TW200422375A - Luminescent material, preferably for LED application - Google Patents

Luminescent material, preferably for LED application Download PDF

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Publication number
TW200422375A
TW200422375A TW092126178A TW92126178A TW200422375A TW 200422375 A TW200422375 A TW 200422375A TW 092126178 A TW092126178 A TW 092126178A TW 92126178 A TW92126178 A TW 92126178A TW 200422375 A TW200422375 A TW 200422375A
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Taiwan
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light
patent application
scope
item
material according
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TW092126178A
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TWI287566B (en
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Hubertus T Hintzen
Yuan-Qiang Li
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Osram Opto Semiconductors Gmbh
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    • H01L33/48Semiconductor devices having potential barriers specially adapted for light emission; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof characterised by the semiconductor body packages
    • H01L33/50Wavelength conversion elements
    • H01L33/501Wavelength conversion elements characterised by the materials, e.g. binder
    • H01L33/502Wavelength conversion materials
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Description

200422375 玖、發明說明: (一) 發明所屬之技術領域 本發明係關於一種可在光譜區域的uv -藍光部分中激 發之發光材料;更特別的是,其不但是專門針對光源用之 磷光劑,較佳爲其用於發光二極體(LED)。該磷光劑的類別 屬於經稀土活化的氧氮化矽類。 (二) 先前技術 至今,白光LED已藉由將發藍光的二極體與發黃光磷 光劑結合而達成。此一組合具有差的色彩重現性,但是, 其可藉由使用一紅光-綠光-藍光系統(RGB)而明顯地改善。 此系統使用例如一紅光及藍光發光器與一發綠光的鋁酸鹽 磷光劑(如SrAl 204 : Eu或BaAl 204 : Eu,其可將Μη加入至 Eu,其發光最大値在約520奈米處)組合,參見US-A 6 278 1 3 5。但是,這些鋁酸鹽的激發位置及發射帶並非最理想。 它們必需由範圍在3 30至400奈米的短UV激發。 新穎引入注意的發光材料爲摻雜Eu2 +的α_塞隆(s i a 1 on) 材料。它們具有+ + 結構,其中Μ爲
Ca或γ或稀土金屬。t値則以m/val+提供,其中val+爲離 子Μ的價電荷。例如,M = Sr2 +的val+値爲2。因此,可完全 補償整個結構的電荷。更詳細的細節可參見例如”摻雜Tb、 C e或E u的α-塞隆材料之發光性質π,由〗·凡克瑞弗(v a η Krevel)等人,J. Sol. St. Chem·, 2002 年 4 月,ρ.19-24 ; 及亦可參見n共摻雜Ca及稀土金屬的α-塞隆陶瓷之製備及 發光光譜·,,由R.-J·夕(Xie)等人在J· A. Ceram· Soc. 200422375 2002,ρ·1 229 - 1 2 34,2002 年 5 月;及進一步在 US-Pub 2002 / 0043 9 26中,此些參考資料全部關於α—塞隆型式的ca- 塞隆。此時並不熟知其它型式的塞隆。 (三)發明內容 本發明之目的在於提供一種如申請專利範圍第1項之 前言的新穎發光材料。進一步目的在於提供一種具有經細 微調諧的發光之磷光劑,其可有效率地由UV /藍光輻射激 發。再進一步目的爲提供一種磷光劑,其可與至少一種LED 使用在照明裝置中作爲光源,該LED會發射範圍從3 6 0至4 7 0 奈米的一級輻射,此輻射可藉由已曝露至來自LED的一級 輻射之磷光劑而部分或完全轉換成波長較長的輻射。又進 一步目的爲提供一種可發射白光,特別是具有高彩色表現 的照明裝置。仍進一步目的爲提供一種如LED裝置般高效 率的照明裝置,其在3 6 0至470奈米的範圍有良好的吸收 且容易製造。 這些目的可各別藉由申請專利範圍第1及1 0項所表明 的特徵而達成。特別優良的結構則提供在相依的申請專利 範圍中。 該轉換至少可藉由氧氮化物磷光劑(其源自於經Eu活 化或經Eu,Μη共活化的鋁酸鹽種類)的輔助而達成。更詳細 的是,先述技藝之缺點可藉由將氮摻入MA104: Eu(M = Ca、Sr、 B a )中而克服,此可產生一氧氮化物磷光劑,通常且較佳地 維持該鱗矽石結構。但是並不排除其它結構。更特別的是, (A10) +部分由(SiN) +置換而提供一共通組成:MAl2_xSix04. 200422375 XNX ·· (Eu 或 Eu,Mn )。x 値設定爲 〇〇· 0〇2 且至多 X=1 · 5。與 先前提及之先述技藝的α-塞隆型式結構(其來自氮化物 s i…4)比較’於本文之結構更像衍生自s丨〇2改質的氧化物, 更特別佳的是衍生自鱗矽石結構。 •比較上’ α-塞隆材料顯示出一種所謂的氮化物結構, 換句話說它們以S i 3Ν4爲主而有部分S i - Ν由A 1 - 0及/或由 A1-N置換。追些不同的結構會造成不同的發光行爲,因爲 在α -塞隆及鱗砂石中可能的活化位置在與週圍離子的局部 交互作用中強烈地不同。 在Ca作爲 Μ的主要組分之實例中,較佳的値爲 O.Ol^x^O.l。在Ba或Si.作爲Μ的主要組分之實例中,較 佳的値爲0 · 1 · 7。氮之摻入可增加共價鍵結及配位場 分裂的程度。因此,此可導致激發及發射帶偏移至較長的 波長(與氧化物晶格比較)。所獲得的磷光劑顯示出具有高 化學及熱穩定性。全部相關性質之更擴大的細微調諧可藉 由使用陽離子Μ而獲得,此可藉由結合數種Μ金屬(特別是 Sr及Ba),藉由進一步內含Ζη作爲部分的陽離子Μ(較佳爲 10-40莫耳%),及/或$丨至少部分由〇6置換(較佳爲5-25 莫耳%)及/或Α1由Ga置換(較佳爲5-25莫耳%)而達成。較 佳的是,對發射綠光的材料來說,該金屬Μ主要爲Ba及/ 或Sr,且對發射藍光的材料來說主要爲Ca。摻雜至陽離子 Μ的Eu量在Μ的0.1至25%間,較佳爲在2至15%之間。 此外,當進一步摻雜Μη來細微調諧相關聯的性質時’其可 能的摻雜量較佳爲至多Eu的50%。 200422375 因爲這些材料可將uv-藍光輻射轉換成藍-綠光(由於 低能量激發帶),它們可例如應用在白光光源(例如燈)中, 特別是以主要發射藍光的LED(典型爲可發射約43 0至470 奈米的G a N或I n g a N )與發射紅光的磷光劑之結合爲主的光 源。合適的發射紅光之磷光劑爲摻雜Eu的氮化矽材料,如 M2Si5N8(M = Ca、Sr、Ba),參見例如 WO 01/40403。亦可應 用於有顏色的光源。 (四)實施方式 以實例說明之,本文描述一類似於在WO 0 1 / 40403中 所使用的結構,將其使用在與InGaN晶片一起的白光LED 中。此一白光光源的結構特別顯示在第1 a圖中。該光源以 InGaN型式的半導體構件(晶片丨)爲主,其具有400奈米的 波峰發射波長且具有第一及第二電連接2,3,其埋入一不透 明的基礎外罩8之凹處區域9中。連接3之一經由連結電 線4連接至晶片1。該凹處具有邊壁7,其提供作爲晶片丄 之藍光一級輻射的反射器。以封裝化合物5塡充該凹處9, 該化合物包含一矽酮鑄模樹脂(或環氧鑄模樹脂)作爲其主 要組分(較佳爲多於80重量%),且進一步包含磷光顏料6(較 佳爲少於1 5重量% )。尤其是,亦更含有小量的甲基醚及氣 相二氧化矽。該磷光顏料爲三種顏料(其可發射藍光、綠光 及紅光,而該綠色磷光劑乃根據本發明)之混合物。 第lb圖顯示出一具有半導體構件i〇的光源之具體實 施例,其中該轉換成白光可藉由直接塗佈至各別晶片的磷 光劑轉換層丨6而實現。在基材11之頂端上,有一接觸層12、 一 8 - 200422375 一鏡子1 3、一 LED晶片14、一濾光器15及一隣光劑層16, 該憐光劑層可藉由該LED的一級輻射激發而將該一級輻射 轉換成可看見的長波輻射。此結構單位由塑膠鏡片1 7包圍。 僅闡明該二歐姆接觸的上接觸器1 8。該LED的一級UV輻射 約4 0 0奈米,而二級輻射則由根據本發明的M (i 。> A 12. xSi X04.XNX : D。第一磷光劑發射,D爲Eu或Eu,Mn。特別佳 的是使用BaAl2.xSix04.xNx: (10%)Eu2+,其發射約525奈米 (或在調諧的一般式語言中,c = 0. 1及D = Eu),且第二磷光 劑可使用發射橙-紅光的次氮基矽酸鹽。 第2圖顯示出一照明裝置20。其包含一共同載體21, 其黏著性地黏結至一立方體外罩2 2。其上邊提供一共同遮 蓋物2 3。該立方體外罩具有一些可各別容納半導體構件24 的切口。它們爲可發射藍光的發光二極體,其具有約450 至470奈米的發射波峰。該轉換成白光可經由安排在全部 表面上之易受藍光輻射影響的轉換層25而發生。這些包括 該外罩、遮蓋物及載體的側壁之內部表面。該些轉換層25 由可在紅光光譜區域中發射的磷光劑與使用根據本發明在 綠光光譜區域的磷光劑所組成,且與不吸收一級輻射藍光 的部分一起主要混合成白光。 使用 Eu203 (純度 99.99%)、BaC03(純度 >99.0%)、 SrC03(純度 >99.0%)、CaC03(純度〉99.0%)、Al2〇3(純度 99.9%)、3丨02及Si3N4f爲商業上可購得的起始材料,用來 製造本發明之新穎的磷光劑。利用行星式球磨機,將該些 原始材料在異丙醇中,以適當的量均相溼式混合4 - 5小時。 200422375 在混合後,在火爐中乾燥該混合物且在瑪瑙硏缽中硏磨。 隨後,在1100-1400 °c之還原氮/氫大氣氛下,於水平管爐 中,在鉬坩堝內燒製該些粉末。在燒製後,利用粉末X -射 線繞射(銅K - α線)標出該些材料的特徵。 全部的樣品皆顯示出在UV -藍光之激發下有有效率的 發光,其在藍光(在M = Ca的實例中)中具有最大發射,特別 是435至445奈米;或綠光(對M = Sr或Ba來說),特別是 在Ba的實例中爲495至530奈米,及在Si·的實例中爲515 至575奈米。可在第3及4圖中看見二種發射及激發光譜 的典型實例。第3圖顯示出具有不同X値的SrAl2 xSix〇4. XNX : Eu之發射光譜及激發光譜。第4圖顯示出具有不同X 値的BaAl2.xSix04.xNx: Eu之發射/激發光譜。 藉由變化氮的量,該發射可在495_575奈米的範圍內 偏移。特別是’Sr對偏移敏感(第3圖),同時該激發帶的 頂_可從低於400奈米向上偏移直到430至465奈米,較 佳爲至440奈米’參見M = Ba (第4圖)。所觀察到之至較長 波長的偏移爲Eu 5d帶在較低能量處的重心與Eu 5d帶的 較強配位場分裂之結果。 額外的細微調諧可藉由將Zn摻入陽離子Μ作爲一添加 物(較佳地不多於3 0% ),且至少部分的A 1由G a置換(較佳 地不多於25%),及/或S i由Ge置換(較佳地不多於25%)而 200422375 表1 原始材料 等級 MC〇3(M = Ca、Sr、Ba) ^99^. 0% Si02 氣相二氧化矽0X50 γ- A 12〇3 >99 · 995 Si3N4 β 含量·· 2 3 . 3 %,0 〜0 . 7 % Eu2〇3 99 . 99% 在下列中’提供 MAl2.xSix〇4 xNx: (i〇%)Eu2+(M = Ca、Sr、 φ Ba )之合成程序。可能的起始材料顯示在表1。 全部的氧氮化物磷光劑(包括鱗矽石)皆根據下列反應 方程式(忽略氣相)來合成: (1-y)MC03+(2-x)/2 Al 203 + x/ 4 Si3N4 + x/4 Si02 + y / 2 E u 2 0 3 M1.yEUyAl2.xSix〇4.xNx 其中M = Ca、Sr、Ba(單獨或以組合)。一實例爲y = 〇 . }。 例如’組成物B a .9 E u。· ! A 12 · x S i x 04 · x N x則顯示在下列表 鲁 2中。 表2(單位 :克) X値 BaC03 ai2o3 Si3N4 Si02 Eu2〇3 0.3 3.497 1.689 0.205 0.088 0 . 343 0 . 5 3.500 1.492 0.342 0.146 0.343 詳細的實驗結果顯示出該些憐光劑的發光性質事實上 200422375 幾乎與$丨02含量無關。但是,減低適當量的Si02含量(即, 其可減低最高經計算的S i 02量之1 / 6 0 )會強烈地增加相純 度和效率。 在含有小量H2(10%)之還原大氣氛N2下,在1100-1 400°C的水平管爐中,於Mo ‘坩堝內燒製該些粉末混合物數 個小時。 闡明3丨02減低的角色之樣品的進一步激發及發射光譜 則顯示在第5至8圖中。 根據第5圖的具體實施例:Ba^EunAU^O^N,, 其x = 〇.3且無減少Si02。對發射光譜來說,以λεχ^440奈 米激發該磷光劑及在Xmc)n = 5 3 0奈米處監視該激發光譜。其 主要相具有BaAl 204結構。 根據第6圖的具體實施例:Bao^Euo.MUixO^Nx, 其x = 0.3且Si02量減低至經計算的Si02量之1/4(λεχ。=440 奈米,Xmc)n =530奈米)。其主要相具有BaAl204結構。 根據第7圖的具體實施例:BauEunAUixO^N,, 其χ = 0·3且Si02量減低至經計算的Si02量之1/16(λεχ。=440 奈米,Xm()n =530奈米)。其主要相具有BaAl204結構。 使用Si3N4作爲根據下列反應[1]的(SiN)+來源: MC03+(2-x)/2 A 1 203 + x/ 4 Si3N4 + x/4 S i 02->ΜΑ 12.XS i X04-XNX (+C02t) (M=Ca、Sr、Ba)° 隨著原子半徑從Ba減小至Ca,已發現利用此反應來 將(A10) +由(SiN) +置換會變得更困難。晶格參數結果顯示出 N在具有鱗矽石結構的BaAl 204中之最大溶解度爲約P0 . 6。 200422375 第9圖顯示出在具有鱗矽石結構之BaAl2.xSix04.xNx的單位 晶格體積與X値間之關係。如所預期,如與A 1- 0距離比較 S i - N距離較小,該單位晶格體積會隨著X增加而減少,如 顯示在第9圖。對明顯大於0 . 6的X値來說,該單位晶格 體積仍然幾乎固定,且可觀察到二次相。 如此,可由鋁酸Ba且X最高約0 . 6而不需要調整S i 02 量而達成好的結果。 好的結果亦可從鋁酸S r看見。S i 02含量之減少(表示 爲y量)會產生非化學計量的MAl2.xSix-y04.x.2yNx: Eu型式 之鋁酸鹽,較佳爲y^O . 25x。最佳性能可隨著修正Si02而 達成,且X最高爲0 . 5。對鋁酸Ca來說亦相同,但是較小 的X値較佳地低於0.05。 現在更詳細地討論MAl2.xSix04.xNx: 10%Eu2+的發光性 質。第 8 圖顯示出 MAl2.xSix04.xNx: Eu2+(M=Sr,Ca)的激發 及發射光譜。Si 02含量不減少。更詳細來說,第8a圖顯示 出SrAl2.xSix〇4.xNx: Eu2+(10%)的激發及發射光譜;且第8b 圖爲CaAl2.xSix〇4.xNx: Eu2 + (10%)的激發及發射光譜,每個 具有不同的X。 與在MAl2.xSix04_xNx的單位晶格體積與X値間之關係 的結果相符合,該發射帶依陽離子而或多或少地偏移至較 長的波長。在Ba的實例中,該偏移典型地從495至53 0奈 米;在S r的實例中,該偏移典型地從5 1 5至5 7 5奈米;及 在Ca的貫例中,該偏移典型地從440至445奈米。對 BaAl2.xSix04.xNx: (1〇%)Eu2 +來說,隨著摻入氮的X含量增 200422375 加,該發射帶會從約4 9 7偏移至5 2 7奈米。因此,該激發 帶的位置會從3 8 5偏移至42 5奈米。 對 MAl2.xSix04.xNx ·· ( i〇%)Eu2 +來說,Μ 爲 Sr 或 Ca 的 至少一種’(S i N ) +的量基本上不增加發射及激發波長,因 爲在晶格參數上幾乎無觀察到偏移。在M = Ca的實例中,Eu 發射帶的最大偏移少於1 0奈米,此與摻入小量的氮之事實 相符合。因此,小量的(SiN) +摻入僅可對Eu2 +離子的局部 配位發揮弱的影響。此討論經了解爲加入正常化學計量的 Si02 量。 但是,非常驚人的結果是,在一些實例中,可優良地 使用在化學計量下的S i 02量。減少在反應(1 )中的s i 02量 對 N之摻入及對發光性質的效應在 SrAl2.xSix〇4_xNx : E u2 + ( 1 0 % )的實例中最明顯。此理由尙未完全了解。當應該 使用在反應(1)中的Si02量採用爲較低的因子60時,已發 現所增加的(S i N )+量可摻入具有塡塞的鱗矽石結構之 S r A 1 204晶格中。最大溶解度爲x^O · 5 (表1 )。摻入n的結 果爲該Eli發射帶會偏移至較長的波長,最高爲575奈米(第 3圖)。在4 3 0奈米處之明顯的激發肩狀物則顯露在氮的最 大溶解度U = 〇 . 3…0 · 5 )處’如顯示在第3圖。 除了來自鱗矽石的結構外,來自3]^丨八12〇31^結構的結 構亦可能。此化合物已由史尼克(Schni ck)在1 998年發現。 其與LnSi3N5(其中1^ = 1^、〇6、?]:、_)型式的矽酸鹽氮化 物同位。 (五)圖式簡單說明 -14- 200422375 第1圖顯示出一種可提供作爲白光光源的半導體構件 (LED ) ’其含鑄模樹脂圖(第丨a圖)及不含鑄模樹脂圖(第j b 圖); 第2圖顯示出含有根據本發明之磷光劑的照明裝置; 第3圖顯示出根據本發明之磷光劑的發射光譜及反射 光譜; 第4至8b圖顯示出根據本發明之進一步磷光劑的發射 光譜及反射光譜; 第9圖顯示出在體積單位晶^格與X値間之關係。 元件符號說明 1 晶片 2 第一電連接 3 第二電連接 4 連結電線 5 封裝化合物 6 磷光顏料 7 邊壁 8 不透明的基礎外罩 9 凹處 10 半導體橇件 11 基材 12 接觸層 13 鏡子 14 LED晶片 濾光器 磷光劑層 塑膠鏡片 上接觸器 照明裝置 共同載體 立方體外罩 共同遮蓋物 半導體構件 轉換層 - 1 6 -

Claims (1)

  1. 200422375 拾、申請專利範圍: 1 . 一種發光材料,較佳爲一種用於led應用的憐光劑,其 可在360至470奈米的UV-藍光區域中激發,其特徵爲 具有共通組成MAl2.xSix〇4.xNx之摻雜Ειι的宿主晶格,其 中Μ爲至少一種選擇自於Ca、Sr、Ba的鹼土金屬族,其 中x20.00 2且x51 . 5,較佳的是X低於0 . 7,而Ειι的比 例爲Μ的0 . 1至2 5 %。 2 .如申請專利範圍第1項之發光材料,其中該宿主晶格來 自一鱗矽石結構。 3 ·如申g靑專利範圍第1項之發光材料,其中μ爲總及/或鎖 ,以達成發射綠光。 4 ·如申請專利範圍第丨項之發光材料,其中μ爲鈣,以達 成發射藍光。 5 ·如申請專利範圍第!項之發光材料,其中μ爲這些金屬 的至少二種之混合物, 6 .如申s靑專利範圍第1項之發光材料,其中μ額外包含& ’較佳爲最高40莫耳%。 7 ·如申請專利範圍第i項之發光材料,其中a丨由Ga完全 或部分置換。 8·如申請專利範圍第1項之發光材料,其中由Ge完全 或部分置換’較佳爲不多於2 5%。 9 .如申請專利範圍第丨項之發光材料,其中該基材材料進 一步摻雜Μη,該共摻雜的Mn量較佳爲該Eu摻雜物的至 多最高50%。 200422375 1 0 . —種具有如申請專利範圍第1至9項中任一項之發光材 料之光源(20)。 1 1 .如申請專利範圍第1 〇項之光源,其中該一級發射光爲藍 光’且如申請專利範圍第1至9項之發光材料可與其它 磷光劑結合(特別是發射紅光的磷光劑),以將該一級發 射光部分轉換成較長波長的二級發射光,而造成發射白 光。 1 2 ·如申請專利範圍第1 〇項之光源,其中該一級發射輻射爲 UV,且將如申請專利範圔第1至9項之發光材料與其它 磷光劑(特別是發射紅光及藍光的磷光劑)結合,以將該 一級發射輻射轉換成較長波長的二級發射光,以造成發 射白光。 1 3 .如申請專利範圍第1 〇項之光源,其中該光源爲一種含有 至少一 LED的照明裝置。
    -1 8 -
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DE60307411T2 (de) 2007-03-29
US7485243B2 (en) 2009-02-03
EP1438364B1 (en) 2006-08-09
US20060033081A1 (en) 2006-02-16
TWI287566B (en) 2007-10-01
JP3906224B2 (ja) 2007-04-18
EP1438364A1 (en) 2004-07-21
WO2004029177A1 (en) 2004-04-08
CN1596292A (zh) 2005-03-16
JP2005529229A (ja) 2005-09-29
EP1413619A1 (en) 2004-04-28
DE60307411D1 (de) 2006-09-21
WO2004029177A8 (en) 2004-06-03
ATE335799T1 (de) 2006-09-15
CN1311055C (zh) 2007-04-18

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