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TW201006004A - A photonic crystal equipped solid state light-emitting component - Google Patents

A photonic crystal equipped solid state light-emitting component Download PDF

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TW201006004A
TW201006004A TW97129024A TW97129024A TW201006004A TW 201006004 A TW201006004 A TW 201006004A TW 97129024 A TW97129024 A TW 97129024A TW 97129024 A TW97129024 A TW 97129024A TW 201006004 A TW201006004 A TW 201006004A
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Taiwan
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photonic crystal
epitaxial film
light
array
solid
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TW97129024A
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Chinese (zh)
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TWI443857B (en
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Zhong-Xiang Lin
chang-zhi Yu
Rui-Yan Cai
Hong-Wen Huang
hao-zhong Guo
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Luxtaltek Corp
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Abstract

This invention is a photonic crystal equipped solid state light-emitting component. It comprises a baseboard, a opto-semiconductor epitaxial film formed on the baseboard for generating a pre-determined spectrum, an electrode unit that connects to the opto-semiconductor epitaxial film, a compound type reflective lens of a univariate photonic crystal that is positioned in between the opto-semiconductor epitaxial film and the baseboard mainly for the electrode unit to make electrical contact. The opto-semiconductor epitaxial film has a light exiting face and a back light face that opposites to the light existing face and is connected to the baseboard; and a positive/negative interface that forms in between the light exiting face and the back light face. The opto-semiconductor epitaxial film has a photonic crystal formed at the light exiting face. The photonic crystal is either a two-dimensional photonic crystal or a kind of photonic crystal. The electrode unit provides the electrons and electric holes of the opto-semiconductor epitaxial film to combine with the electrons and electric holes generated by the positive/negative interface.

Description

201006004 九、發明說明: 【發明所屬之技術領域】 本發明是有關於一種固態發光元件(solid_state Ught emitting device),特別是指一種具光子晶體(Photonic crystal ;簡稱PCs)的固態發光元件。 【先前技術】 於固態發光元件相關領域中’發光二極體(LED)因具備 有體積小、重量輕、反應速度快等優點’而使得其逐漸地 取代傳統的鎢絲燈(incandescent)及螢光燈(fluorescent)等光 源並作為照明設備使用。目前常見的應用可見有大型戶外 顯示看板、交通指示燈號,以及液晶顯示器背光滹等。 而為了實現如汽車車燈、投影機用光源等更高亮度需 求的應用,常見的改善方式,可見有藉由粗化出光面的技 術手段,亦或藉由在背光面形成分散式布拉格反射鏡 (distribution Bragg reflector ;簡稱 DBR)或一維光子晶體等 技術手段,以增加LED之出光面的光取出率(extraction efficiency)並提昇其發光亮度。 參閱圖 1,Aur0lien David 等人於 APPLIED PHYSICS LETTERS 88,133514 (2006)的 Photonic crystal laser lift-off GaN light-emitting diodes —文中,揭示出一種具有二維光 子晶體(two-dimensional photonic crystal;簡稱 2DPCs)的藍 光發光二極體1。該發光二極體1之製作方法是簡單地說明 於下。 在一形成於一藍寶石(sapphire)基板(圖未示)上之以 201006004BACKGROUND OF THE INVENTION 1. Field of the Invention This invention relates to a solid state light emitting device, and more particularly to a solid state light emitting device having a photonic crystal (PCs). [Prior Art] In the field of solid-state light-emitting devices, 'light-emitting diodes (LEDs) have gradually replaced the traditional incandescents and fires because of their small size, light weight, and fast response speed. A light source such as a fluorescent lamp is used as a lighting device. At present, common applications include large outdoor display billboards, traffic indicator numbers, and LCD backlights. In order to achieve higher brightness requirements such as automotive lights, projectors, etc., the common improvement methods can be seen by the technique of roughening the light surface, or by forming a decentralized Bragg mirror on the backlight surface. (distribution Bragg reflector; referred to as DBR) or one-dimensional photonic crystal and other technical means to increase the light extraction efficiency of the LED light-emitting surface and enhance its luminous brightness. Referring to Figure 1, Aur0lien David et al., Photonic crystal laser lift-off GaN light-emitting diodes in APPLIED PHYSICS LETTERS 88, 133514 (2006), reveals a two-dimensional photonic crystal (2DPCs). ) blue light emitting diode 1 . The manufacturing method of the light-emitting diode 1 is simply described below. On a sapphire substrate (not shown) on 201006004

GaN為主並具有正負接面(p_n juncti〇n)的蟲晶媒〗丨上,依 序形成複數由Ru〇2/Ni/Ag所構成並相間隔設置的p_電極12 、一圍繞該等p-電極12的Si02層13,及一形成於該Si02 層13上的金(Au)層14 ;後續,將該金層14轉貼到—ain 陶瓷基板15上並利用雷射剝離法(laser Hft〇ff,簡稱ll〇) 將該磊晶膜11自該藍寶石基板(圖未示)移除;進一步地, 利用反應式離子蝕刻法(reactive i〇nic etching,簡稱RIE)於 該遙晶膜11上形成一二維光子晶體16 ;最後,於該二維光 子晶體16上形成一 n_電極17以完成該發光二極餿1q 该二維光子晶體16是一呈六邊形排列的圓形凹槽陣列 ,且該發光二極體1的發光波長約430 nm。該二維光子晶 體16的晶格常數(iattice c〇nstant,簡稱幻為215 ,填充 率(纽1丨吨&(^〇1*,簡稱〇為0_38(即,凹槽直徑為8111111;相 鄰凹槽間距為134 nm)。 雖然該發光二極體1可利用該二維光子晶體16控制場 型與發散角的變化,藉以提高整體發光二極體之輸出的發 光亮度》然而,Aui^lien David等人所揭示的二維光子晶體 16只能控制場型與增加光輸出功率,卻無法降低發光光源 之光譜訊號峰的半高寬。 經上述說明可知,降低發光光源之發光訊號峰的半高 寬值以提昇發光亮度,是固態發光元件相關領域者所待突 破的課題。 【發明内容】 <發明概要> 201006004 本發明主要是選擇二維光子晶體結構及類光子晶體 (photonic quasi crystal ;簡稱 PQC)結構其中一者,來與— 維光子晶體(〇ne_dimensional photonic crystal ;簡稱 lDPCs)On the arsenic medium of GaN-based and having positive and negative junctions (p_n juncti〇n), a plurality of p_electrodes 12 composed of Ru〇2/Ni/Ag and arranged at intervals are formed in sequence, and one surrounds the same a SiO 2 layer 13 of the p-electrode 12, and a gold (Au) layer 14 formed on the SiO 2 layer 13; subsequently, the gold layer 14 is transferred onto the -ain ceramic substrate 15 and subjected to laser lift-off (laser Hft) 〇ff, abbreviated as 〇 〇), the epitaxial film 11 is removed from the sapphire substrate (not shown); further, reactive ion etching (RIE) is applied to the remote crystal film 11 Forming a two-dimensional photonic crystal 16 thereon; finally, forming an n-electrode 17 on the two-dimensional photonic crystal 16 to complete the light-emitting diode 1q. The two-dimensional photonic crystal 16 is a circular concave arranged in a hexagonal shape. The array of grooves, and the light-emitting diode 1 has an emission wavelength of about 430 nm. The lattice constant of the two-dimensional photonic crystal 16 (iattice c〇nstant, referred to as 215, the filling rate (New 丨 ton & (^ 〇 1 *, 〇 〇 is 0_38 (ie, the groove diameter is 8111111; phase The adjacent groove pitch is 134 nm. Although the light-emitting diode 1 can control the variation of the field type and the divergence angle by using the two-dimensional photonic crystal 16, the luminance of the output of the overall light-emitting diode can be improved. However, Aui^ The two-dimensional photonic crystal 16 disclosed by Lien David et al. can only control the field type and increase the optical output power, but cannot reduce the full width at half maximum of the spectral signal peak of the illuminating light source. According to the above description, the illuminating signal peak of the illuminating light source is reduced. The invention relates to a subject of a solid-state light-emitting device, which is a subject of breakthrough in the field of solid-state light-emitting devices. [Summary of the Invention] The present invention mainly selects a two-dimensional photonic crystal structure and a photonic crystal (photonic quasi) Crystal; abbreviated as PQC) structure, one of which comes with - 维ne_dimensional photonic crystal (referred to as lDPCs)

搭配使用’藉以降低光譜訊號峰的半高寬。其主要原因在 於’利用具備有較寬的角度、較窄的波長與無吸收問題等 優點的一維光子晶體作為反射鏡,同時配合具備有控制場 型之特點的二維光子晶體及類光子晶體其中一者的辅助, 可有效地達到窄化發光訊號峰之半高寬的目的。 <發明目的> 因此,本發明之目的,即在提供一種具光子晶體的固 態發光元件。 於是’本發明具光子晶體的固態發光元件,包含:一 基板、一形成於該基板並產生一預定波段的光電半導體磊 晶臈、一連結於該光電半導體磊晶膜之電極單元,及一供 該電極單元電性導通的複合式反射鏡。該光電半導體蟲晶 膜具有一出光面、一相反於該出光面並與該基板連接的背 光面,及一形成於該出光面與背光面之間的正負接面。該 光電半導體蟲晶膜於該出光面形成有—光子晶體。該光子 j體是一二維光子晶體及一類光子晶體其中一者。該電極 單兀供.亥光電半導體磊晶臈的電子與電洞於該正負接面產 生電子電洞對復合。該複合式反射鏡具有一夾置於該光電 半導體磊晶膜與該基板之間的一維光子晶體。 本發明之功效在於,藉由一維光子晶體,與二維光子 晶體及類光子晶體其中一者的整合,適當地降低發光光譜 201006004 訊號峰的半高寬值,並提昇固態發光元件的發光亮度β 【實施方式】 有關本發明之前述及其他技術内容、特點與功效,在 以下配合參考圖式之十二個較佳實施例的詳細說明中,將 可清楚的呈現。 在本發明被詳細描述之前,要注意的是,在以下的說 明内容中’類似的元件是以相同的編號來表示。 <第一較佳實施例> 參閱圖2,本發明具光子晶體的固態發光元件之一第一 較佳實施例,包含:一基板2、一形成於該基板2並產生一 預疋波段的光電半導體蟲晶膜3、一連結於該光電半導體蟲 晶膜3的電極單元5,及一供該電極單元5電性導通的複合 式反射鏡(composite reflector)6。 在本發明之具光子晶體的固態發光元件中,該第一較 佳實施例是一經由基板分離(lift-0ff)技術與晶圓鍵合技術 (wafer bonding)所構成之垂直導通式(vertical feedthr〇ugh)的 發光二極體;因此,該基板2是一經摻雜的矽(Si)基板。相 關於基板分離技術與晶圓鍵合技術並非本發明之技術特徵 ’於此不再多加贊述。 該光電半導體磊晶膜3具有一出光面31、一相反於該 出光面31並與該基板2連接的背光面32,及一形成於該出 光面31與背光面32之間的正負接面33。 該光電半導體磊晶膜3於該出光面31形成有一光子晶 體4,該光子晶髏4是一二維光子晶體(2D pCs)及一類光子 201006004 日日(PQC)其中一者;在本發明該第一較佳實施例中該光 1晶體4是一二維光子晶體。該二維光子晶體是-呈正六 邊形細ag〇nal)排列或正四邊形(叫叫排列(如附件ι所示 )的圓形凹槽41陣列’亦可是-呈蜂巢狀排列的圓形凹槽陣 ^如附件2所示);在本發明該第—較佳實施例中該二維 :子晶體是-呈正六邊形排列的圓形凹槽Μ p車列。此處值 传提的疋,备填充率過大時,發光源的場形雖然有變窄 ❹ ❿ 的現象,但電特性效果較差;反之,當填充率過小時不 僅發光源的場型會變寬,且光特性效果也較差。因此,較 佳地,該二維光子晶體的填充率是介於0.10〜0.90之間; 更佳地胃一維光子晶體是一呈正六邊形排列的圓形凹槽 陣歹J „亥一維光子晶體的填充率是介於。仂〜〇 7〇之間 更佳地該一維光子晶趙的填充率是介於〇 %〜〇 6〇 之間;該光電半導編膜3所產生的預定波段是介於63〇 nm〜700 nm之間。 值仵S的疋,在設計二維光子晶體時所需考量的晶 格常數⑷值,主要是以光源的騎波段做為參考基礎;即 ’二維光子晶體的a值必須小於、/n,且a值與心同量級 ,、是該預定波段,η是光子晶體本身材質的折射率 (ref_Ve index)。因此,較佳地,本發明該第一較佳實施 例之二維光子晶體的晶格常數是介於5G nm〜_ nm之間 。在本發明該第-較佳實施例中,該光電半導體遙晶膜3 所產生的預定波段i 65〇 nm ;該二維光子晶趙的玨值是 200.0 rnn且填充率是〇·52;即’每一圓形凹槽41的直徑是 201006004 104.0 run,每兩相鄰圓形凹槽41之間的間距是96 〇nm。 該電極單7L 5供該光電半導體磊晶膜3的電子與電洞 於該正負接面33產生電子電洞對復合(rec〇mbinati〇n),並 具有一形成於該出光面31的第一電極51及一形成於該基 板2之一下表面的第二電極52。 該複合式反射鏡6具有一夾置於該光電半導體磊晶膜3 與該基板2之間的-維光子晶趙62、—夾置於該光電半導 體磊晶膜3與該一維光子晶鱧62之間的電流散佈層61、一 失置於該一維光子晶體62與該基板2之間的晶圓鍵合層63 φ ’及複數相間隔地設置於該—維光子晶體62並夾置於該電 流散佈層與該晶圓鍵合層63之間的導電柱64。在本發 明該第一較佳實施例中,該一維光子晶體62是由Μ對的 Ti〇2/Si〇2介電層對(dlelectric layer ^卜)所構成且加2與 si〇2的厚度分別是87 nm# 1G5 nm。本發明之複合式反射 鏡6主要是藉由該電流散佈層61、該等導電柱^及該一維 光子晶體62,以同時提供電流垂直注人卜㈣^ ίη_〇η)Use together to reduce the full width at half maximum of the spectral signal peak. The main reason is to use a one-dimensional photonic crystal with a wide angle, a narrow wavelength and no absorption problem as a mirror, and a two-dimensional photonic crystal and photonic crystal with control field characteristics. The assistance of one of them can effectively achieve the purpose of narrowing the half-height of the peak of the illuminating signal. <Objectives> Accordingly, it is an object of the present invention to provide a solid state light-emitting element having a photonic crystal. Thus, the solid-state light-emitting element having a photonic crystal of the present invention comprises: a substrate, an optoelectronic semiconductor epitaxial layer formed on the substrate and generating a predetermined wavelength band, an electrode unit coupled to the epitaxial film of the optoelectronic semiconductor, and one for The composite mirror in which the electrode unit is electrically conductive. The optoelectronic semiconductor crystal film has a light emitting surface, a back surface opposite to the light emitting surface and connected to the substrate, and a positive and negative junction formed between the light emitting surface and the backlight surface. The photo-electric semiconductor crystal film is formed with a photonic crystal on the light-emitting surface. The photon body is one of a two-dimensional photonic crystal and a type of photonic crystal. The electrode and the electrons and holes of the electron-emitting semiconductor epitaxy are combined to form an electron hole pair on the positive and negative junctions. The composite mirror has a one-dimensional photonic crystal sandwiched between the epitaxial film of the optoelectronic semiconductor and the substrate. The effect of the invention is that, by integrating one-dimensional photonic crystal with one of two-dimensional photonic crystals and photonic crystals, the half-height value of the signal peak of the luminescence spectrum 201006004 is appropriately reduced, and the luminance of the solid-state illuminating element is improved. The above and other technical contents, features and effects of the present invention will be apparent from the following detailed description of the preferred embodiments of the accompanying drawings. Before the present invention is described in detail, it is to be noted that in the following description, similar elements are denoted by the same reference numerals. <First Preferred Embodiment> Referring to Fig. 2, a first preferred embodiment of a solid-state light-emitting element having a photonic crystal of the present invention comprises: a substrate 2 formed on the substrate 2 and generating a pre-turn band The photo-electric semiconductor crystal film 3, an electrode unit 5 connected to the optoelectronic semiconductor crystal film 3, and a composite reflector 6 for electrically conducting the electrode unit 5. In the solid-state light-emitting element with photonic crystal of the present invention, the first preferred embodiment is a vertical feedthrough formed by a wafer-to-wafer technique and a wafer bonding technique (vertical feedthr). a light emitting diode; therefore, the substrate 2 is a doped germanium (Si) substrate. Regarding the substrate separation technique and the wafer bonding technique, it is not a technical feature of the present invention. The optoelectronic semiconductor epitaxial film 3 has a light emitting surface 31, a backlight surface 32 opposite to the light emitting surface 31 and connected to the substrate 2, and a positive and negative junction 33 formed between the light emitting surface 31 and the backlight surface 32. . The photo-semiconductor epitaxial film 3 is formed on the light-emitting surface 31 with a photonic crystal 4, which is one of a two-dimensional photonic crystal (2D pCs) and a photon of 201006004 (PQC); In the first preferred embodiment, the light 1 crystal 4 is a two-dimensional photonic crystal. The two-dimensional photonic crystal is a regular hexagonal arrangement or a regular square (an array of circular grooves 41 called a display arrangement (as shown by the attachment ι) can also be a circular concave arranged in a honeycomb shape. The groove array is as shown in the attachment 2; in the first preferred embodiment of the invention, the two-dimensional: sub-crystal is a circular groove Μp train arranged in a regular hexagon. Here, when the fill rate is too large, the field shape of the light source is narrower and narrower, but the electrical characteristics are less effective. Conversely, when the fill rate is too small, the field pattern of the light source will be widened. And the light characteristics are also poor. Therefore, preferably, the filling rate of the two-dimensional photonic crystal is between 0.10 and 0.90; more preferably, the one-dimensional photonic crystal of the stomach is a circular groove array arranged in a regular hexagon 歹J „海一维The filling rate of the photonic crystal is between 仂~〇7〇, and the filling rate of the one-dimensional photonic crystal is more than 〇%~〇6〇; the photoelectric semi-conductive film 3 is produced. The predetermined band is between 63〇nm and 700nm. The value of 仵S, the lattice constant (4) value to be considered when designing a two-dimensional photonic crystal, is mainly based on the riding band of the light source; 'The a value of the two-dimensional photonic crystal must be less than /n, and the value of a is the same as the magnitude of the heart, which is the predetermined wavelength band, and η is the refractive index (ref_Ve index) of the material of the photonic crystal itself. Therefore, preferably, The lattice constant of the two-dimensional photonic crystal of the first preferred embodiment is between 5 G nm and _ nm. In the first preferred embodiment of the present invention, the photo-semiconductor crystal film 3 is produced. The predetermined wavelength band i 65〇nm; the 玨 value of the two-dimensional photonic crystal Zhao is 200.0 rnn and the filling rate is 〇·52; that is, 'each round The diameter of the groove 41 is 201006004 104.0 run, and the spacing between each two adjacent circular grooves 41 is 96 〇 nm. The electrode single 7L 5 is used for the electron and the hole of the optoelectronic semiconductor epitaxial film 3 in the positive and negative connection. The surface 33 is formed by electron-hole pair recombination, and has a first electrode 51 formed on the light-emitting surface 31 and a second electrode 52 formed on a lower surface of the substrate 2. The composite reflection The mirror 6 has a -dimensional photonic crystal 62 sandwiched between the epitaxial film 3 of the optoelectronic semiconductor and the substrate 2, sandwiched between the epitaxial film 3 of the optoelectronic semiconductor and the one-dimensional photonic crystal 62 a current spreading layer 61, a wafer bonding layer 63 φ ' lost between the one-dimensional photonic crystal 62 and the substrate 2, and a plurality of spaced-apart photonic crystals 62 are interposed therebetween and interposed therebetween. The conductive pillar 64 between the layer and the wafer bonding layer 63. In the first preferred embodiment of the invention, the one-dimensional photonic crystal 62 is a pair of Ti〇2/Si〇2 dielectric layers The thickness of (dlelectric layer ^b) and the addition of 2 and si〇2 are 87 nm#1G5 nm, respectively. The composite mirror 6 of the present invention is mainly The current distribution layer 61, the conductive pillars, and the one-dimensional photonic crystal 62 are used to simultaneously provide a current vertical injection (4)^ ίη_〇η)

及光源反射的作用。 G <第二較佳實施例> 再參閱圖2’本發明具光子晶體的㈣發光元件之一第 二,佳實施例大致上是相同於該第—較佳實施例,其不同 處疋在於,該一維光子晶體62的細部條件及該光電半導體 磊晶膜3所產生的預定波段是介於48〇 nm〜55〇 nm之間。 在該本發明該第二較佳實施例中,該光電半導體蟲晶膜3 所產生的預定波段是530 nm,該一維光子晶體Μ之丁丨〇2 10 201006004 與Si02的厚度分別是67.95 nm與83.05 nm。 <第三較佳實施例> 再參閱圖2,本發明具光子晶體的固態發光元件之一第 三較佳實施例大致上是相同於該第一較佳實施例,其不同 處是在於,該一維光子晶體62的細部條件、該光電半導體 磊晶膜3所產生的預定波段,及該二維光子晶體的晶格常 數。 較佳地’該光電半導體蟲晶膜3所產生的預定波段是 介於420 nm〜480 nm之間;該二維光子晶體的晶格常數是 介於50 nm ~ 900 nm之間。 在本發明該第三較佳實施例中,該光電半導體磊晶膜3 的膜層結構是 n-GaN/(InGaN/GaN)/p-GaN,其中,n-GaN、 InGaN、GaN 及 p-GaN 的厚度分別是 230 nm、3 nm、7 nm 及230 nm,且該光電半導體磊晶膜3所產生的預定波段是 433 nm ;該二維光子晶體的晶格常數是209.1 nm ;該第一 電極51是Ti/Al/Ni/Au,該第二電極52是Ti/Pt/Au;該電 流散佈層61是厚度300 nm的氧化銦錫(ITO);該一維光子 晶體62之Ti02與Si02在430 nm處的折射率分別是2.52與 1.48,且 Ti02 與 Si02 的厚度分別是 58.96 nm 與 75.04 nm, 該一維光子晶體62是在417 nm〜450 nm之波段内形成一 全方位光帶隙(band gap)以將該第三較佳實施例所產生的光 源反射回該出光面31;該晶圓鍵合層63是Au/Ti ;每一導 電柱64是一直徑為50 μηι且高度為7 μιη的Cr/Au。 參圖3,由本發明該第三較佳實施例之掃描式電子顯微 11 201006004 鏡(SEM)影像顯示可知,該二維光子晶體的晶格常數是 209.1 nm ° <第四較佳實施例> 再參閱圖2,本發明具光子晶體的固態發光元件之一第 四較佳實施例大致上是相同於該第一較佳實施例,其不同 處是在於,該一維光子晶體62的細部條件、該光電半導體 磊晶膜3所產生的預定波段,及該二維光子晶體的適用範 圍。 較佳地,本發明該第四較佳實施例之光電半導體磊晶 © 膜3所產生的預定波段是介於380 nm ~ 420 nm之間;該二 維光子晶體的晶格常數是介於50 nm〜900 nm之間。在該 本發明該第四較佳實施例中,該光電半導體磊晶膜3所產 生的預定波段是400 nm,該一維光子晶體62之Ti02與 Si02的厚度分別是46.20 nm與63.80 nm。 本發明該第一〜四較佳實施例之光子晶體(2DPCs)4與一 維光子晶體(lDPCs)62之細部條件,是簡單地整理於下列表 表1. 圭實施例 一 二 三 四 預定波段(nm) 650 530 433 400 lDPCs Ti02 厚度(nm) 87 67.95 58.96 46.20 Si〇2 厚度(nm) 105 83.05 75.04 63.80 晶格常數(nm) 200 200 209.1 200 凹槽直徑(nm) 104 104 109.6 104 2DPCs 凹槽間距(nm) 96 96 99.5 96 填充率 0.52 0.52 0.52 0.52 凹槽深度(mn) 300 170 170 170 12 201006004 <第五較佳實施例> 參閲圖4與圖5,本發明具光子晶體的固態發光元件之 一第五較㈣施例λ致上是相同於該第^較佳實施例。其 不:處在於,該光子晶體4是-類光子晶體(PQC)。該類光 子日a體是一呈正四邊形與正三邊形交錯排列、串齒輪 (pmwheel)排列(如附件3所示)或太陽花(fib〇nacc〇排列(如 附件4所不)的正四邊形凹槽42陣列;在本發明該第五較佳 φ 冑施例中’ S亥類光子晶體是一呈正四邊形與正三邊形交錯 排列的正四邊形凹槽42 p車列。較佳地,該類光子晶體的填 充率是介於0.10〜0.90之間;該類光子晶體的晶格常數是 介於300 nm〜800 nm之間。 該正四邊形凹槽42陣列具有複數陣列單元42〇 ;且每 三彼此相鄰接的陣列單元42〇是共用三正四邊形凹槽42(如 圖5所示)。每一陣列單元42〇具有一第一陣列組421與一 第二陣列組422(如圖4所示)。每一第一陣列組421是由六 e 個呈正三邊形排列之凹槽陣列所構成以形成一呈正六邊形 排列之凹槽陣列組(圖4是未顯示出正四邊形凹槽42)。每一 第二陣列組422是由六個相間隔設置之呈正四邊形排列的 凹槽陣列與八個呈正二邊形排列的凹槽陣列所構成(圖4是 未顯示出正四邊形凹槽42)。每一陣列單元42〇的第二陣列 組422是圍繞其第一陣列組421。 更佳地,該光電半導體磊晶膜3所產生的預定波段是 介於480 nm〜550 nm之間;該類光子晶體的填充率是介於 〇·40〜0.70之間;又更佳地,該類光子晶體的填充率是介於 13 201006004 0.60 ~ 0.70之間。在本發明該第五較佳實施例中,該類光子 晶體的晶格常數、正四邊形凹槽42寬度、正四邊形凹槽42 間距與填充率分別是350 nm、220 nm、130 nm與0.63。 <第六較佳實施例> 再參閱圖5,本發具光子晶體的固態發光元件之一第六 較佳實施例大致上是相同於該第五較佳實施例。其不同處 在於,該類光子晶體的晶格常數、正四邊形凹槽42寬度、 正四邊形凹槽42間距與填充率分別是450 nm、280 nm、 170 nm 與 0·62 〇 <第七較佳實施例> 再參閱圖5,本發明具光子晶體的固態發光元件之一第 七較佳實施例大致上是相同於該第五較佳實施例。其不同 處在於,該類光子晶體的晶格常數、正四邊形凹槽42寬度 、正四邊形凹槽42間距與填充率分別是550 nm、330 nm、 220 nm 與 0·60 〇And the role of light source reflection. G <Second Preferred Embodiment> Referring again to Figure 2, a second embodiment of the (four) light-emitting element of the present invention having a photonic crystal, the preferred embodiment is substantially the same as the first preferred embodiment, and the difference is The detailed condition of the one-dimensional photonic crystal 62 and the predetermined wavelength band generated by the optoelectronic semiconductor epitaxial film 3 are between 48 〇 nm and 55 〇 nm. In the second preferred embodiment of the present invention, the predetermined wavelength band generated by the optoelectronic semiconductor crystal film 3 is 530 nm, and the thickness of the one-dimensional photonic crystal 丨〇 丨〇 2 10 201006004 and SiO 2 is 67.95 nm, respectively. With 83.05 nm. <Third Preferred Embodiment> Referring again to Fig. 2, a third preferred embodiment of the solid-state light-emitting element of the present invention having a photonic crystal is substantially the same as the first preferred embodiment, and the difference lies in The detail condition of the one-dimensional photonic crystal 62, the predetermined wavelength band generated by the optoelectronic semiconductor epitaxial film 3, and the lattice constant of the two-dimensional photonic crystal. Preferably, the predetermined wavelength band produced by the optoelectronic semiconductor crystal film 3 is between 420 nm and 480 nm; the lattice constant of the two-dimensional photonic crystal is between 50 nm and 900 nm. In the third preferred embodiment of the present invention, the film structure of the optoelectronic semiconductor epitaxial film 3 is n-GaN/(InGaN/GaN)/p-GaN, wherein n-GaN, InGaN, GaN, and p- The thickness of GaN is 230 nm, 3 nm, 7 nm and 230 nm, respectively, and the predetermined wavelength band produced by the optoelectronic semiconductor epitaxial film 3 is 433 nm; the lattice constant of the two-dimensional photonic crystal is 209.1 nm; The electrode 51 is Ti/Al/Ni/Au, the second electrode 52 is Ti/Pt/Au; the current spreading layer 61 is indium tin oxide (ITO) having a thickness of 300 nm; and the TiO2 and SiO2 of the one-dimensional photonic crystal 62 The refractive indices at 430 nm are 2.52 and 1.48, respectively, and the thicknesses of TiO2 and SiO2 are 58.96 nm and 75.04 nm, respectively. The one-dimensional photonic crystal 62 forms an omnidirectional optical band gap in the band of 417 nm to 450 nm. The light source generated by the third preferred embodiment is reflected back to the light exit surface 31; the wafer bonding layer 63 is Au/Ti; each conductive pillar 64 is a diameter of 50 μm and the height is 7 μιη Cr/Au. Referring to FIG. 3, the scanning electron microscope 11 201006004 mirror (SEM) image of the third preferred embodiment of the present invention shows that the lattice constant of the two-dimensional photonic crystal is 209.1 nm ° and the fourth preferred embodiment. Referring again to FIG. 2, a fourth preferred embodiment of the solid state light-emitting element of the present invention having a photonic crystal is substantially the same as the first preferred embodiment, except that the one-dimensional photonic crystal 62 is The detailed condition, the predetermined wavelength band generated by the optoelectronic semiconductor epitaxial film 3, and the applicable range of the two-dimensional photonic crystal. Preferably, the predetermined wavelength band generated by the optoelectronic semiconductor epitaxial film 3 of the fourth preferred embodiment of the present invention is between 380 nm and 420 nm; the lattice constant of the two-dimensional photonic crystal is between 50 Between nm and 900 nm. In the fourth preferred embodiment of the present invention, the predetermined wavelength band generated by the optoelectronic semiconductor epitaxial film 3 is 400 nm, and the thickness of the TiO2 and SiO2 of the one-dimensional photonic crystal 62 is 46.20 nm and 63.80 nm, respectively. The detailed conditions of the photonic crystals (2DPCs) 4 and the one-dimensional photonic crystals (lDPCs) 62 of the first to fourth preferred embodiments of the present invention are simply summarized in the following table. 1. Example 1 2 3 4 predetermined band (nm) 650 530 433 400 lDPCs Ti02 Thickness (nm) 87 67.95 58.96 46.20 Si〇2 Thickness (nm) 105 83.05 75.04 63.80 Lattice constant (nm) 200 200 209.1 200 Groove diameter (nm) 104 104 109.6 104 2DPCs Concave Groove pitch (nm) 96 96 99.5 96 Filling rate 0.52 0.52 0.52 0.52 Groove depth (mn) 300 170 170 170 12 201006004 <Fifth preferred embodiment> Referring to Figures 4 and 5, the present invention has a photonic crystal One of the solid state light-emitting elements is the same as the fourth preferred embodiment. It is not: the photonic crystal 4 is a photonic crystal (PQC). The photon day a is a regular quadrilateral concave with a regular quadrilateral and a regular triangular arrangement, a pmwheel arrangement (as shown in Annex 3) or a sun flower (fib〇nacc〇 arrangement (as in Annex 4). An array of slots 42; in the fifth preferred embodiment of the present invention, the 'S-type photonic crystal is a regular quadrilateral groove 42p arranged in a regular quadrilateral and a regular triangular shape. Preferably, the photon is such a photon. The filling rate of the crystal is between 0.10 and 0.90; the lattice constant of the photonic crystal is between 300 nm and 800 nm. The array of regular quadrilateral grooves 42 has a plurality of array elements 42 〇; and each of the three The adjacent array elements 42A share a common square regular groove 42 (as shown in Fig. 5.) Each array unit 42 has a first array group 421 and a second array group 422 (as shown in Fig. 4). Each of the first array groups 421 is formed by six e-shaped arrays of grooves arranged in a regular triangle to form a groove array group arranged in a regular hexagon (FIG. 4 is a square-shaped groove 42 not shown). Each second array group 422 is formed by six spaced apart positive four sides The array of aligned grooves is formed with eight arrays of grooves arranged in a regular quadrilateral (Fig. 4 shows a regular quadrilateral groove 42.) The second array set 422 of each array unit 42 is surrounded by its first Array group 421. More preferably, the predetermined wavelength band generated by the optoelectronic semiconductor epitaxial film 3 is between 480 nm and 550 nm; the filling rate of the photonic crystal is between 〇40 and 0.70; More preferably, the filling rate of the photonic crystal is between 13 201006004 0.60 and 0.70. In the fifth preferred embodiment of the present invention, the lattice constant of the photonic crystal, the width of the regular quadrangular groove 42 , The pitch and filling ratio of the regular quadrangular groove 42 are 350 nm, 220 nm, 130 nm, and 0.63, respectively. <Sixth Preferred Embodiment> Referring again to Fig. 5, the sixth solid-state light-emitting element of the present photonic crystal is sixth. The preferred embodiment is substantially the same as the fifth preferred embodiment. The difference is that the lattice constant of the photonic crystal, the width of the regular quadrangular groove 42, the pitch of the regular quadrilateral groove 42, and the filling rate are 450, respectively. Nm, 280 nm, 170 nm and 0·62 〇< seventh better EXAMPLES Referring again to Figure 5, a seventh preferred embodiment of a solid state light-emitting element having a photonic crystal of the present invention is substantially identical to the fifth preferred embodiment. The difference lies in the lattice of the photonic crystal. The constant, the width of the regular quadrangular groove 42 and the pitch and filling ratio of the regular quadrilateral groove 42 are 550 nm, 330 nm, 220 nm and 0·60 〇, respectively.

<第八較佳實施例> 再參閱圖5,本發明具光子晶體的固態發光元件之一第 八較佳實施例大致上是相同於該第五較佳實施例。其不同 處在於,該類光子晶體的晶格常數、正四邊形凹槽42寬度 、正四邊形凹槽42間距與填充率分別是750 nm、450 nm、 300 nm 與 0.60。 本發明該第五〜八較佳實施例之類光子晶體(PQC)4的細 部條件,是簡單地整理於下列表2.中。 表2. 14 201006004 類光子晶體 五 六 七 八 晶格常數(nm) 350 450 550 750 C3槽寬度(nm) 220 280 330 450 凹槽間距(nm) 130 170 220 300 填充率 0.63 0.62 0.60 0.60 <第九較佳實施例><Eighth Preferred Embodiment> Referring again to Fig. 5, an eighth preferred embodiment of the solid-state light-emitting element of the present invention having a photonic crystal is substantially the same as the fifth preferred embodiment. The difference is that the lattice constant of the photonic crystal, the width of the regular quadrilateral groove 42, the pitch and filling ratio of the regular quadrilateral groove 42 are 750 nm, 450 nm, 300 nm and 0.60, respectively. The detailed conditions of the photonic crystal (PQC) 4 of the fifth to eighth preferred embodiments of the present invention are simply arranged in the following Table 2. Table 2. 14 201006004 Photonic crystals 567 晶 lattice constant (nm) 350 450 550 750 C3 slot width (nm) 220 280 330 450 Groove spacing (nm) 130 170 220 300 Filling rate 0.63 0.62 0.60 0.60 < Ninth preferred embodiment >

再參閱圖5,本發明具光子晶體的固態發光元件之一第 九較佳實施例大致上是相同於該第五較佳實施例。其不同 處在於,該光電半導體磊晶膜3所產生的預定波段是介於 420 nm〜480 nm之間;該類光子晶體的填充率是介於0.40 〜0.70之間;又更佳地,該類光子晶體的填充率是介於0.50 ~ 0.60之間。 在本發明該第九較佳實施例中,該類光子晶體的晶格 常數、正四邊形凹槽42寬度、正四邊形凹槽42間距與填 充率分別是 350 nm、203 nm、147 nm 與 0_58 〇 <第十較佳實施例> 再參閱圖5,本發明具光子晶體的固態發光元件之一第 十較佳實施例大致上是相同於該第九較佳實施例。其不同 處在於,該類光子晶體的晶格常數、正四邊形凹槽42寬度 、正四邊形凹槽42間距與填充率分別是450 nm、264 nm、 1 86 nm 與 0.57 〇 <第十一較佳實施例> 再參閱圖5,本發明具光子晶體的固態發光元件之一第 十一較佳實施例大致上是相同於該第九較佳實施例。其不 同處在於,該類光子晶體的晶格常數、正四邊形凹槽42寬 15 201006004 度、正四邊形凹槽42間距與填充率分別是550 nm、305 nm ' 245 nm 與 0.55 〇 <第十二較佳實施例> 再參閱圖5,本發明具光子晶體的固態發光元件之一第 十二較佳實施例大致上是相同於該第九較佳實施例。其不 同處在於,該類光子晶體的晶格常數、正四邊形凹槽42寬 度、正四邊形凹槽42間距與填充率分別是750 nm、424 nm 、326 nm 與 0.57 ° 本發明該第九〜十二較佳實施例之光子晶體(PQC)4的細 β 部條件,是簡單地整理於下列表3.中。 表3 · 圭實施例 類光子晶體 九 十 十一 十二 晶格常數(nm) 350 450 550 750 凹槽寬度(nm) 203 264 305 424 凹槽間距(nm) 147 186 245 326 填充率 0.58 0.57 0.55 0.57 <分析數據>Referring again to Figure 5, a ninth preferred embodiment of a solid state light emitting device having a photonic crystal of the present invention is substantially identical to the fifth preferred embodiment. The difference is that the predetermined wavelength band generated by the optoelectronic semiconductor epitaxial film 3 is between 420 nm and 480 nm; the filling rate of the photonic crystal is between 0.40 and 0.70; more preferably, the The filling rate of a photonic crystal is between 0.50 and 0.60. In the ninth preferred embodiment of the present invention, the lattice constant of the photonic crystal, the width of the regular quadrilateral groove 42, the pitch and filling ratio of the regular quadrilateral groove 42 are 350 nm, 203 nm, 147 nm and 0_58, respectively. <Tenth Preferred Embodiment> Referring again to Fig. 5, a tenth preferred embodiment of the solid state light-emitting element of the present invention having a photonic crystal is substantially the same as the ninth preferred embodiment. The difference is that the lattice constant of the photonic crystal, the width of the regular quadrilateral groove 42, the pitch and filling ratio of the regular quadrilateral groove 42 are 450 nm, 264 nm, 1 86 nm and 0.57 〇 < DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS Referring again to Figure 5, an eleventh preferred embodiment of a solid state light emitting device having a photonic crystal of the present invention is substantially identical to the ninth preferred embodiment. The difference is that the lattice constant of the photonic crystal, the width of the regular quadrilateral groove 42 is 15 201006004 degrees, the pitch and filling ratio of the regular quadrilateral groove 42 are 550 nm, 305 nm ' 245 nm and 0.55 〇 < tenth Second Preferred Embodiment> Referring again to Figure 5, a twelfth preferred embodiment of a solid state light emitting device having a photonic crystal of the present invention is substantially identical to the ninth preferred embodiment. The difference is that the lattice constant of the photonic crystal, the width of the regular quadrangular groove 42 , the pitch and filling ratio of the regular quadrilateral groove 42 are 750 nm, 424 nm, 326 nm and 0.57 °, respectively. The fine β-conditions of the photonic crystal (PQC) 4 of the second preferred embodiment are simply arranged in the following Table 3. Table 3 · Example photonic crystals Ninety-one eleven twelve lattice constants (nm) 350 450 550 750 Groove width (nm) 203 264 305 424 Groove pitch (nm) 147 186 245 326 Filling rate 0.58 0.57 0.55 0.57 <analysis data>

參閱圖6,由本發明該第三較佳實施例之頻率對波向量 (wave vector)與頻率對光子狀態密度(density of state,簡稱 DOS)分析數據可知,圖6之左圖所顯示的三角形、圓形與 正方形曲線分別代表圖6之右圖的三個能階模態。由圖6 的左圖觀之,可看到頻率位在0.523 a/λ〜0.445 a/λ之間(即 ,波長介於399.81 nm〜469.89 nm之間)的三個能階模態, 在對應到圖6的右圖之後,三個能階模態在頻率介於0.49 a/λ 〜0.47 a/λ之間(即,426.73 nm ~ 444.89 nm 波段内)的光 16 201006004 子狀態密度增加;因此’該第三較佳實施例之二維光子晶 體4在0.523 a/λ〜0.445 a/λ的頻段内為光子提供共振腔的 作用’因而增加了其光外出效率。 另’參圖7’由本發明該第三較佳實施例的光譜圖可知 ,該第三較佳實施例之光譜訊號峰的半高寬僅約5 nm,而 未使用有二維光子晶體的發光二極體(LED)之光譜訊號的半 咼寬部尚達30 nm,顯見本發明該第三較佳實施例因使用有 ^ 該一維光子晶體62作為一高反射率的反射鏡,配合該光子 晶體(即,二維光子晶體)4改變光在半導體波導内傳播的行 為,形成一類似共振腔的光導,大幅降低光譜訊號峰的半 尚寬。本發明所提供的固態光源,具有更純的光譜訊號峰 ,在配合使用螢光粉以封裝構成白光光源的貢獻上,可大 幅地改善其亮度及良率。 參圖8,由本發明該第三較佳實施例的光輸出功率對注 入電流(injection eurrent)曲線圖可知,與未使用有二維光子 〇 日曰曰體的LED相比較下’本發明該第三較佳實施例的光輸出 f率相對增加10 %,顯見本發明該第三較佳實施例可同時 提升整體的光輪出功率。因此,更進一步提升利用本發明 之固態發光元件並配合使用f光粉所封裝成之白光光源的 亮度。 、 綜上所述,本發明具光子晶體的固態發光元件,利用 具備有較寬的角度、較窄的波長與無吸收問題等優點的一 維光子晶體作為反射鏡,同時配合具備有控制場型之特點 維光子B曰體及類光子晶體其中一者的輔助,可有效地 17 201006004 達到窄化發光訊號峰之半高寬並提昇固態發光元件的發光 亮度,確實達到本發明之目的。 惟以上所述者,僅為本發明之較佳實施例而已,當不 能以此限定本發明實施之範圍,即大凡依本發明申請專利 範圍及發明說明内容所作之簡單的等效變化與修飾皆仍 屬本發明專利涵蓋之範圍内。 【圖式簡單說明】 圖1是一正視示意圖,說明Aur01ien David等人所揭示 之具有二維光子晶體的藍光發光二極體; © 圖2是一正視示意圖,說明本發明具光子晶體的固態 發光元件之一第一較佳實施例; 圖3疋一 SEM影像圖,說明本發明之一第三較佳實施 例之二維光子晶體; 圓4是一示t圖’㈣树明之一第五較佳實施例的 一類光子晶體;Referring to FIG. 6, according to the frequency-pair wave vector and the frequency-to-photon state density (DOS) analysis data of the third preferred embodiment of the present invention, the triangle shown in the left figure of FIG. 6 is The circular and square curves represent the three energy level modes of the right image of Figure 6, respectively. From the left diagram of Figure 6, we can see the three energy modes of the frequency between 0.523 a / λ ~ 0.445 a / λ (that is, the wavelength between 399.81 nm ~ 469.89 nm), in the corresponding After the right diagram of FIG. 6, the three energy modes have a sub-state density increase in the light 16 201006004 sub-state density between 0.49 a/λ and 0.47 a/λ (ie, in the 426.73 nm to 444.89 nm band); The two-dimensional photonic crystal 4 of the third preferred embodiment provides a photonic cavity for photons in the frequency band of 0.523 a/λ~0.445 a/λ, thus increasing its light out efficiency. Further, referring to the spectrogram of the third preferred embodiment of the present invention, the full width at half maximum of the spectral signal peak of the third preferred embodiment is only about 5 nm, and no luminescence with a two-dimensional photonic crystal is used. The half-turn width of the spectral signal of the diode (LED) is up to 30 nm. It is apparent that the third preferred embodiment of the present invention uses the one-dimensional photonic crystal 62 as a mirror with high reflectivity. The photonic crystal (ie, two-dimensional photonic crystal) 4 changes the behavior of light propagating within the semiconductor waveguide to form a light guide similar to the resonant cavity, which greatly reduces the half-width of the spectral signal peak. The solid-state light source provided by the invention has a purer spectral signal peak, and the brightness and yield can be greatly improved by using the fluorescent powder to encapsulate the contribution of the white light source. Referring to FIG. 8, the optical output power versus injection current (electroscope) graph of the third preferred embodiment of the present invention can be seen as compared with an LED that does not use a two-dimensional photon 曰曰 曰曰 '. The light output f rate of the third preferred embodiment is relatively increased by 10%. It is apparent that the third preferred embodiment of the present invention can simultaneously increase the overall light wheel output power. Therefore, the brightness of the white light source packaged by the solid-state light-emitting element of the present invention and used in combination with the f-powder is further improved. In summary, the solid-state light-emitting element with photonic crystal of the present invention uses a one-dimensional photonic crystal having a wide angle, a narrow wavelength, and no absorption problem as a mirror, and is equipped with a control field type. The feature of one of the photon B-body and the photonic crystal can effectively achieve the purpose of the present invention by achieving the half-height width of the narrowed luminescence signal peak and increasing the luminance of the solid-state light-emitting element. The above is only the preferred embodiment of the present invention, and the scope of the present invention is not limited thereto, that is, the simple equivalent changes and modifications made by the scope of the invention and the description of the invention are all It is still within the scope of the invention patent. BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a front elevational view showing a blue light emitting diode having a two-dimensional photonic crystal disclosed by Aur01ien David et al.; FIG. 2 is a front elevational view showing solid state light emission of a photonic crystal of the present invention. A first preferred embodiment of the device; FIG. 3 is an SEM image showing a two-dimensional photonic crystal according to a third preferred embodiment of the present invention; and a circle 4 is a t-picture '(4) a type of photonic crystal of a preferred embodiment;

圓5疋不意圖,說明本發明之該第五較佳實施例之 類光子晶體之正四邊形凹槽陣列; 4圖6是—頻率對波向量與頻率對光子狀態密度(D帅 :數據圖’說明本發明該第三較佳實施例之光子的能階, 圖7是一光譜圖, 譜之場形;及 圖8是本發明該第 電流曲線圖。 說明本發明該第三較佳實施例的光 二較佳實施例之光輸出功率對注入 18 201006004 附件1 :呈正四邊形排列的圓形凹槽陣列之二維光子晶 體。 附件2:呈蜂巢狀排列的圓形凹槽陣列之二維光子晶體 〇 附件3 :呈串齒輪排列的正四邊形凹槽陣列之類光子晶 體。 附件4:呈太陽花排列的正四邊形凹槽陣列之類光子晶 體。Circle 5疋 is not intended to illustrate the regular quadrilateral groove array of the photonic crystal of the fifth preferred embodiment of the present invention; 4 FIG. 6 is—frequency versus wave vector and frequency versus photon state density (D handsome: data graph' The energy level of the photon of the third preferred embodiment of the present invention, FIG. 7 is a spectrum diagram, the field shape of the spectrum; and FIG. 8 is the current current graph of the present invention. The third preferred embodiment of the present invention is illustrated. Optical output power pair injection 18 of the preferred embodiment of light 2 201006004 Annex 1: Two-dimensional photonic crystal of a circular groove array arranged in a regular quadrilateral. Annex 2: Two-dimensional photonic crystal of a circular groove array arranged in a honeycomb shape 〇 Attachment 3: Photonic crystals such as a regular quadrilateral groove array arranged in a string of gears. Annex 4: Photonic crystals such as a regular quadrilateral groove array arranged in a sun flower arrangement.

19 201006004 【主要元件符號說明】 2…… …·基板 422… …·第二陣列組 3…… 光電半導體日日膜 5…… •…電極單元 31 •.… —出光面 51 ·.··· —第 電極 32"... •…背光面 52·..· •…第二電極 33·.··· •…正負接面 6…… •…複合式反射鏡 4…… •…光子晶體 61 ····. …·電流散佈層 41 ··.·. •…圓形凹槽 62·..·· -----維光子晶體 42…… ----正四邊形凹槽 63"… •…晶圓鍵合層 420… •…陣列單元 64••… •…導電柱 421… •…第一陣列組 2019 201006004 [Explanation of main component symbols] 2...... ...·Substrate 422...··Second array group 3... Photoelectric semiconductor solar film 5... •...electrode unit 31 •....——light-emitting surface 51 ····· - the first electrode 32 "... •...the backlight surface 52·..·...the second electrode 33·.···•...the positive and negative junction 6...•...the composite mirror 4...•...photonic crystal 61 ····....·current distribution layer 41 ·····.......circular groove 62·..·· -----dimensional photonic crystal 42... ----square groove 63"... •... wafer bonding layer 420... •...array unit 64••... •...conductive column 421... •...first array group 20

Claims (1)

201006004 十、申請專利範圍: 1. 一種具光子晶體的固態發光元件,包含: 一基板; 一形成於該基板並產生一預定波段的光電半導體 磊晶膜,具有一出光面、一相反於該出光面並與該基板 連接的背光面’及一形成於該出光面與背光面之間的正 負接面’該光電半導體磊晶膜於該出光面形成有一光子 晶體,該光子晶體是一二維光子晶體及一類光子晶體其 •中-者; ' 一電極單元’連結於該光電半導體磊晶膜並供該 光電半導體磊晶膜的電子與電洞於該正負接面產生電子 電洞對復合;及 一供該電極單元電性導通的複合式反射鏡,具有 一夾置於該光電半導體磊晶膜與該基板 之間的一維光子 晶體。 ❹2.依據申請專利範圍第】項所述之具光子 項所述之具光子晶體的固態發光201006004 X. Patent application scope: 1. A solid-state light-emitting element with a photonic crystal, comprising: a substrate; an optoelectronic semiconductor epitaxial film formed on the substrate and generating a predetermined wavelength band, having a light-emitting surface, opposite to the light-emitting surface a backlight surface connected to the substrate and a positive and negative junction formed between the light-emitting surface and the backlight surface. The photoelectric semiconductor epitaxial film forms a photonic crystal on the light-emitting surface, and the photonic crystal is a two-dimensional photon. a crystal and a type of photonic crystal, wherein the 'one electrode unit' is coupled to the optoelectronic semiconductor epitaxial film and the electrons and holes of the optoelectronic semiconductor epitaxial film are combined at the positive and negative junctions to form an electron hole pair; A composite mirror for electrically conducting the electrode unit has a one-dimensional photonic crystal sandwiched between the epitaxial film of the optoelectronic semiconductor and the substrate. ❹ 2. Solid-state luminescence with photonic crystals as described in the photon clause according to the scope of the patent application 凹槽陣列,該二绅 之間。 項所述之具光子晶體的固態發光元 據申請專利範圍第 21 201006004 件’其中’該光電半導體蟲晶膜所產生的預定波段是介 於630 nm〜700 nm之間;該二維光子晶體的晶格常數 是介於50 nm ~ 900 nm 之間。 5. 依據申請專利範圍第3項所述之具光子晶體的固態發光 元件,其中’該光電半導體磊晶膜所產生的預定波段是 介於480 nm〜HO nm之間;該二維光子晶體的晶格常 數是介於50 nm ~ 900 nm之間。 6. 依據申請專利範圍第3項所述之具光子晶體的固態發光 元件,其中,該光電半導體磊晶膜所產生的預定波段是 壽 介於420 nm〜480 nm之間;該二維光子晶體的晶格常 數是介於50 nm〜900 nm之間。 7·依據申請專利範圍第3項所述之具光子晶體的固態發光 元件,其中,該光電半導體磊晶膜所產生的預定波段是 介於380 nm〜420 nm之間;該二維光子晶體的晶格常 數是介於 5 0 nm 〜900 nm 之間 ° 8_依據申請專利範圍第1項所述之具光子晶體的固態發光 元件’其中’該光子晶體是一類光子晶體,該類光子晶 ❹ 體是一呈正四邊形與正三邊形交錯排列、串齒輪排列或 太陽花排列的正四邊形凹槽陣列;該類光子晶體的填充 率是介於0.10 ~ 0.90之間;該類光子晶體的晶格常數是 介於300 nm〜800 nm之間。 9·依據申請專利範圍第8項所述之具光子晶體的固態發光 元件,其中,該類光子晶艘是一呈正四邊形與正三邊形 交錯排列的正四邊形凹槽陣列,該正四邊形凹槽陣列具 22 201006004 有複數陣列單元,每三彼此相鄰接的陣列單元是共用三 正四邊形凹槽,且每一陣列單元具有一第一陣列=與一 第二陣列組,每一第一陣列組是由六個呈正三邊形排列 之凹槽陣列所構成以形成一呈正六邊形排列之凹槽陣列 組,每一第二陣列組是由六個相間隔設置之呈正四邊形 排列的凹槽陣列與六個呈正三邊形排列的凹槽陣列所構 成,每一陣列單元的第二陣列組是圍繞其第一陣列組。 ❿10.依據中請專利範圍第9項所述之具光子晶體的固態發光 元件,其中,該光電半導體磊晶膜所產生的預定波段是 介於480 nm〜550 nm之間;該類光子晶體的填充率是 介於0.40〜〇·7〇之間。 11.依據申請專利範圍第9項所述之具光子晶體的固態發光 元件,其中,該光電半導體磊晶膜所產生的預定波段是 介於420 nm〜480 nm之間;該類光子晶體的填充率是 介於0.40 ~ 0.70之間。 Φ 12.依據申請專利範圍第1〜11項任一項所述之具光子晶體 的固態發光元件,其中,該電極單元具有一形成於該出 光面的第一電極及一形成於該基板之一下表面的第二電 極。 13.依據申請專利範圍第丨〜^項任一項所述之具光子晶體 的固態發光元件,其中,該複合式反射鏡具有一夾置於 該光電半導體磊晶膜與該一維光子晶體之間的電流散佈 層、一夾置於該一維光子晶體與該基板之間的晶圓鍵合 層’及複數相間隔地設置於該一維光子晶體並夾置於該 23 201006004 電流散佈層與該晶圓鍵合層之間的導電柱。An array of grooves, between the two turns. The solid-state light-emitting element with a photonic crystal according to the above-mentioned patent application No. 21 201006004, wherein the predetermined wavelength band produced by the photoelectric semiconductor film is between 630 nm and 700 nm; the two-dimensional photonic crystal The lattice constant is between 50 nm and 900 nm. 5. The solid-state light-emitting element with a photonic crystal according to claim 3, wherein the predetermined wavelength band produced by the epitaxial film of the optoelectronic semiconductor is between 480 nm and HO nm; the two-dimensional photonic crystal The lattice constant is between 50 nm and 900 nm. 6. The solid-state light-emitting element with a photonic crystal according to claim 3, wherein the predetermined wavelength band produced by the optoelectronic semiconductor epitaxial film is between 420 nm and 480 nm; the two-dimensional photonic crystal The lattice constant is between 50 nm and 900 nm. The solid-state light-emitting element with a photonic crystal according to claim 3, wherein the predetermined wavelength band produced by the optoelectronic semiconductor epitaxial film is between 380 nm and 420 nm; the two-dimensional photonic crystal The lattice constant is between 50 nm and 900 nm. 8_ The solid-state light-emitting element having a photonic crystal according to the scope of claim 1 'where the photonic crystal is a type of photonic crystal, the photonic crystal The body is a regular quadrilateral groove array with a regular quadrilateral and a regular triangular staggered arrangement, a string gear arrangement or a sun flower arrangement; the filling rate of the photonic crystal is between 0.10 and 0.90; the lattice constant of the photonic crystal It is between 300 nm and 800 nm. 9. The solid-state light-emitting element with a photonic crystal according to claim 8, wherein the photonic crystallizer is an array of regular quadrangular grooves arranged in a regular quadrilateral and a regular triangular shape, the regular quadrilateral groove array With 22 201006004 having a plurality of array elements, each of the three adjacent array units is a common three-square quadrangular groove, and each array unit has a first array = and a second array group, each of the first array groups is Formed by six arrays of grooves arranged in a regular triangle to form a groove array group arranged in a regular hexagon shape, each second array group is composed of six groove arrays arranged in a regular quadrangle Six arrays of grooves arranged in a regular triangle shape, the second array group of each array unit being around its first array group. The solid-state light-emitting element with a photonic crystal according to claim 9, wherein the predetermined wavelength band produced by the optoelectronic semiconductor epitaxial film is between 480 nm and 550 nm; The fill rate is between 0.40 and 〇·7〇. The solid-state light-emitting element with a photonic crystal according to claim 9, wherein the predetermined wavelength band produced by the optoelectronic semiconductor epitaxial film is between 420 nm and 480 nm; filling of the photonic crystal The rate is between 0.40 and 0.70. The solid-state light-emitting element having a photonic crystal according to any one of claims 1 to 11, wherein the electrode unit has a first electrode formed on the light-emitting surface and one formed under the substrate The second electrode of the surface. The solid-state light-emitting element with a photonic crystal according to any one of the preceding claims, wherein the composite mirror has a sandwiched between the epitaxial film of the optoelectronic semiconductor and the one-dimensional photonic crystal. a current spreading layer, a wafer bonding layer sandwiched between the one-dimensional photonic crystal and the substrate, and a plurality of spaced-apart photonic crystals are interposed between the two-dimensional photonic crystal and sandwiched between the current and current layers A conductive pillar between the wafer bonding layers. 24twenty four
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Publication number Priority date Publication date Assignee Title
US8755645B2 (en) 2011-03-28 2014-06-17 Industrial Technology Research Institute Circular photonic crystal structure, light emitting diode device and photoelectric conversion device

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US8755645B2 (en) 2011-03-28 2014-06-17 Industrial Technology Research Institute Circular photonic crystal structure, light emitting diode device and photoelectric conversion device

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