TW540164B - Radiation-emitting semiconductor-body and its production method - Google Patents

Radiation-emitting semiconductor-body and its production method Download PDF

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TW540164B
TW540164B TW090127499A TW90127499A TW540164B TW 540164 B TW540164 B TW 540164B TW 090127499 A TW090127499 A TW 090127499A TW 90127499 A TW90127499 A TW 90127499A TW 540164 B TW540164 B TW 540164B
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radiation
layer
algaas
semiconductor body
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Stephan Lutgen
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Osram Opto Semiconductors Gmbh
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L33/00Semiconductor 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
    • H01L33/02Semiconductor 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 bodies
    • H01L33/26Materials of the light emitting region
    • H01L33/30Materials of the light emitting region containing only elements of Group III and Group V of the Periodic Table
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L33/00Semiconductor 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
    • H01L33/02Semiconductor 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 bodies
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L33/00Semiconductor 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
    • H01L33/005Processes
    • H01L33/0062Processes for devices with an active region comprising only III-V compounds
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L33/00Semiconductor 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
    • H01L33/005Processes
    • H01L33/0093Wafer bonding; Removal of the growth substrate
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S2301/00Functional characteristics
    • H01S2301/17Semiconductor lasers comprising special layers
    • H01S2301/173The laser chip comprising special buffer layers, e.g. dislocation prevention or reduction
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S5/00Semiconductor lasers
    • H01S5/10Construction or shape of the optical resonator, e.g. extended or external cavity, coupled cavities, bent-guide, varying width, thickness or composition of the active region
    • H01S5/16Window-type lasers, i.e. with a region of non-absorbing material between the active region and the reflecting surface
    • H01S5/164Window-type lasers, i.e. with a region of non-absorbing material between the active region and the reflecting surface with window regions comprising semiconductor material with a wider bandgap than the active layer
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S5/00Semiconductor lasers
    • H01S5/10Construction or shape of the optical resonator, e.g. extended or external cavity, coupled cavities, bent-guide, varying width, thickness or composition of the active region
    • H01S5/18Surface-emitting [SE] lasers, e.g. having both horizontal and vertical cavities
    • H01S5/183Surface-emitting [SE] lasers, e.g. having both horizontal and vertical cavities having only vertical cavities, e.g. vertical cavity surface-emitting lasers [VCSEL]

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  • Engineering & Computer Science (AREA)
  • Manufacturing & Machinery (AREA)
  • Computer Hardware Design (AREA)
  • Microelectronics & Electronic Packaging (AREA)
  • Power Engineering (AREA)
  • Led Devices (AREA)

Abstract

The radiation-generating layer-sequence (2) is grown directly on a window-layer (3), which has one or several overlapped AlGaAs-layers (4, 5, 6). The AlGaAs-layers are produced by means of liquid-phase-epitaxy or a similar method and have respectively an Al-content far from the layer-sequence (2), in which AlGaAs is transparent for the generated radiation. The Al-content decreases in each AlGaAs-layers (4, 5, 6) in the direction to the active layer-sequence (2). The Window-layer (3) is alternatively composed of a non-supporting AlGaAs-epitaxy substrate (7), which has Al-content, in which AlGaAs is transparent for the generated radiation.

Description

540164 五、發明説明(5 ) 體,活性層序列2之總厚度通常只有數個μπι。540164 V. Description of the invention (5) The total thickness of the active layer sequence 2 is usually only a few μm.

AlGaAs層4,5,6較佳是藉由液相磊晶法(LPE)而製成 且厚度可達50μιη。在生長方向中液相磊晶法中所產生之 鋁空乏(depletion)可藉由本發明之AlGaAs多層結構而成 爲”無害處(undamaged)’’。以本發明具有二個或多個 AlGaAs層之AlGaAs多層結構爲基礎,則可藉由多次LPE 生長(或拉升(boot))過程而製成層厚度較大之無支撐式透 明之AlGaAs-LPE層。具有足夠之機械穩定性之總厚度介 於100和200μηι之間之層可以上述方式很簡單地製成。沈 積時之溫度是在7〇〇-l〇〇〇°C。 緦之,AlGaAs多層結構4,5,6中之A1含量未超過一 較大之層厚度(> 1 〇〇nm)時對活性層中所產生之光而言須下 降至小於該透明範圍之下,所發出之光在AlGaAs層中因 此不會被大量地(>3%)吸收。但鋁含量小於透明範圍之這 些薄層(10-30 Onm)(例如,請比較第lb圖中以圓圈所示之 由AlGaAs多層結構至活性層序列2之接面區10)特別是 可作爲鋁含量很高之AlGaAs層用之覆蓋層,因此可使含 鋁之層在空氣中不會被氧化,否則氧化後之層對該活性層 序列2之隨後之各磊晶層而言是一種不期望之電性隔離用 之截止層。 在第2a至2e圖所示之製造第la,lb圖之可發出輻射 之半導體主體所用之方法中,首先在磊晶基板7(其例如由 GaAs或其它適當之材料所構成)上藉由液相磊晶法依序生 長二個AlGaAs層4,5,6。這些步驟是在第一'製程溫度( 540164 五、發明説明(7 ) (Freez)法(VGF)來製成。 爲了獲得電性接觸區相面對之此種晶片結構,則磊晶基 板Π須摻雜成具有導電性。 本發明之半導體層序列同樣特別適合用來製成半導體主 體,其中經由視窗層3親合而出或親合而入之輻射之波長 是在紅外線區域中或紅色光譜區中且小於8 70nm。視窗層 3之吸收邊緣調整至一種較耦合而出或耦合而入之輻射還 短之波長處。 本發明之層序列可有利地用於垂直式表面發射之半導體 雷射結構中或用於發光二極體結構中。 本發明之半導體主體之半導體層依據組件結構而由下述 方式所形成: -在發光之二極體(LEDs)中由各導電層(可能另有一些佈 拉格(Bragg)反射層)所形成,其對該活性層中所產生之 光而言是透明的。活性層通常由一個或多個量子膜所構 成。一種配置在活性層上之層序列另外可由導電層所構 成以便與電性接觸區形成歐姆連接。由AlGaAs-多層結 構及AlGaAs-嘉晶基板之穿透性,則低能量光束之一部 份可由活性層經由AlGaAs-視窗層之背面或藉由可反射 之背面接觸區而反射至AlGaAs-視窗層之背面且一部份 向外耦合至側面及/或向前耦合而出。因此,藉助於透 明之AlGaAs-多層結構或透明之AlGaAs-磊晶基板亦可 形成向後發射用之LED結構。活性LED結構之磊晶過 程直接在視窗層上進行,即,在AlGaAs多層結構上或 -9- 540164 五、發明説明(8 )The AlGaAs layers 4, 5, 6 are preferably made by liquid phase epitaxy (LPE) and have a thickness of up to 50 µm. The aluminum depletion generated in the liquid phase epitaxy in the growth direction can be "undamaged" by the AlGaAs multilayer structure of the present invention. According to the present invention, AlGaAs having two or more AlGaAs layers Based on a multi-layer structure, an unsupported and transparent AlGaAs-LPE layer with a large layer thickness can be made through multiple LPE growth (or boot) processes. The total thickness of the layer has sufficient mechanical stability. Layers between 100 and 200 μηι can be made very simply as described above. The temperature at the time of deposition is 700-1000 ° C. In other words, the Al content in AlGaAs multilayer structure 4, 5, 6 is not Beyond a larger layer thickness (> 1000 nm), the light generated in the active layer must fall below the transparent range, and the light emitted in the AlGaAs layer will not be greatly affected. (≫ 3%) absorption. However, these thin layers (10-30 Onm) whose aluminum content is less than the transparent range (for example, compare the interface from the AlGaAs multilayer structure to the active layer sequence 2 shown by the circle in Figure lb) Zone 10) is particularly useful as a cover layer for AlGaAs layers with a high aluminum content, This prevents the aluminum-containing layer from being oxidized in the air, otherwise the oxidized layer is an undesired stop layer for electrical isolation for the subsequent epitaxial layers of the active layer sequence 2. In the method for manufacturing the radiation-emitting semiconductor body shown in Figs. 2a to 2e, the epitaxial substrate 7 (which is made of, for example, GaAs or other suitable materials) is firstly subjected to liquid phase epitaxy on the method The two AlGaAs layers 4, 5, and 6 are sequentially grown by the crystal method. These steps are made at the first process temperature (540,164, 5. Description of the invention (7) (Freez) method (VGF). In order to obtain the electrical contact area For such a wafer structure facing each other, the epitaxial substrate Π must be doped to have conductivity. The semiconductor layer sequence of the present invention is also particularly suitable for making a semiconductor body, in which the window layer 3 is affinity-bonded or affinity-bonded. The wavelength of the incoming radiation is in the infrared region or the red spectral region and is less than 8 70 nm. The absorption edge of the window layer 3 is adjusted to a wavelength shorter than the radiation that is coupled out or coupled in. The layer of the invention Sequences can be advantageously used for vertical tables The emitting semiconductor laser structure or used in the light-emitting diode structure. The semiconductor layer of the semiconductor body of the present invention is formed in the following manner depending on the component structure:-Each light-emitting diode (LEDs) is electrically conductive Layer (possibly some other Bragg reflective layers), which is transparent to the light generated in the active layer. The active layer is usually composed of one or more quantum films. A configuration is The layer sequence on the active layer may also be composed of a conductive layer to form an ohmic connection with the electrical contact area. Due to the permeability of the AlGaAs-multilayer structure and the AlGaAs-Jiajing substrate, part of the low-energy beam can be passed by the active layer The back side of the AlGaAs-window layer is reflected to the back side of the AlGaAs-window layer through a reflective back contact area and a part is coupled out to the side and / or forwardly. Therefore, a transparent AlGaAs-multilayer structure or a transparent AlGaAs-epitaxial substrate can also be used to form an LED structure for backward emission. The epitaxial process of the active LED structure is performed directly on the window layer, that is, on the AlGaAs multilayer structure or -9-540164. V. Description of the invention (8)

AlGaAs磊晶基板上進行,此時事後不必藉由技術上昂 貴之晶圓連結或熔合而形成部份導電性之透明之基板載 體接觸區。 -在由導電層構成之共振發光二極體(RCLEDs)中,其具 有週期數較少(典型上是5個週期,因此未使用雷射功 倉g)之回授式佈拉格(Bragg)反射層,其對活性層中所產 生之光而言是透明的。 活性層通常由一個或多個量子膜所構成。總厚度是發 射波長之一半之整數倍。量子膜之位置是在駐波場 (field)之腹部位置中。 隨後所配置之層序列由相位已調整之佈拉格-反射層 所構成。這些層另外可由稍後之歐姆金屬接觸用之導電 層所構成。 由於AlGaAs多層結構或AlGaAs磊晶基板之透明性 ,則低能量光束之一部份可由活性層經由AlGaAs-視窗 層之背面或藉由可反射之背面接觸區而反射至AlGaAs-視窗層之背面且一部份向外耦合至側面及/或向前耦合而 出。因此,藉助於透明之AlGaAs-多層結構或透明之 AlGaAs-磊晶基板亦可形成向後發射用之LED結構。活 性RCLED結構之嘉晶過程直接在AlGaAs-多層結構上 或AlGaAs-磊晶基板上進行,此時事後不必藉由技術上 昂貴之晶圓連結或熔合而形成部份導電性之透明之基板 載體接觸區。 -在經由基板向後耦合而出之垂直式表面發射用雷射結構 -10- 540164 五、發明説明(9) (VCSEL)中,其由導電層所構成且具有週期數較多(典型 上是22個週期)之回授式佈拉格反射層,因此可在品質 較高之共振器中在大於臨限(threshold)電流時使用吸收 性較小之雷射功能。 活性層通常由一個或多個量子膜所構成。總厚度是發 射波長之一半之整數倍。量子膜之位置是在駐波場 (field)之腹部位置中。 隨後所配置之層序列由相位已調整之佈拉格-反射層( 典型上是27週期)所構成,其作爲活性層中所產生之光 束用之較高品質之反射器(R大約是0.99)。這些層另外 可由稍後之歐姆金屬接觸用之導電層所構成。 由於AlGaAs -多層結構或AlGaAs -嘉晶基板之透明性 ,則低能量之雷射束之此部份(其由於已回授之佈拉格 反射層之較小之反射性而離開雷射共振器)未被吸收即 經由AlGaAs-背面層耦合而出。藉助於透明之AlGaAs-多層結構或AlGaAs-磊晶基板,則可製成可向後發射之 VCSEL結構。活性VCSEL結構之磊晶過程直接在視窗 層上進行’即,在AlGaAs多層結構上或AlGaAs嘉晶 基板上進行,此時事後不必藉由技術上昂貴之晶圓連結 或熔合而形成部份導電性之透明之基板載體接觸區。 符號之說明 1 半導體主體 2 層序列 3 視窗層 4,5,6 AlGaAs 層 -11- 540164 10 磊晶基板 接觸層 五、發明説明() 7,11 8,9 -12-AlGaAs epitaxial substrate is carried out. At this time, it is not necessary to form a partially conductive transparent substrate carrier contact area by connecting or fusing technically expensive wafers afterwards. -In resonant light emitting diodes (RCLEDs) composed of conductive layers, they have feedback Braggs with a small number of cycles (typically 5 cycles, so laser power g is not used) The reflective layer is transparent to the light generated in the active layer. The active layer is usually composed of one or more quantum films. The total thickness is an integral multiple of one-half the emission wavelength. The position of the quantum film is in the abdomen position of the standing wave field. The layer sequence subsequently configured consists of a Bragg-reflective layer whose phase has been adjusted. These layers may additionally consist of a conductive layer for later ohmic metal contact. Due to the transparency of the AlGaAs multilayer structure or the AlGaAs epitaxial substrate, part of the low-energy beam can be reflected by the active layer through the backside of the AlGaAs-window layer or through the reflective backside contact area to the backside of the AlGaAs-window layer and A portion is coupled out to the side and / or forward. Therefore, the LED structure for backward emission can also be formed by means of a transparent AlGaAs-multilayer structure or a transparent AlGaAs-epitaxial substrate. The Jiajing process of the active RCLED structure is performed directly on the AlGaAs-multilayer structure or AlGaAs-epitaxial substrate. At this time, it is not necessary to form a partially conductive transparent substrate carrier contact afterwards by technically expensive wafer bonding or fusion. Area. -In the vertical surface-emitting laser structure coupled back through the substrate-10-540164 V. Description of Invention (9) (VCSEL), which is composed of a conductive layer and has a large number of cycles (typically 22) Cycle) of the feedback Bragg reflector, so the higher-quality resonator can use the laser function with less absorption when the current is greater than the threshold. The active layer is usually composed of one or more quantum films. The total thickness is an integral multiple of one-half the emission wavelength. The position of the quantum film is in the abdomen position of the standing wave field. The layer sequence subsequently configured consists of a phase-adjusted Bragg-reflective layer (typically 27 cycles), which serves as a higher-quality reflector for the beam generated in the active layer (R is approximately 0.99) . These layers may additionally consist of a conductive layer for later ohmic metal contact. Due to the transparency of the AlGaAs-multilayer structure or AlGaAs-Jiajing substrate, this part of the low-energy laser beam (which leaves the laser resonator due to the smaller reflectivity of the feedback Bragg reflective layer) ) Without absorption, it is coupled out through the AlGaAs-back layer. With the aid of a transparent AlGaAs-multilayer structure or an AlGaAs-epitaxial substrate, a VCSEL structure that can be emitted backward can be made. The epitaxial process of the active VCSEL structure is performed directly on the window layer, that is, on the AlGaAs multilayer structure or on the AlGaAs Jiajing substrate. At this time, there is no need to form a part of the conductivity by technically expensive wafer bonding or fusion. The transparent substrate carrier contact area. Explanation of symbols 1 Semiconductor body 2 Layer sequence 3 Window layer 4,5,6 AlGaAs layer -11- 540164 10 Epitaxial substrate Contact layer V. Description of the invention () 7,11 8,9 -12-

Claims (1)

540164 q碎Lf月H補土六、申請專利範圍 第90 1 27499號「可發出輻射之半導體主體及其製造方法 」專利案 (92年4月修正) 六、申請專利範圍: 1. 一種可發出輻射之半導體主體(1),其包含:一可發 出輻射之層序列(2 )及一種對所產生之輻射而言至少 是一部份可透過之視窗層(3 ),其特徵爲: 視窗層具有一個或多個依序配置之 AlGaAs層 (4,5,6 ),其藉由液相磊晶法或相同形式之方法而製 成且在遠離層序列(2)之處分別具有一種A1含量, 此種A1含量使AlGaAs對所產生之光束而言是可透 過的且此種A1含量在每一 AlGaAs層(4, 5,6)中在輻 射產生用之層序列(2 )中逐漸減少。 2. 如申請專利範圍第1項之可發出輻射之半導體主體 (1),其中鄰接於層序列(2)之AlGaAs層(6)在至層 序列(2 )之接面區中具有一種鈍化層。 3. 如申請專利範圍第1項之可發出輻射之半導體主體 (1 ),其中鄰接於層序列(2)之AlGaAs層(6)在至層 序列(2)之接面區中具有一種鋁含量,其中AlGaAs 在含氧之大氣中未被氧化或只稍微氧化,因此該 AlGaAs層可用作鈍化層。 4. 如申請專利範圍第3項之可發出輻射之半導體主體(1 ) ,其中該接面區之層厚度介於10nm和3 0nm之間。 ^164 六 申凊專利範圍540164 q broken Lf month H supplementary soil 6. Patent application range 90 1 27499 "Semiconductor body capable of emitting radiation and its manufacturing method" patent case (amended in April 1992) 6. Scope of patent application: 1. A type that can be issued Radiation semiconductor body (1), comprising: a layer sequence (2) that can emit radiation and a window layer (3) that is at least partially transparent to the generated radiation, and is characterized by: AlGaAs layers (4,5,6) with one or more sequentially arranged, which are made by liquid phase epitaxy or the same method, and each have an A1 content at a distance from the layer sequence (2) This Al content makes AlGaAs transparent to the generated light beam and this Al content decreases gradually in each AlGaAs layer (4, 5, 6) in the layer sequence (2) for radiation generation. 2. For example, the radiation-emitting semiconductor body (1) in the scope of patent application, wherein the AlGaAs layer (6) adjacent to the layer sequence (2) has a passivation layer in the junction area to the layer sequence (2) . 3. The radiation-emitting semiconductor body (1), such as in the scope of patent application, wherein the AlGaAs layer (6) adjacent to the layer sequence (2) has an aluminum content in the junction area to the layer sequence (2) The AlGaAs layer is not oxidized or only slightly oxidized in an atmosphere containing oxygen, so the AlGaAs layer can be used as a passivation layer. 4. The radiation-emitting semiconductor body (1), such as the scope of application for patent No. 3, wherein the layer thickness of the junction area is between 10nm and 30nm. ^ 164 Six patent application scope 5·如申請專利範圍第1至4項中任一項之可發出輻射 之半導體主體(1),其中一經由視窗層(3)耦合而出 或耦合而入之輻射之波長小於870nm且視窗層(3)之 吸收邊緣藉由可改變之鋁含量而整體上處於較短之 波長中。 6·如申請專利範圍第1項之可發出輻射之半導體主體 (1),其中AlGaAs層(4,5,6)摻雜成具有導電性。 7·如申請專利範圍第1項之可發出輻射之半導體主體 ㈠),其中視窗層(3)之厚度大於5μπι。 δ· 申請專利範圍第7項之可發出輻射之半導體主體 (1 ),其中視窗層(3 )具有一種無支撐之基板,其厚 度介於ΙΟΟμπι和ΙΟΟΟμπι之間。 9·如申請專利範圍第1項之可發出輻射之半導體主體 (1 ),其中視窗層(3 )藉由液相磊晶或類似方法生長 而成,層序列(2 )藉由氣相磊晶,特別是藉由金屬有 機之氣相磊晶或分子束磊晶或類似之磊晶方式,生 長而成。 10.—種可發出輻射之半導體主體(1),其包含:一可發 出輻射之層序列(2 )及一種對所產生之輻射而言至少 是一部份可透過之視窗層(3 ),其特徵爲: 視窗層(3 )由無支撐之磊晶基板(1 1 )所形成,其由 AlGaAs所構成且具有一種鋁(Α1 )含量,此種鋁含量 使AlGaAs對所產生之輻射而言是可透過的。 540164 _______I 你丨》上―i U^—麵 六、申請專利範圍 ; 11·如申請專利範圍第1 0項之可發出輻射之半導體主體 (1 ),其中一經由視窗層(3 )耦合而出或耦合而入之 輻射之波長小於870nm且視窗層(3)之吸收邊緣處於 一種較短之波長中。 12如申請專利範圍第1 0或1 1項之可發出輻射之半導 體主體(1 ),其中該磊晶基板藉由 Vert i cal Gradient Freeze方法而製成。 Π如申請專利範圍第1或1 0項之可發出輻射之半導體 主體(1 ),其中視窗層(3 )摻雜成具有導電性。 14. 如申請專利範圍第1或1 0項之可發出輻射之半導體 主體(1),其中層序列(2)具有一垂直式表面發射用 之半導體雷射結構。 15. 如申請專利範圍第1或1 0項之可發出輻射之半導體 主體(1 ),其中此層序列(2 )具有發光二極體結構。 16. —種可發出輻射之半導體主體(1 )之製造方法,此半 導體主體(1 )是申請專利範圍第1至9項中任一項或 第1 3至1 5項中任一項(其依附於第1至9項中任一 項)所述者,其特徵爲以下各步驟: a )製備一種裔晶基板(7 ); b )在第一製程溫度中藉由液相磊晶而在磊晶基板(7 ) 上生長 AlGaAs 層(4,5,6); c )在第二製程溫度中藉由金屬有機之氣相磊晶或分 子束磊晶而在AlGaAs層(4, 5,6)上生長該層序列 540164 屮年9月,构修正 六、申請專利範圍 (2)0 17. 如申請專利範圍第1 6項之製造方法,其中第一製程 溫度介於7 0 0 °C和1 0 0 0 °C之間,第二製程溫度介於 400°C 及 800°C 之間。 18. 如申請專利範圍第1 6或1 7項之製造方法,其中在 步驟c )之後使嘉晶基板(7 )被去除。 ia —種可發出輻射之半導體主體(1)之製造方法,此半 導體主體(1)是申請專利範圍第10,11或12項或第 1 3,1 4或1 5項(其依附於第1 0,1 1或1 2項)所述 者,其特徵爲以下各步驟: a) 製備一種無支撐之磊晶基板(11),其由AlGaAs多 層結構所構成且具有一種A1含量,此種a 1含量 使AlGaAs對所產生之輻射而言是可透過的, b) 在第二製程溫度中藉由金屬有機之氣相磊晶或分 子中磊晶而在磊晶基板上生長該層序列(2 )。 2〇·如申請專利範圍第1 9項之製造方法,其中磊晶基板 藉由垂直梯度冷凍法(Vertical Gradient Freeze (VGF))方法而製成。 21· —種基板(3 )之製造方法,其用來生長一可發出輻射 之半導體主體,其特徵爲以下各步驟: a )製備一種磊晶基板(7 ); b)藉由液相嘉晶在嘉晶板(7)上生長一*種AlGaAs層 (4,5,6),其中磊晶層中之A1含量隨著生長厚度 540164 六、申請專利範圍 涿漸增加而減少且須選取AlGaAs層之厚度,使其 中之A1含量對該可發出輻射之結構中所產生之輻 射而言不小於-或只在厚度到達30nm時才小於穿 透極限値; c)重複步驟b)直至基板(由AlGaAs層(4,5,6)所構 成)達到所期望之厚度爲止。 22. —種可發出輻射之半導體主體生長所用之基板(3 ), 其特徵爲: 其具有一個或多個依序配置之AlGaAs層(4,5, 6) ,這些層藉由液相磊晶法或類似之方法所製成且其 平均具有一種A1含量,此種A1含量使AlGaAs對一 種在可發出輻射之半導體主體中所產生之輻射而言 是可透過的,且在每一 AlGaAs層中由面向基板(3) 之第一主面之此側開始在至一種面向此基板(3 )之 第二主面(其與第一主面相面對)之此側之方向中此 AlGaAs具有下降之A1含量,其中之A1含量對所 產生之輻射而言不小於或只有厚度到達30nm時才 小於穿透極限値。5. The radiation-emitting semiconductor body (1) according to any of claims 1 to 4 of the scope of patent application, wherein the wavelength of a radiation which is coupled out through or coupled through the window layer (3) is less than 870 nm and the window layer (3) The absorption edge is in a shorter wavelength as a whole by changing the aluminum content. 6. The radiation-emitting semiconductor body (1) according to item 1 of the patent application scope, wherein the AlGaAs layer (4, 5, 6) is doped to have conductivity. 7. If the radiation-emitting semiconductor body ㈠) of item 1 of the patent application scope, wherein the thickness of the window layer (3) is greater than 5 μm. δ. The radiation-emitting semiconductor body (1) in the scope of patent application No. 7 in which the window layer (3) has an unsupported substrate having a thickness between 100 μm and 100 μm. 9. The radiation-emitting semiconductor body (1), as described in the first patent application, wherein the window layer (3) is grown by liquid phase epitaxy or a similar method, and the layer sequence (2) is by gas phase epitaxy , Especially by metal organic vapor phase epitaxy or molecular beam epitaxy or similar epitaxial growth. 10. A radiation-emitting semiconductor body (1), comprising: a sequence of radiation-emitting layers (2) and a window layer (3) that is at least partially transparent to the radiation produced, It is characterized by: The window layer (3) is formed by an unsupported epitaxial substrate (1 1), which is composed of AlGaAs and has an aluminum (A1) content. This aluminum content makes AlGaAs to the radiation generated Is permeable. 540164 _______I You》 "i U ^ —Sixth, the scope of patent application; 11. If the patent application scope of the tenth of the semiconductor body (1) that can emit radiation, one of them is coupled out through the window layer (3) Or the coupled radiation has a wavelength of less than 870 nm and the absorption edge of the window layer (3) is in a shorter wavelength. 12 The radiation-emitting semiconductor body (1) according to claim 10 or 11, wherein the epitaxial substrate is made by the Vert i cal Gradient Freeze method. Π The radiation-emitting semiconductor body (1), such as the scope of patent application No. 1 or 10, wherein the window layer (3) is doped to have conductivity. 14. The radiation-emitting semiconductor body (1), such as in the scope of patent application No. 1 or 10, wherein the layer sequence (2) has a semiconductor laser structure for vertical surface emission. 15. For example, a radiation-emitting semiconductor body (1) in the scope of application for a patent, wherein the layer sequence (2) has a light-emitting diode structure. 16. —A method for manufacturing a semiconductor body (1) capable of emitting radiation, the semiconductor body (1) is any one of items 1 to 9 or 13 to 15 (which According to any one of items 1 to 9), it is characterized by the following steps: a) preparing a crystal substrate (7); b) at the first process temperature by liquid phase epitaxy and An AlGaAs layer (4, 5, 6) is grown on the epitaxial substrate (7); c) the AlGaAs layer (4, 5, 6) is formed by metal organic vapor phase epitaxy or molecular beam epitaxy at the second process temperature; The layer sequence is grown on 540164 in September of the following year, and the structure is revised. 6. The scope of patent application (2) 0 17. The manufacturing method of item 16 in the scope of patent application, wherein the first process temperature is between 70 ° C and Between 1 0 0 0 ° C, the second process temperature is between 400 ° C and 800 ° C. 18. The manufacturing method according to claim 16 or 17, wherein the Jiajing substrate (7) is removed after step c). ia — a manufacturing method of a semiconductor body (1) that can emit radiation, the semiconductor body (1) is the patent application for item 10, 11 or 12 or item 1 3, 1 4 or 15 (which is attached to item 1 0, 11 or 12), characterized by the following steps: a) preparing an unsupported epitaxial substrate (11), which is composed of an AlGaAs multilayer structure and has an A1 content, such a The content of 1 makes AlGaAs transparent to the generated radiation, b) the layer sequence is grown on the epitaxial substrate by metal organic vapor phase epitaxy or molecular epitaxy at the second process temperature (2 ). 20. The manufacturing method according to item 19 of the scope of patent application, wherein the epitaxial substrate is made by a Vertical Gradient Freeze (VGF) method. 21 · —A method for manufacturing a substrate (3), which is used to grow a semiconductor body capable of emitting radiation, which is characterized by the following steps: a) preparing an epitaxial substrate (7); b) by liquid phase Jiajing A * AlGaAs layer (4,5,6) is grown on the Jiajing plate (7). The A1 content in the epitaxial layer decreases with the growth thickness of 540164. 6. The scope of the patent application gradually increases and the AlGaAs layer must be selected The thickness is such that the A1 content in it is not less than the radiation generated in the structure that can emit radiation-or it is less than the penetration limit only when the thickness reaches 30nm; c) repeat step b) until the substrate (by AlGaAs Layer (4,5,6) to the desired thickness. 22. A substrate (3) for the growth of a semiconductor body capable of emitting radiation, characterized in that it has one or more sequentially arranged AlGaAs layers (4, 5, 6), which are epitaxially formed by liquid phase And similar methods and have an average A1 content, this A1 content makes AlGaAs transparent to the radiation generated in a radiation-emitting semiconductor body, and in each AlGaAs layer From the side facing the first main surface of the substrate (3), the AlGaAs has a decreasing direction in a direction facing the side facing the second main surface of the substrate (3), which faces the first main surface. The A1 content, where the A1 content is not less than the radiation produced or less than the penetration limit 値 only when the thickness reaches 30nm.
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