TW540164B - Radiation-emitting semiconductor-body and its production method - Google Patents
Radiation-emitting semiconductor-body and its production method Download PDFInfo
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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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- 238000004519 manufacturing process Methods 0.000 title claims description 9
- 229910000980 Aluminium gallium arsenide Inorganic materials 0.000 claims abstract description 39
- 239000000758 substrate Substances 0.000 claims abstract description 31
- 238000000034 method Methods 0.000 claims abstract description 22
- 230000005855 radiation Effects 0.000 claims abstract description 22
- 238000004943 liquid phase epitaxy Methods 0.000 claims abstract description 10
- 230000007423 decrease Effects 0.000 claims abstract 3
- 238000000407 epitaxy Methods 0.000 claims abstract 3
- 239000004065 semiconductor Substances 0.000 claims description 31
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 claims description 9
- 229910052782 aluminium Inorganic materials 0.000 claims description 8
- 238000010521 absorption reaction Methods 0.000 claims description 6
- 229910052751 metal Inorganic materials 0.000 claims description 5
- 239000002184 metal Substances 0.000 claims description 5
- 239000013078 crystal Substances 0.000 claims description 2
- 239000012071 phase Substances 0.000 claims description 2
- 238000000927 vapour-phase epitaxy Methods 0.000 claims 3
- 239000007791 liquid phase Substances 0.000 claims 2
- 238000001451 molecular beam epitaxy Methods 0.000 claims 2
- 238000002161 passivation Methods 0.000 claims 2
- 230000035515 penetration Effects 0.000 claims 2
- QVGXLLKOCUKJST-UHFFFAOYSA-N atomic oxygen Chemical compound [O] QVGXLLKOCUKJST-UHFFFAOYSA-N 0.000 claims 1
- 230000003247 decreasing effect Effects 0.000 claims 1
- 239000007789 gas Substances 0.000 claims 1
- 239000001301 oxygen Substances 0.000 claims 1
- 229910052760 oxygen Inorganic materials 0.000 claims 1
- 239000002689 soil Substances 0.000 claims 1
- 235000012431 wafers Nutrition 0.000 description 4
- 210000001015 abdomen Anatomy 0.000 description 2
- 230000004927 fusion Effects 0.000 description 2
- 229910001218 Gallium arsenide Inorganic materials 0.000 description 1
- 238000000151 deposition Methods 0.000 description 1
- 230000008021 deposition Effects 0.000 description 1
- 238000002955 isolation Methods 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 230000035699 permeability Effects 0.000 description 1
- 238000002310 reflectometry Methods 0.000 description 1
- 230000003595 spectral effect Effects 0.000 description 1
Classifications
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L33/00—Semiconductor 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
- H01L33/02—Semiconductor 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
- H01L33/26—Materials of the light emitting region
- H01L33/30—Materials of the light emitting region containing only elements of Group III and Group V of the Periodic Table
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L33/00—Semiconductor 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
- H01L33/02—Semiconductor 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
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L33/00—Semiconductor 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
- H01L33/005—Processes
- H01L33/0062—Processes for devices with an active region comprising only III-V compounds
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L33/00—Semiconductor 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
- H01L33/005—Processes
- H01L33/0093—Wafer bonding; Removal of the growth substrate
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES 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
- H01S2301/00—Functional characteristics
- H01S2301/17—Semiconductor lasers comprising special layers
- H01S2301/173—The laser chip comprising special buffer layers, e.g. dislocation prevention or reduction
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES 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
- H01S5/00—Semiconductor lasers
- H01S5/10—Construction 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
- H01S5/16—Window-type lasers, i.e. with a region of non-absorbing material between the active region and the reflecting surface
- H01S5/164—Window-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
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES 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
- H01S5/00—Semiconductor lasers
- H01S5/10—Construction 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
- H01S5/18—Surface-emitting [SE] lasers, e.g. having both horizontal and vertical cavities
- H01S5/183—Surface-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
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-
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DE10056476A DE10056476B4 (en) | 2000-11-15 | 2000-11-15 | Radiation-emitting semiconductor body and method for its production |
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CN112038456A (en) * | 2015-02-10 | 2020-12-04 | 晶元光电股份有限公司 | Light emitting element |
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DE102004057802B4 (en) | 2004-11-30 | 2011-03-24 | Osram Opto Semiconductors Gmbh | Radiation-emitting semiconductor component with intermediate layer |
DE102013112740B4 (en) * | 2013-11-19 | 2021-03-18 | OSRAM Opto Semiconductors Gesellschaft mit beschränkter Haftung | Radiation-emitting semiconductor component |
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US4946542A (en) * | 1988-12-05 | 1990-08-07 | At&T Bell Laboratories | Crystal growth method in crucible with step portion |
US5103271A (en) * | 1989-09-28 | 1992-04-07 | Kabushiki Kaisha Toshiba | Semiconductor light emitting device and method of fabricating the same |
US5656829A (en) * | 1994-08-30 | 1997-08-12 | Showa Denko K.K. | Semiconductor light emitting diode |
JP3195194B2 (en) * | 1995-05-26 | 2001-08-06 | シャープ株式会社 | Semiconductor light emitting device and method of manufacturing the same |
JP3959434B2 (en) * | 1995-08-29 | 2007-08-15 | 昭和電工株式会社 | Light emitting diode element |
DE19630689C1 (en) * | 1996-07-30 | 1998-01-15 | Telefunken Microelectron | Semiconductor device and manufacturing method |
CN1227670A (en) * | 1996-08-07 | 1999-09-01 | 西门子公司 | Process for manufacturing an infrared-emitting luminescent diode |
US6057562A (en) * | 1997-04-18 | 2000-05-02 | Epistar Corp. | High efficiency light emitting diode with distributed Bragg reflector |
US6201264B1 (en) * | 1999-01-14 | 2001-03-13 | Lumileds Lighting, U.S., Llc | Advanced semiconductor devices fabricated with passivated high aluminum content III-V materials |
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2000
- 2000-11-15 DE DE10056476A patent/DE10056476B4/en not_active Expired - Fee Related
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2001
- 2001-11-06 TW TW090127499A patent/TW540164B/en not_active IP Right Cessation
- 2001-11-15 WO PCT/DE2001/004293 patent/WO2002065555A1/en active Application Filing
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CN112038456A (en) * | 2015-02-10 | 2020-12-04 | 晶元光电股份有限公司 | Light emitting element |
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DE10056476A1 (en) | 2002-05-23 |
WO2002065555A1 (en) | 2002-08-22 |
DE10056476B4 (en) | 2012-05-03 |
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