiation facet of 16 201022411 in the form of thickness hooks. The weight ratio of the light powder particles is 6 to 70 〇 / 。. It should also be pointed out here that the light-emitting diode of the present invention proposed by the present invention uses a heterojunction radiation excitation displacement to be wider at a longer wavelength, compared with the standard (λ = 450 to 465 nm), the present invention The proposed light-emitting diode with ruthenium cast ruthenium has a heterojunction radiation region from λ=420~485nm, and it must be emphasized that the standard Shiquanshi phosphor powder (Yo.wGdo.^Ceo.oAAlsOi2 is not as wide as this) Excitation wavelength. Such a high-luminance luminance heterojunction requires a very high saturation color and a high quantum output. The color temperature of the light-emitting diode is 2500~4500K, and the color coordinates of the warm white light are

❿ χ=0·42,y=〇.44。 上述以釓錆鈽為基質之發光二極體之特徵在於:其進一步具 有一圓錐形的球形透鏡蓋(圖未示),係位於該發光轉換器之上 方,該圓錐形的球形透鏡蓋在輻射觀測角2T=60。時, 卜5_咖,功率胸瓦特,光通量㈣〜9Q ^發光強度 本發明所提出之以釓縳鈽為基質之發光二極體,其特徵在 於:對於自功率w=i瓦特至w=2瓦特,其光通量增加至f>15〇 流明,儀器的發光效率η275流明/瓦特。 因此,藉由本發明之以釓鉾鈽為基質之暖白光發光二極體及 /、螢光粉,其在短波半導體InGaN異質結結構區域中創建具 發光材料,本發日月中最具重要的是在WOnm的區域具有撥紅色 輪射’其可建立转寬的寬鮮㈣並具有S演色鎌Ra等優 點,以改善習知暖自光發光二極體及石權石螢光粉之缺點。 ’乃較佳實施例,舉凡局部之變更或修飾而源 ====_㈣該項祕之人所易於推知者,俱不脫 綜上所陳,本案無論就目的、手段與 徵,且其首先個合於料,亦在 專要+ “貴審查委員明察,並析早曰賜予專利,俾嘉惠 17 201022411 社會,實感德便。 【圖式簡單說明】 圖1為一示意圖,其繪示本發明矣] 示音圖。. ㈣1中樣本1螢光粉的光譜 示意=為-示意圖’其綠示本翻表i中樣本2螢光粉的光譜 示意=為—示意圖’鱗示本發1中樣本3螢光粉的光譜 -咅Γ為一示意圖,驗示本發明表1中樣本4螢光粉的光譜 不葸圖。 圖5為一示意圖’其繪示本發明矣]士描_丄 ^ 一立_ 个赞月表1中樣本5螢光粉的光譜 不思圖0 -咅=6為$意圖’其纷不本發明表1中樣本6螢光粉的光譜 不意圖。 圖7為-示意圖’其緣示本發明表!中樣本7螢光粉的光譜 不意圖。 圖8為-示意圖’其繪示本發明表丨中樣本8螢錄的光謹 不意圖〇 【主要元件符號說明】 無。 18❿ χ=0·42, y=〇.44. The above-mentioned ruthenium-based light-emitting diode is characterized in that it further has a conical spherical lens cover (not shown) located above the luminescence converter, and the conical spherical lens cover is irradiated The observation angle is 2T=60. At the time, the self-power w=i watt to w=2 Watts, whose luminous flux is increased to f > 15 lumens, the luminous efficiency of the instrument is η 275 lumens / watt. Therefore, by using the ruthenium-based warm white light-emitting diode and/or phosphor powder of the present invention, the luminescent material is created in the short-wave semiconductor InGaN heterojunction structure region, which is the most important in the present month. It is in the area of WOnm that it has the advantages of red-shifting, which can establish the width and width of the widening (four) and has the S coloring 镰Ra, so as to improve the shortcomings of the conventional warm self-lighting diode and the stone weighting powder. 'It is a preferred embodiment. Anyone who changes or modifies the local source ====_(4) The person who knows the secret is easy to infer, and the case is not inconsistent with the purpose, the means and the levy, and the first The materials are also in the special + also in the "extraordinary review", and the analysis of the early patents, Yan Jiahui 17 201022411 society, real sense of virtue. [Simplified schematic] Figure 1 is a schematic diagram, showing this Inventive 矣] 音音图.. (4) Spectral indication of sample 1 fluorescent powder in 1 = is the schematic diagram 'The green spectrum of the sample 2 is the spectrum of the fluorescent powder in the sample i = _ schematic 'scale' shows the hair 1 The spectrum of the sample 3 phosphor powder is a schematic diagram showing the spectrum of the sample 4 phosphor powder in Table 1 of the present invention. Fig. 5 is a schematic view showing the invention. A _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ The schematic diagram of the present invention shows that the spectrum of the sample 7 phosphor powder is not intended. Fig. 8 is a schematic view showing the sample 8 in the form of the present invention. Light is not intended to honor The main element symbol square DESCRIPTION no. 18

Claims (1)

201022411 十、申請專利範園: 乂-種錢_為基f之螢光粉,其係⑽猶為基質,其特 政在該螢光粉材料成份中添加F-1離子及Ν'3離子,取代部八 石榴石晶格中的氧離子,其化學計量式 σ刀 f f 0為)满〇^鳥2 ’該螢光粉具有一特定201022411 X. Applying for the patent garden: 乂-cultivating money _ is the fluorescent powder of the base f, the system (10) is still the substrate, and its special government adds F-1 ions and Ν'3 ions to the fluorescent powder material. Substituting the oxygen ions in the eight garnet lattice, the stoichiometric formula σ knife ff 0 is) full 〇 ^ bird 2 'the fluorescent powder has a specific 中該其 Ζ=0,0001〜G.5 原子分率。 「· υΐ 0·08 ’ 3.如申請專利範圍第1項所述之以_料 I該橙紅如f __技絲譜錄為^=5751^;^^ 長 λ=580ηπι。 4·如申請專利範圍第!項所述之以乱鑄錦為基質之 盆 中該釓(Gd)與鑄(Lu)之間的原子分率比3〇〇:1〜5:1時 ^ 分率比2〇:i〜i〇:i,激活劑成份Ce+3自0 005〜0 〇8原子分率y、 5.如申請專利範圍第!項所述之以乱鑄飾為基質之榮光粉,盆 中該陰離?自格巾的氧離子、F_i離子及N.3料 ’、 [^=1^=0.00005〜0.25。 刀 6. 如申請專利範圍第1項所述之以釓鉾鈽為基 中該釓勝15:1及引入原子分率[FiMn-i]=〇 〇〇1〜〇 〇〇5時&最 大輻射光譜在λ=582ηηι,引入的原子分率[Γι]气π卜〇 〇5〜〇f時, 最大輻射光譜位移至λ=585ηηι。 .、’ 7. 如申請專利範圍第1項所述之以乳鑄鈽為基質之螢光粉 色座標值Sx+y>〇.82時,其輻射波長值λ=585〜6001^。 、 8. 如申請專利範圍第1項所述之以釓镥鈽為基質之螢光粉,复 發光激發光譜位魏長卩视自λ=·〜5GGnm,主要纽變此^錯; 19 201022411 之間的含量。 9.如申請專利範圍第1項所述之賊麟為基質之螢光粉,其 光譜最大輻射的半波寬λ〇.5=135〜138nm。 、 1〇.如申請專纖圍第1項所述之贼麟為基#之螢光粉, 其中該螢光粉以超分散雜形式製成,且該螢光粉雛形狀呈擴 圓形狀,中位線直徑為d5()=2微米。 11.一種以釓鉾鈽為基質的暖白光發光二極體,其係以一氮化 姻鎵(InGaN)異質結為基質,且具有一發光轉換器其可將第一The Ζ = 0,0001~G.5 atomic fraction. "· υΐ 0·08 ' 3. As stated in item 1 of the patent application, the orange red as f __ technical silk is ^=5751^; ^^ long λ=580ηπι. The ratio of the atomic ratio between the gadolinium (Gd) and the cast (Lu) in the pot of the chaotic cast brocade as described in the scope of the patent item is 3〇〇: 1~5:1, the fraction ratio is 2〇 :i~i〇:i, activator composition Ce+3 from 0 005~0 〇8 atomic fraction y, 5. According to the scope of application of the patent item! The anion is from the oxygen ion, F_i ion and N.3 material of the towel, '^=1^=0.00005~0.25. Knife 6. According to the scope of claim 1 The 釓 win 15:1 and the introduction of the atomic fraction [FiMn-i] = 〇〇〇 1 ~ 〇〇〇 5 & maximum radiation spectrum at λ = 582 ηηι, the introduced atomic fraction [Γι] gas π 〇〇 When 5~〇f, the maximum radiation spectrum shifts to λ=585ηηι. ., ' 7. As shown in the first paragraph of the patent application, the fluorescent pink coordinate value Sx+y> , the radiation wavelength value λ = 585 ~ 6001 ^., 8. If the patent application scope 1萤 釓镥钸 釓镥钸 之 之 , , , , 复 复 复 复 复 复 复 复 复 复 复 复 复 复 复 复 复 复 复 复 复 复 复 复 复 复 复 复 复 复 复 复 复 复 复 复 复 釓镥钸 釓镥钸 釓镥钸 釓镥钸 釓镥钸 釓镥钸 釓镥钸The thief is a matrix of phosphor powder, and the half-wave width of the maximum radiation of the spectrum is λ 〇 5 5 5 5 5 5 5 5 5 5 如 如 如 如 如 如 如 如 如 如 如 如 如 如 如 如 如 如 如 如 如 如 如 如 如a phosphor powder, wherein the phosphor powder is formed in a form of ultra-dispersion, and the shape of the phosphor powder is rounded, and the diameter of the median line is d5 () = 2 μm. Warm white light emitting diode, which is based on an InGaN heterojunction and has a luminescence converter which can be the first 級的藍光輻雜光雜觀紐自發光,特徵在於:該發光轉換 器的螢光粉雌組份如巾請專職圍第丨項所述,與有機石夕聚合 物相連接以厚度均自的形式分佈在該異質結的輻射表面及輕射 棱面。 12.如申請專利範圍第u項所述之以釓縳鈽為基質的暖白光 發光二極體’其中該螢光粉顆粒的重量比為6〜7〇%。 “13.如申請專利範圍第u項所述之以釓鉾鈽為基質的暖白光 發光二極體’其中該發光二極體適用於λ=420〜50〇nm#藍色異曾 結輻射’該發光概||具有暖白色調缝色輻射,其色、 T=2500〜4500K及色座標為χ=〇 42及尸〇 44。 14.如申清專利範圍第^項所述之以釓錆鈽為基質的暖白光 發光二極體’其進—步具有—Ϊ錐形的球形透鏡蓋,係位於該發 光轉換器之上方’該m轉的球猶鏡蓋在練觀_ 2τ=^ 時’發光強度l>50〇〇mcd,功率W=1瓦特,光通量F=8〇〜如沪 明。 /JlL 15.一種以⑽鈽為基質之螢光粉之製法,用以製備如申珠直 利範圍第1項所述之叹_為基質之螢光粉,其包括熱處二爐 分 溫度階段 ,自最㈣氧化材料’其特徵在f該減理是在還原氣體 二個溫度階熱處理,第_溫度階段,第 20 201022411 T>1250°C,第三溫度階段T>1330°C,總時間超過t=12小時,隨 後將產品冷卻並用礦物酸溶液進行酸洗,在其表面形成薄的薄膜 Zn0,Si02。The level of blue light is illuminating, and the characteristic is that the fluorescent powder of the luminescent converter is as described in the article 专, and is connected with the organic stone polymer. The form is distributed on the radiating surface of the heterojunction and the light-emitting facet. 12. The warm white light-emitting diode according to the invention of claim 5, wherein the weight ratio of the phosphor powder particles is 6 to 7% by weight. "13. A warm white light-emitting diode based on yttrium as described in the scope of claim 5, wherein the light-emitting diode is suitable for λ=420~50〇nm#blue different-junction radiation' The illuminating light|| has a warm white tone color radiation, the color thereof, T=2500~4500K, and the color coordinates are χ=〇42 and the corpse 44. 14. As stated in the claim The warm white light-emitting diode of the substrate is 'stepped with a spherical lens cover of a cone-shaped cone, which is located above the light-emitting converter'. The m-turned ball is covered by the mirror _ 2τ=^ 'Luminous intensity l> 50〇〇mcd, power W=1 watt, luminous flux F=8〇~如沪明. /JlL 15. A method for preparing phosphor powder based on (10) ruthenium, for preparing such as Shenzhu Zhili The sigh _ is a matrix of fluorescing powder according to the first item, which includes a heat stage at a temperature of two furnaces, and the most (four) oxidized material is characterized in that the reduction is a heat treatment at two temperature steps of the reducing gas, _temperature stage, 20th 201022411 T> 1250 ° C, third temperature stage T > 1330 ° C, total time exceeds t = 12 hours, then the product is cold And an acid solution with a mineral acid, to form a thin film on the surface thereof Zn0, Si02. 21twenty one
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