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TW200840095A - Nitride semiconductor light emitting element and method for manufacturing the same - Google Patents

Nitride semiconductor light emitting element and method for manufacturing the same Download PDF

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Publication number
TW200840095A
TW200840095A TW096148804A TW96148804A TW200840095A TW 200840095 A TW200840095 A TW 200840095A TW 096148804 A TW096148804 A TW 096148804A TW 96148804 A TW96148804 A TW 96148804A TW 200840095 A TW200840095 A TW 200840095A
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Taiwan
Prior art keywords
nitride semiconductor
layer
active layer
light
emitting device
Prior art date
Application number
TW096148804A
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Chinese (zh)
Inventor
Kuniyoshi Okamoto
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Rohm Co Ltd
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Publication of TW200840095A publication Critical patent/TW200840095A/en

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    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10HINORGANIC LIGHT-EMITTING SEMICONDUCTOR DEVICES HAVING POTENTIAL BARRIERS
    • H10H20/00Individual inorganic light-emitting semiconductor devices having potential barriers, e.g. light-emitting diodes [LED]
    • H10H20/80Constructional details
    • H10H20/81Bodies
    • H10H20/822Materials of the light-emitting regions
    • H10H20/824Materials of the light-emitting regions comprising only Group III-V materials, e.g. GaP
    • H10H20/825Materials of the light-emitting regions comprising only Group III-V materials, e.g. GaP containing nitrogen, e.g. GaN
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B82NANOTECHNOLOGY
    • B82YSPECIFIC USES OR APPLICATIONS OF NANOSTRUCTURES; MEASUREMENT OR ANALYSIS OF NANOSTRUCTURES; MANUFACTURE OR TREATMENT OF NANOSTRUCTURES
    • B82Y20/00Nanooptics, e.g. quantum optics or photonic crystals
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10HINORGANIC LIGHT-EMITTING SEMICONDUCTOR DEVICES HAVING POTENTIAL BARRIERS
    • H10H20/00Individual inorganic light-emitting semiconductor devices having potential barriers, e.g. light-emitting diodes [LED]
    • H10H20/80Constructional details
    • H10H20/81Bodies
    • H10H20/811Bodies having quantum effect structures or superlattices, e.g. tunnel junctions
    • H10H20/812Bodies having quantum effect structures or superlattices, e.g. tunnel junctions within the light-emitting regions, e.g. having quantum confinement structures
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10HINORGANIC LIGHT-EMITTING SEMICONDUCTOR DEVICES HAVING POTENTIAL BARRIERS
    • H10H20/00Individual inorganic light-emitting semiconductor devices having potential barriers, e.g. light-emitting diodes [LED]
    • H10H20/80Constructional details
    • H10H20/81Bodies
    • H10H20/813Bodies having a plurality of light-emitting regions, e.g. multi-junction LEDs or light-emitting devices having photoluminescent regions within the bodies
    • H10P14/24
    • H10P14/2908
    • H10P14/3216
    • H10P14/3416
    • 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
    • H01S5/04Processes or apparatus for excitation, e.g. pumping, e.g. by electron beams
    • H01S5/041Optical pumping
    • 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
    • H01S5/30Structure or shape of the active region; Materials used for the active region
    • H01S5/32Structure or shape of the active region; Materials used for the active region comprising PN junctions, e.g. hetero- or double- heterostructures
    • H01S5/3202Structure or shape of the active region; Materials used for the active region comprising PN junctions, e.g. hetero- or double- heterostructures grown on specifically orientated substrates, or using orientation dependent growth
    • H01S5/32025Structure or shape of the active region; Materials used for the active region comprising PN junctions, e.g. hetero- or double- heterostructures grown on specifically orientated substrates, or using orientation dependent growth non-polar orientation
    • 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
    • H01S5/30Structure or shape of the active region; Materials used for the active region
    • H01S5/32Structure or shape of the active region; Materials used for the active region comprising PN junctions, e.g. hetero- or double- heterostructures
    • H01S5/3202Structure or shape of the active region; Materials used for the active region comprising PN junctions, e.g. hetero- or double- heterostructures grown on specifically orientated substrates, or using orientation dependent growth
    • H01S5/320275Structure or shape of the active region; Materials used for the active region comprising PN junctions, e.g. hetero- or double- heterostructures grown on specifically orientated substrates, or using orientation dependent growth semi-polar orientation
    • 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
    • H01S5/30Structure or shape of the active region; Materials used for the active region
    • H01S5/34Structure or shape of the active region; Materials used for the active region comprising quantum well or superlattice structures, e.g. single quantum well [SQW] lasers, multiple quantum well [MQW] lasers or graded index separate confinement heterostructure [GRINSCH] lasers
    • H01S5/343Structure or shape of the active region; Materials used for the active region comprising quantum well or superlattice structures, e.g. single quantum well [SQW] lasers, multiple quantum well [MQW] lasers or graded index separate confinement heterostructure [GRINSCH] lasers in AIIIBV compounds, e.g. AlGaAs-laser, InP-based laser
    • H01S5/34333Structure or shape of the active region; Materials used for the active region comprising quantum well or superlattice structures, e.g. single quantum well [SQW] lasers, multiple quantum well [MQW] lasers or graded index separate confinement heterostructure [GRINSCH] lasers in AIIIBV compounds, e.g. AlGaAs-laser, InP-based laser with a well layer based on Ga(In)N or Ga(In)P, e.g. blue laser
    • 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
    • H01S5/40Arrangement of two or more semiconductor lasers, not provided for in groups H01S5/02 - H01S5/30
    • H01S5/4025Array arrangements, e.g. constituted by discrete laser diodes or laser bar
    • H01S5/4031Edge-emitting structures
    • H01S5/4043Edge-emitting structures with vertically stacked active layers
    • 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
    • H01S5/40Arrangement of two or more semiconductor lasers, not provided for in groups H01S5/02 - H01S5/30
    • H01S5/4025Array arrangements, e.g. constituted by discrete laser diodes or laser bar
    • H01S5/4087Array arrangements, e.g. constituted by discrete laser diodes or laser bar emitting more than one wavelength
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10HINORGANIC LIGHT-EMITTING SEMICONDUCTOR DEVICES HAVING POTENTIAL BARRIERS
    • H10H20/00Individual inorganic light-emitting semiconductor devices having potential barriers, e.g. light-emitting diodes [LED]
    • H10H20/80Constructional details
    • H10H20/81Bodies
    • H10H20/817Bodies characterised by the crystal structures or orientations, e.g. polycrystalline, amorphous or porous

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  • Chemical & Material Sciences (AREA)
  • Engineering & Computer Science (AREA)
  • Nanotechnology (AREA)
  • Physics & Mathematics (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Biophysics (AREA)
  • Optics & Photonics (AREA)
  • Crystallography & Structural Chemistry (AREA)
  • Led Devices (AREA)

Abstract

A nitride semiconductor light emitting element is provided with a III nitride semiconductor laminated structure having a laminated main surface other than a c-plane. The III nitride semiconductor laminated structure includes a first active layer, which has the main surface of the prescribed crystal plane other than the c-plane and generates light having a first wavelength, and a second active layer, which has the main surface of the prescribed crystal plane and generates light having a second wavelength different from the first wavelength. Furthermore, the III nitride semiconductor laminated structure may include an N-type nitride semiconductor layer and a P-type nitride semiconductor layer.; In such case, the first active layer may be between the N-type nitride semiconductor layer and the P-type nitride semiconductor layer and the second active layer may at areas other than the area between the N-type nitride semiconductor layer and the P-type semiconductor layer.

Description

200840095 九、發明說明: 【發明所屬之技術領域】 本發明係關於氮化物半導體發光元件(發光二極體、雷 射二極體等)及其製造方法。 田 【先前技術】[Technical Field] The present invention relates to a nitride semiconductor light-emitting element (light-emitting diode, laser diode, etc.) and a method of manufacturing the same. Field [prior art]

於III-V族半導體中作為V族元素使用氮之半導體係稱為 「III族氮化物半導體」,其代表例為氮化鋁(A1N)、氮化鎵 (GaN)、氮化銦(InN)。一般而言可表示為AlxInyGa^yN (O^x^l ’ ,於以下將此記為「氮化 鎵半導體」或「GaN半導體」。 據知有一種氮化物半導體之製造方法,其係在以c面為 主面之氮化鎵(GaN)基板上,藉由有機金屬化學汽相成長 (MOCVD法)法來使m族氮化物半導體成長。藉由適用此 方法,可形成具有N型層及P型層之GaN半導體疊層構造, 可製作利用此疊層構造之發光元件。此類發光元件例如可 作為液晶面板用背光之光源來利用。 在以c面作為主面之GaN基板上進行再成長之GaN半導體 之主面為c面。從此c面取出之光呈隨機偏光(無偏光)狀 恝。因此,射入液晶面板時,對應於射入側偏光板之特定 偏光以外均被遮蔽’對於射出側之亮度無助益。因此,具 有難以實現高亮度顯示(效率最大僅止50%)之問題。 為了解決此問題’檢討使以c面以外,亦即使以a面、m 面等無極性(Nonepolar)面,或以半極性(Semip〇lar)面為主 面之GaN半導體成長,來製作發光元件。若藉由以無極性 127612.doc 200840095 面或半極性面為主面之GaN半導體層,來製作具有P型層 或N型層之發光元件,可實現強偏光狀態之發光。因此, 藉由使此類發光元件之偏光方向與液晶面板之射入側偏光 板之通過偏光之方向一致,可減少射入側偏光板之損失。 其結果,可實現高亮度顯示。 [非專利文獻 1] T. Takeuchi et al·,Jap· J_ Appl. Phys. 39, 413-416, 2000 [非專利文獻2] A. Chakraborty,B· A· Haskell,H· S. Her, J· s· Speck,S,P. DenBaars,S· Nakamura and U· K.A semiconductor in which a nitrogen is used as a group V element in a group III-V semiconductor is referred to as a "group III nitride semiconductor", and representative examples thereof are aluminum nitride (A1N), gallium nitride (GaN), and indium nitride (InN). . In general, it can be expressed as AlxInyGa^yN (O^x^l ', which will be referred to as "GaN semiconductor" or "GaN semiconductor" hereinafter. It is known that a method for producing a nitride semiconductor is The m-type nitride semiconductor is grown by a metal organic chemical vapor phase growth (MOCVD) method on a gallium nitride (GaN) substrate having a c-plane as a main surface, and an N-type layer can be formed by applying this method. A GaN semiconductor stacked structure of a P-type layer can produce a light-emitting element having such a laminated structure. Such a light-emitting element can be used as a light source for a backlight for a liquid crystal panel, for example, on a GaN substrate having a c-plane as a main surface. The main surface of the grown GaN semiconductor is the c-plane. The light taken out from the c-plane is randomly polarized (no polarized light). Therefore, when it is incident on the liquid crystal panel, it is shielded in addition to the specific polarized light of the incident-side polarizing plate. It does not contribute to the brightness of the emission side. Therefore, it is difficult to achieve high-brightness display (the efficiency is only 50% maximum). In order to solve this problem, the review is based on the c-plane, and even the a-plane, m-plane, etc. Nonepolar face, A GaN semiconductor having a semi-polar (Semip〇lar) surface as a main surface is grown to produce a light-emitting element, and a P-type is formed by a GaN semiconductor layer having a polarity-free 127612.doc 200840095 surface or a semipolar plane as a main surface. The light-emitting element of the layer or the N-type layer can realize the light emission in a strong polarization state. Therefore, by making the polarization direction of such a light-emitting element coincide with the direction of polarization of the light-emitting plate on the incident side of the liquid crystal panel, the incident side can be reduced. Loss of the polarizing plate. As a result, high-brightness display can be achieved. [Non-Patent Document 1] T. Takeuchi et al., Jap J_ Appl. Phys. 39, 413-416, 2000 [Non-Patent Document 2] A. Chakraborty , B. A. Haskell, H. S. Her, J. s. Speck, S, P. DenBaars, S. Nakamura and U. K.

Mlshra: Jap. J. Appl. Phys. 44 (2005) L173 【發明内容】 [發明所欲解決之問題] 例如右欲實現白色發光,要與以往之白色LED(發光二 極體)之情況相同地與螢光體組合。亦即,藉由使發光元 件所备出之偏光光線射入螢光體,並將從此螢光體放出之 光取出至外部,可實現白色發光。 之2而"彳之螢光體放出之光為散射光,其為偏光方向隨機 源’、、、扁光光線。因此,若適用作為液晶面板之背光用光 、:在偏光板無法避免甚大之損失,未能實現高亮度顯 不 〇 之“方面,右形成111族氮化物半導體且具有500 rnn以上 性!光波長之性層,則可知此類活性層對於熱損傷耐受 半^具體而§ ’例如舉例於GaN基板i,使卵 •、成長,於此璺層由ΙΠ族氮化物半導體所組成之活 1276l2.(j〇c 200840095 性層,並進一步使P型GaN半導體層成長來形成發光二極 體構造之情況。此情況下,為了成為5〇〇 nm以上之發光波 長,必須於活性層取入銦。因此,活性層成長時之基板溫 度設為700°C〜800°C。另一方面,於形成於活性層上之1>型 GaN層之蠢晶成長時,基板溫度設為8〇〇ac以上。此時,活 性層會受到熱損傷,顯著損害其其發光效率。因此,未必 容易獲得500 nm以上之波長。 此發明之目的係在於提供一種可取出2種以上之波長峰 值之偏光光線,且容易進行其發光波長之控制及高效率化 之氮化物半導體發光元件及其製造方法,總言之即實現例 如偏光之白色發光二極體。 [解決問題之技術手段] 本發明之氮化物半導體發光元件係具備具有e面以外之 璺層主面之III族氮化物半導體疊層構造;前述m族氮化物 半導體豐層構造包含:第一活性層,其係具有c面以外之 特定結晶面之主面,產生第一波長之光,·及第二活性層, 其係具有丽述特定結晶面之主面,產生與前述第一波長不 同之第二波長之光。 若根據此結構,由於第一及第二活性層均具有共同結晶 面之主面,因此於相同方向產生偏光之光。藉由從第一及 第二活性層同時產生第一及第二波長之光,在視覺上會觀 測到此等之混色光。如此,可產生以m族氮化物半導體之 活性層之組成控制所無法產生之發光色(波長)之偏光,容 易控制視覺上之發光波長。 1276I2.doc 200840095 W述第一及第二活性層宜由AlxlnyGai.x_yN (0Sx$ 1, OSy^l,O^x+y^l)組成。 前述in族氮化物半導體疊層構造亦可進一步包含:N型 氮化物半導體層及P型氮化物半導體層。於此情況,前述 • 第一活性層位於前述N型氮化物半導體層及p型氮化物半導 • 體層間,前述第二活性層位於前述N型氮化物半導體層及P 型氮化物半導體層間以外之場所亦可。 φ 若根據此結構,藉由N型氮化物半導體層及p型氮化物 半導體層’來形成夾住第一活性層之發光二極體構造。因 此,藉由於第一活性層注入電流,可激發此第一活性層來 使其發光。關於第二活性層例如可藉由第一活性層所產生 之光來激發以使其發光。 由於第二活性層位於N型氮化物半導體層及p型氮化物 半導體層間以外之場所,因此可於形成此等之後形成第二 活性層。如此的話’由於第二活性層可避免N型或p型氮化 # 物半導體層之形成時之熱損傷,因此可容易控制其發光波 長。 前述第二活性層亦可對於前述P型氮化物半導體層位於 與前述第一活性層相反側。 " 而且,前述第二活性層亦可對於前述N型氮化物半導體 層位於與前述第一活性層相反側。 當然,第三活性層、第四活性層或進一步其他活性層亦 可進一步設置於前述N型氮化物半導體層及p型氮化物半導 體層間以外之%所。如此的話,由於會觀測到視覺上混合 127612.doc 200840095 3種以上之波長之偏光光線,因此可增加發光波長之控制 自由度。 前述氮化物半導體元件亦可進一步包含基板,其係具有 均為前述特定結晶面之第一主面及第二主面。此情況下, 前述III族氮化物半導體疊層構造亦可包含:第一部分,其 係包含疊層於前述基板之第一主面之前述第一活性層;及 第二部分,其係包含疊層於前述基板之第二主面之前述第 二活性層。 若根據此結構,III族氮化物半導體疊層構造被分配至基 板之一方主面側及另一方主面側。例如疊層於基板之第一 主面側之第一部分可為包含N型氮化物半導體層及p型氮化 物半導體層、以及配置於此等之間之第一活性層之結構。 藉此,於基板之第一主面側,藉由電流注入來激發第一活 性層以使其進行偏光發光,將其偏光光線經由基板而導引 至第一主面側之第二活性層,藉由光激發可使其進行偏光 發光。 前述第二主面宜為鏡面。 作為前述基板可使用藍寶石基板(例如以r面為主面)、 LiAh〇3基板、碳化矽基板(例如以瓜面為主面)、氮化鎵基 板(例如以a面或m面為主面)等。於Γ面藍寶石基板上可形 成a面ΠΙ族氮化物半導體層,於LiA12〇3基板上可形成瓜面 III族氮化物半導體層,於m面碳切基板上可形成祕⑴ 氮化鎵基板上可形成&面職氛 化物半導體層’於m面氮化鎵基板上可形心面⑴族氮化 127612.doc 200840095 物半導體層。 前述基板宜具有比前述第-活性層寬之帶隙。於前述基 ^為導電性基板(例如碳切基板或⑽基板)之情況時, 精由使其帶隙比第-活性層之帶隙寬,可抑制在基板之光 .吸收。藉此,可有效率地將第二活性層予以光激發。 • 、v⑥0月1J i^基板宜對於前述第-活性層之發光波 長呈透明(宜為9〇%以上之光穿透率)。藉此,將來自第一 • 雜層之光有效率地導引至第二活性層,可有效率地將第 二活性層予以光激發。 珂:第-活性層係藉由電流注入而發光,前述第二活性 層係藉由來自前述第一活性層之光所造成之光激發而發 光。 若根據此結構,關於第二活性層則不需要用以注入電流 、、、。構口此,結構變得簡單。而且,於ΠΙ族氮化物半導 體疊層構造之形成時,可於形成與第一活性層相關連之發 _ A —極體構造後,形成第二活性層,關於此第二活性層不 品要幵/成發光一極體構造。因此,可避免發光二極體構造 之形成時之熱損傷並形成第二活性層。藉此,第二活性層 可具有良好之發光效率。 刖述第一活性層亦可由帶隙比前述第二活性層大之Ιπ族 氣化物半導體組成。帶隙越大從而發光波長越短,活性層 之耐熱性變得越佳。因此,於Ν型氮化物半導體層及ρ型氮 化物半導體層間配置第一活性層,形成發光二極體構造, 並且於該發光二極體構造之外側配置第二活性層亦可。藉 I27612.doc 200840095 此,第一活性層可耐受III族氮化物半導體疊層構造之形成 時之高溫,第二活性層不置於該高溫環境下即可形成。因 此,第一及第二活性層均能以良好效率來進行偏光發光。 前述特定結晶面亦可為無極性面或半極性面。無極性面 . 之例為瓜面(10_10)及8面(ιυο)。作為半極性面之例可舉 出面、(1(M_3)面、(11-22)面。 關於本發明之一態樣之氮化物半導體發光元件之製造方 參 法’係具備具有e面以外之疊層主面之in族氮化物半導體 豐層構造;形成前述m族氮化物半導體疊層構造之步驟包 含以下步驟:形成具有c面以外之特定結晶面之主面,產 生第一波長之光之第一活性層之步驟;及將具有前述特定 結晶面之主面,產生比前述第一波長長之第二波長之光之 第二活性層,於形成前述ΠΙ族氮化物半導體疊層構造之構 成層中,形成溫度比該第二活性層之形成溫度高之所有層 後形成之步驟。 • 藉由此方法’發光波長甚長,因此耐熱性差之第二活性 層可避免受到熱損傷。藉此,第一及第二活性層均可具有 良好之發光特性,可進行第一及第二波長之光在視覺上混 合之發光色,例如白色之偏光發光。 ~ ΠΙ族氮化物半導體疊層構造之形成可藉由氫化物汽相成 長(HVPE: Hydride Vapor Phase Epitaxy)法或有機金屬化 予 A 相成長(MOCVD : Metal Organic Chemical Vapor Deposition)法來進行。 關於本發明之其他態樣之氮化物半導體發光元件之製造 127612.doc -11 - 200840095 方,係具備具有C面以外之疊層主面之m族氮化物半導 t層構造,·形成前述111族氮化物半導體疊層構造之步驟 包3以了步驟:形成第一導電型之氮化物半導體層之步 驟:於則述第-導電型之氮化物半導體層Jl,形成具有c 面乂外之特定結晶面之主面,產生第一波長之 性層之半_ ^ ^ V驟;於前述第一活性層上,形成第二導電型之 化物半:體層之步驟;及將具有前述特定結晶面之主面, /生:别述第一波長長之第二波長之光之第二活性層,於 形ί =第一導電型之氮化物半導體層、前述第-活性層 及:述弟二導電型之氮化物半導體層後形成之步驟。 ::據此方法’於形成與第一活性層相關連之發光二極 盥Μ k谈,形成第二活性層。因此,第二活性層不會受到 :::活性層相關連之發光二極體構造形成時之高溫處理 :成之熱損傷。如此’第一及第二活性層均能以良好之 發光政率,來分別產生第一及第二波長之偏光光線。 本::珂述第二活性層之步驟宜為於形成前述111族氮化物 h體豐層構造之其他所有構成層後,形成該第二活性層 ^步驟。根據此方法’可確實地避免第二活性層受到高溫 處理所造成之熱損傷。 刖述第二波長亦可為500 nm以上。因此,前述 亦可例如小於500 nme / # 知此外,關於氮化物半導體發光元件之製造方法,亦可與 氮化物半導體發光元件之發明之情況同樣地變形。 本發明之上述或進-步其他㈣、特徵及㈣,可藉由 127612.doc -12- 200840095 參考附圖並於以下所述之實施型態之說明來闡明。 【實施方式】 圖1係用以說明有關本發明之一實施型態之氮化物半導 體發光元件之構造之圖解剖面圖。此氮化物半導體發光元 • 件係於GaN(氮化鎵)基板1上,使作為III族氮化物半導體疊 層構造之GaN半導體層2成長而構成。Mlshra: Jap. J. Appl. Phys. 44 (2005) L173 [Description of the Invention] [Problems to be Solved by the Invention] For example, the right to realize white light emission is the same as in the case of the conventional white LED (light emitting diode). Combined with a phosphor. That is, white light is emitted by causing the polarized light which is prepared by the light-emitting element to be incident on the phosphor and extracting the light emitted from the phosphor to the outside. The light emitted by the fluorescent body is the scattered light, which is a random source of polarization direction, and flat light. Therefore, if it is applied as a backlight for a liquid crystal panel, it is impossible to avoid a large loss in the polarizing plate, and a high-brightness display is not realized. The group 111 nitride semiconductor is formed right and has a r r or more. For the layer, it can be seen that such an active layer is resistant to thermal damage. For example, exemplified on the GaN substrate i, the egg is grown, and the layer is composed of a bismuth nitride semiconductor. (J〇c 200840095 layer, and further growth of the P-type GaN semiconductor layer to form a light-emitting diode structure. In this case, in order to obtain an emission wavelength of 5 〇〇 nm or more, it is necessary to take indium in the active layer. Therefore, the substrate temperature at the time of growth of the active layer is set to 700 ° C to 800 ° C. On the other hand, when the stray crystal of the 1 > type GaN layer formed on the active layer is grown, the substrate temperature is set to 8 〇〇 ac or more. At this time, the active layer is thermally damaged, which significantly impairs its luminous efficiency. Therefore, it is not always easy to obtain a wavelength of 500 nm or more. The object of the invention is to provide a polarized light which can take out more than two kinds of wavelength peaks. A nitride semiconductor light-emitting device which is easy to control the light-emitting wavelength and which is highly efficient, and a method for producing the same, and in general, a white light-emitting diode such as a polarized light is realized. [Technical means for solving the problem] The nitrogen of the present invention The semiconductor light-emitting device includes a group III nitride semiconductor stacked structure having a tantalum main surface other than the e-plane, and the m-nitride semiconductor layer structure includes a first active layer having a specific crystal other than the c-plane The main surface of the surface generates light of a first wavelength, and a second active layer having a main surface of a specific crystal plane of the reference, and generating light of a second wavelength different from the first wavelength. Since the first and second active layers each have a main surface of the common crystal plane, the polarized light is generated in the same direction. By simultaneously generating the first and second wavelengths of light from the first and second active layers, visually Such mixed color light is observed. Thus, polarization of the luminescent color (wavelength) which cannot be produced by controlling the composition of the active layer of the group m nitride semiconductor can be generated, and the vision can be easily controlled. The wavelength of the light emitted. 1276I2.doc 200840095 The first and second active layers are preferably composed of AlxlnyGai.x_yN (0Sx$ 1, OSy^l, O^x+y^l). Further, the N-type nitride semiconductor layer and the P-type nitride semiconductor layer may be further included. In this case, the first active layer is located between the N-type nitride semiconductor layer and the p-type nitride semiconductor layer, The two active layers may be located outside the N-type nitride semiconductor layer and the P-type nitride semiconductor layer. φ According to this structure, the N-type nitride semiconductor layer and the p-type nitride semiconductor layer ' are formed to be sandwiched. Light-emitting diode structure of the first active layer. Therefore, the first active layer can be excited to emit light by injecting a current into the first active layer. The second active layer can be excited by, for example, light generated by the first active layer to cause it to emit light. Since the second active layer is located outside the N-type nitride semiconductor layer and the p-type nitride semiconductor layer, the second active layer can be formed after the formation of the above. In this case, since the second active layer can avoid thermal damage at the time of formation of the N-type or p-type nitride semiconductor layer, the luminescence wavelength can be easily controlled. The second active layer may also be located on the opposite side of the first active layer to the P-type nitride semiconductor layer. < Moreover, the second active layer may be located on the opposite side of the first active layer to the N-type nitride semiconductor layer. Of course, the third active layer, the fourth active layer or still further active layers may be further provided in a ratio other than between the N-type nitride semiconductor layer and the p-type nitride semiconductor layer. In this case, since it is observed that the polarized light of three or more wavelengths is visually mixed, the control freedom of the emission wavelength can be increased. The nitride semiconductor device may further include a substrate having a first main surface and a second main surface which are all the specific crystal faces. In this case, the group III nitride semiconductor stacked structure may further include: a first portion including the first active layer laminated on the first main surface of the substrate; and a second portion including the laminate The second active layer on the second main surface of the substrate. According to this configuration, the group III nitride semiconductor stacked structure is distributed to one of the main surface sides and the other main surface side of the substrate. For example, the first portion laminated on the first main surface side of the substrate may be a structure including an N-type nitride semiconductor layer, a p-type nitride semiconductor layer, and a first active layer disposed therebetween. Thereby, on the first main surface side of the substrate, the first active layer is excited by current injection to cause polarized light emission, and the polarized light is guided to the second active layer on the first main surface side via the substrate. It can be polarized by light excitation. The aforementioned second main surface is preferably a mirror surface. As the substrate, a sapphire substrate (for example, a r-plane as a main surface), a LiAh〇3 substrate, a tantalum carbide substrate (for example, a melon surface as a main surface), or a gallium nitride substrate (for example, an a-plane or an m-plane as a main surface) may be used. )Wait. An a-plane lanthanide nitride semiconductor layer can be formed on the sapphire substrate, and a mesa-type nitride semiconductor layer can be formed on the LiA12〇3 substrate to form a secret (1) gallium nitride substrate on the m-plane carbon-cut substrate. Forming & the masking semiconductor layer 'on the m-plane gallium nitride substrate can be formed on the surface of the (1) group nitride 127612.doc 200840095 semiconductor layer. The aforementioned substrate preferably has a band gap wider than that of the aforementioned first active layer. In the case where the above-mentioned substrate is a conductive substrate (for example, a carbon-cut substrate or a (10) substrate), the band gap is made wider than that of the first active layer, and light absorption on the substrate can be suppressed. Thereby, the second active layer can be efficiently photoexcited. • The v60 month 1J i^ substrate should be transparent to the illuminating wavelength of the first active layer (preferably a light transmittance of 9% or more). Thereby, the light from the first impurity layer is efficiently guided to the second active layer, and the second active layer can be efficiently photoexcited.珂: The first active layer emits light by current injection, and the second active layer emits light by excitation of light from the light of the first active layer. According to this configuration, it is not necessary to inject current, or with respect to the second active layer. By constructing this, the structure becomes simple. Moreover, in the formation of the bismuth nitride semiconductor stacked structure, the second active layer may be formed after forming the FET-related structure associated with the first active layer, and the second active layer is not required.幵 / into a luminous body structure. Therefore, thermal damage at the time of formation of the light-emitting diode structure can be avoided and the second active layer can be formed. Thereby, the second active layer can have good luminous efficiency. The first active layer may also be composed of a Ι-π-type vaporized semiconductor having a larger band gap than the second active layer. The larger the band gap, the shorter the emission wavelength, and the better the heat resistance of the active layer. Therefore, the first active layer is disposed between the bismuth nitride semiconductor layer and the p-type nitride semiconductor layer to form a light-emitting diode structure, and the second active layer may be disposed outside the light-emitting diode structure. By I27612.doc 200840095, the first active layer can withstand the high temperature at the time of formation of the group III nitride semiconductor stacked structure, and the second active layer can be formed without being placed in the high temperature environment. Therefore, both the first and second active layers can perform polarized light emission with good efficiency. The specific crystal face may also be a non-polar or semi-polar face. Non-polar surface. Examples are melon (10_10) and 8 (ιυο). Examples of the semipolar surface include a surface, a (1 (M_3) plane, and a (11-22) plane. The method for producing a nitride semiconductor light-emitting device according to an aspect of the present invention has a surface other than the e-plane. The indium nitride semiconductor semiconductor layer structure of the laminated main surface; the step of forming the m-type nitride semiconductor stacked structure includes the steps of: forming a main surface having a specific crystal plane other than the c-plane to generate light of a first wavelength a step of forming a first active layer; and a second active layer having a main surface of the specific crystal face and generating light of a second wavelength longer than the first wavelength to form the cascading nitride semiconductor stacked structure In the constituent layer, a step of forming all the layers having a temperature higher than the formation temperature of the second active layer is formed. • By this method, the emission wavelength is very long, so that the second active layer having poor heat resistance can be protected from thermal damage. Therefore, both the first and second active layers can have good luminescence characteristics, and can perform visually mixed illuminating colors of the first and second wavelengths of light, for example, white polarized luminescence. ~ ΠΙ-nitride semiconductor The formation of the layer structure can be carried out by a HVPE (Hydride Vapor Phase Epitaxy) method or a metal organic chemical Vapor Deposition (MOCVD) method. In the production of a nitride semiconductor light-emitting device, 127612.doc -11 - 200840095, a group-group nitride semi-conductive t-layer structure having a laminated main surface other than the C-plane is provided, and the group 111 nitride semiconductor stacked structure is formed. Step 3 includes the steps of forming a nitride semiconductor layer of a first conductivity type: forming a main surface of a specific crystal plane having a c-plane outside the nitride semiconductor layer J1 of the first conductivity type, resulting in a a half-wavelength layer of the first wavelength of the first conductive layer; a step of forming a second conductivity type half: body layer; and a main surface having the specific crystal face, / a second active layer of light having a second wavelength of a first wavelength is formed after the nitride semiconductor layer of the first conductivity type, the first active layer, and the nitride semiconductor layer of the second conductivity type step According to this method, a second active layer is formed by forming a light-emitting diode associated with the first active layer. Therefore, the second active layer is not exposed to the light-emitting diode associated with the active layer::: The high temperature treatment during the formation of the body structure: thermal damage. Thus both the first and second active layers can produce the first and second wavelengths of polarized light with a good illuminating rate. The step of the second active layer is preferably to form the second active layer after forming all of the other constituent layers of the above-mentioned Group 111 nitride h bulk layer structure. According to this method, the second active layer can be surely prevented from being subjected to high temperature treatment. The resulting thermal damage. The second wavelength can also be above 500 nm. Therefore, the above-described method of manufacturing the nitride semiconductor light-emitting device can be modified in the same manner as in the case of the invention of the nitride semiconductor light-emitting device, for example, less than 500 nme / #. The above or further (4), features and (4) of the present invention can be clarified by the description of the embodiments described below with reference to the accompanying drawings by 127612.doc -12-200840095. [Embodiment] Fig. 1 is a schematic cross-sectional view for explaining the structure of a nitride semiconductor light-emitting element according to an embodiment of the present invention. This nitride semiconductor light-emitting element is formed on a GaN (gallium nitride) substrate 1 and is formed by growing a GaN semiconductor layer 2 which is a group III nitride semiconductor stacked structure.

GaN半導體層2係具有從GaN基板1側,依序疊層N型接 φ 觸層21、作為第一活性層(發光層)之第一多重量子井 (MQW : Multiple-Quantum Well)層 22、GaN 最終障壁層 25、P型電子阻止層23、P型接觸層24、及作為第二活性層 (叙光層)之苐一多重量子井層26之疊層構造。P型接觸層 24層之表面具有往第二多重量子井層%侧方引出之引出 部’於此引出部形成作為透明電極之陽極電極3。進一步 於此陽極電極3之一部分,接合有布線連接用之連接部4。 而且,於N型接觸層21接合有陰極電極5。 Φ GaN基板1接合於支持基板(布線基板)1〇。於支持基板10 之表面形成有布線11,12。然後,連接部4與布線n係以接 合金屬線13連接,陰極5與布線12係以接合金屬線〗4連 接。進一步藉由環氧樹脂等透明樹脂來密封GaN半導體層 2陽極電極3、連接部4及陰極電極5、以及接合金屬線 13, 14,藉此構成氮化物半導體發光元件。 N型接觸層21係由作為N型摻雜物而添加有矽2NsGaN 層所組成。層厚宜為3 μηι。矽之摻雜濃度為例如1〇18 em·3。 更具體而言,N型接觸層21係由在GaN基板丨上(或Α1Ν^8 127612.doc -13- 200840095 上)結晶成長之N型GaN半導體所組成。 第一多重量子井層22及第二多重量子井層26分別例如以 特疋週期(例如5週期),交互地疊層有摻雜矽之InGaN層 (里子井層。例如3 nm厚)與GaN層(障壁層。例如9 nm 尽)於弟一多重量子井層22與p型電子阻止層23間,疊層 有GaN最終障壁層25(例如40 nm厚)。 第一多重量子井層22夾在N型接觸層21與P型接觸層24 間’形成發光二極體構造。此第一多重量子井層22之發光 波長小於500 nm。更具體而言為例如46〇 nm(藍色波長 區)。 關於P型接觸層24而言,第二多重量子井層26配置於與 第一多重量子井層22相反側,藉此位於前述發光二極體構 造外。此第二多重量子井層26之發光波長為500 nm以上。 更具體而言為例如5〇〇 nm〜600 nm(綠色〜黃色波長區)。 亦即,第二多重量子井層26之發光波長比第一多重量子 井層22之發光波長更長。換言之,第二多重量子井層26之 帶隙(更具體而言為InGaN層之帶隙)比第一多重量子井層 22之f隙(更具體而言為InGaN層之帶隙)小。帶隙之調整 可藉由調整銦(In)之組成比來進行。 例如若第一多重量子井層22之發光波長設為藍色波長 區’第二多重量子井層26之發光波長設為黃色波長區 (560 nm〜600 nm),則藉由視覺上混合藍色光與黃色光, 在視覺上可實現白色發光。The GaN semiconductor layer 2 has a first multi-quantum well (MQW) layer 22 which is an N-type Φ contact layer 21 and a first active layer (light-emitting layer) from the GaN substrate 1 side. a GaN final barrier layer 25, a P-type electron blocking layer 23, a P-type contact layer 24, and a stacked structure of a plurality of quantum well layers 26 as a second active layer (synthesizing layer). The surface of the P-type contact layer 24 has a lead-out portion which is drawn to the side of the second multiple quantum well layer, and the lead portion 3 as a transparent electrode is formed at the lead portion. Further, a portion of the anode electrode 3 is joined to the connecting portion 4 for wiring connection. Further, the cathode electrode 5 is bonded to the N-type contact layer 21. The Φ GaN substrate 1 is bonded to a support substrate (wiring substrate) 1A. Wirings 11, 12 are formed on the surface of the support substrate 10. Then, the connection portion 4 and the wiring n are connected by the bonding metal wires 13, and the cathode 5 and the wiring 12 are connected by the bonding metal wires 4. Further, the GaN semiconductor layer 2 anode electrode 3, the connection portion 4 and the cathode electrode 5, and the bonding wires 13 and 14 are sealed by a transparent resin such as an epoxy resin to constitute a nitride semiconductor light-emitting device. The N-type contact layer 21 is composed of a 矽2NsGaN layer added as an N-type dopant. The layer thickness should be 3 μηι. The doping concentration of cerium is, for example, 1 〇 18 em·3. More specifically, the N-type contact layer 21 is composed of an N-type GaN semiconductor grown on the GaN substrate (or Α1Ν^8 127612.doc -13-200840095). The first multiple quantum well layer 22 and the second multiple quantum well layer 26 are alternately laminated with a germanium-doped InGaN layer (for example, 3 nm thick), for example, in a characteristic period (for example, 5 cycles). A GaN final barrier layer 25 (for example, 40 nm thick) is laminated with a GaN layer (a barrier layer such as 9 nm) between the multiple quantum well layer 22 and the p-type electron blocking layer 23. The first multiple quantum well layer 22 is sandwiched between the N-type contact layer 21 and the P-type contact layer 24 to form a light-emitting diode structure. The first multiple quantum well layer 22 has an emission wavelength of less than 500 nm. More specifically, for example, 46 〇 nm (blue wavelength region). With respect to the P-type contact layer 24, the second multiple quantum well layer 26 is disposed on the opposite side of the first multiple quantum well layer 22, thereby being located outside of the above-described light-emitting diode structure. The second multiple quantum well layer 26 has an emission wavelength of 500 nm or more. More specifically, for example, 5 〇〇 nm to 600 nm (green to yellow wavelength region). That is, the second multiple quantum well layer 26 has a longer wavelength of illumination than the first multiple quantum well layer 22. In other words, the band gap of the second multiple quantum well layer 26 (more specifically, the band gap of the InGaN layer) is smaller than the f-gap of the first multiple quantum well layer 22 (more specifically, the band gap of the InGaN layer). . The adjustment of the band gap can be performed by adjusting the composition ratio of indium (In). For example, if the illuminating wavelength of the first multiple quantum well layer 22 is set to the blue wavelength region, and the illuminating wavelength of the second multiple quantum well layer 26 is set to the yellow wavelength region (560 nm to 600 nm), by visual mixing Blue light and yellow light can visually achieve white light.

p型電子阻止層23係由添加作為P型摻雜物之鎭之AlGaN 127612.doc -14 - 200840095 層所組成。層厚為例如28 nm。鎂的摻雜濃度為例如 3xl019 cnT3 〇 P型接觸層24係由高濃度地添加作為p型摻雜物之鎂之The p-type electron blocking layer 23 is composed of a layer of AlGaN 127612.doc -14 - 200840095 added as a P-type dopant. The layer thickness is, for example, 28 nm. The doping concentration of magnesium is, for example, 3xl019 cnT3 〇 The P-type contact layer 24 is added with high concentration as a p-type dopant of magnesium.

GaN層所組成。層厚為例如7〇 nm。鎂的摻雜濃度為例如 1020 cm'3 〇 陽極電極3係由犯及^所構成之透明薄金屬層(例如 200A以下)構成。 陰極電極係由Ti及A1層所構成之膜。The GaN layer is composed of. The layer thickness is, for example, 7 〇 nm. The doping concentration of magnesium is, for example, 1020 cm'3 〇. The anode electrode 3 is composed of a transparent thin metal layer (for example, 200 A or less) composed of a fine electrode. The cathode electrode is a film composed of Ti and an A1 layer.

GaN基板1係由具有〇面以外之主面之GaN所組成之基 板。更具體而言,其以無極性面或半極性面為主面者。其 宜為以從無極性面之面方位具有± i。以内之傾角之面,或 以從半極性面之面方位具有±1。以内之傾角之面為主面之The GaN substrate 1 is a substrate composed of GaN having a main surface other than the facet. More specifically, it is mainly a non-polar or semi-polar surface. It is preferably such that it has a ± i orientation from the plane of the non-polar surface. The surface of the dip inside, or ±1 from the plane of the semi-polar surface. The face of the dip inside is the main face

GaN單晶基板。GaN半導體層2之各層之疊層主面係按照GaN single crystal substrate. The laminated main surface of each layer of the GaN semiconductor layer 2 is in accordance with

GaN基板1之主面之結晶面。亦即,GaN半導體層2之構成 層之主面均與GaN基板!之主面之結晶面具有相同結晶 面0 若k布線11、12,於陽極電極3及陰極電極5間施加順向 電壓,則第一多重量子井層22會由電流注入激發而發光' 發光機制為二極體發光或EL(電激發光)均.可。由於GW基 板1之主面為c面以外之特定結晶面(無極性面或半極性 面)’因此第一多重量子井層22之主面亦成為c面以外之結 晶面(與GaN基板1同一結晶面)。因此,第一多重量子井層 22會產生偏光光線。 另一方面,若從第一多重量子井層22產生之光射入第二 127612.doc -15- 200840095 多重量子井層26,則此第二多重量子井層26會被光激發而 發光。第二多重量子井層26之主面亦與GaN基板1為同一 結晶面。因此,第二多重量子井層26係產生與第一多重量 子井層22相同偏光方向之偏光光線。 如此,於視覺上混合而觀測到從第一及第二多重量子井 層22、26發出之各偏光光線。因此,視覺上可產生第一及 第二多重量子井層22、26之發光色混色之偏光。The crystal plane of the main surface of the GaN substrate 1. That is, the main faces of the constituent layers of the GaN semiconductor layer 2 are bonded to the GaN substrate! The crystal faces of the main faces have the same crystal face 0. If the k wires 11 and 12 are applied, a forward voltage is applied between the anode electrode 3 and the cathode electrode 5, and the first multiple quantum well layer 22 is excited by current injection to emit light. The luminescence mechanism is either diode luminescence or EL (electroluminescence). Since the main surface of the GW substrate 1 is a specific crystal plane (non-polar plane or semi-polar plane) other than the c-plane, the main surface of the first multiple quantum well layer 22 also becomes a crystal plane other than the c-plane (with the GaN substrate 1) Same crystal face). Therefore, the first multiple quantum well layer 22 produces polarized light. On the other hand, if light generated from the first multiple quantum well layer 22 is incident on the second 127612.doc -15-200840095 multiple quantum well layer 26, the second multiple quantum well layer 26 is excited by light to emit light. . The main surface of the second multiple quantum well layer 26 is also the same crystal plane as the GaN substrate 1. Thus, the second multiple quantum well layer 26 produces polarized light of the same polarization direction as the first multi-weight sub-well layer 22. Thus, the respective polarized rays emitted from the first and second multiple quantum well layers 22, 26 are observed visually mixed. Therefore, the polarization of the luminescent color mixing of the first and second multiple quantum well layers 22, 26 can be visually produced.

圖2係表不III族氮化物半導體之結晶構造之單元胞之圖 解圖。III族氮化物半導體之結晶構造能以六方晶系來逼 近,以沿著六角柱之軸向之c軸為法線之面(六角柱之頂面) 為c面(0001)。於III族氮化物半導體,分極方向沿著c軸。 因此,由於c面係於+C軸與-C軸顯示出不同性質,因此稱 為極性面(Polar Plane)。另一方面,六角柱之側面分別為瓜 面(10-10),通過不相鄰之1對稜線之面為a面(11_2〇)。此等 係對於c面呈直角之結晶面,由於對於分極方向呈正交, 因此為未有極性之面,亦即無極性面(N〇np〇lar plane)。進 一步而言,對於c面傾斜(非平行亦非直角)之結晶面對於分 極方向斜向地交叉,因此為具有些許極性之平面,亦即半 極性面(SemiP〇lar Plane)。半極性面之具體例為 面、(10-1-3)面、(11-22)面等。 面之偏角與該結晶面 於非專利文獻1表示對於c面之結晶 之法線方向之分極之關係、。從此非專利文獻i可謂⑴% 面、(1〇-12)面等亦為分極少之結晶面,即為用以取出大偏 光狀態之光所可能採用之甚有希望之結晶面。 127612.doc •16- 200840095 例如以m面為主面之GaN單晶基板可從以〇面為主面之 GaN單晶切出並製作。切出之基板之m面例如藉由化學機 械研磨處理來研磨,製成關於(0001)方向及(11_2〇)方向雙 方之方位誤差為±1。以内(宜為±〇3。以内)。如此,獲得以历 面為主面’且無轉位或疊層缺陷該類結晶缺陷之GaN單晶 基板。於此類GaN單晶基板之表面,僅止於產生原子層級 之階差。Fig. 2 is a diagram showing the unit cell of the crystal structure of the group III nitride semiconductor. The crystal structure of the group III nitride semiconductor can be approximated by a hexagonal system, and the surface along the c-axis in the axial direction of the hexagonal column (the top surface of the hexagonal column) is the c-plane (0001). In the group III nitride semiconductor, the polarization direction is along the c-axis. Therefore, since the c-plane exhibits different properties on the +C axis and the -C axis, it is called Polar Plane. On the other hand, the side faces of the hexagonal columns are melon faces (10-10), respectively, and the faces of the pair of ridgelines which are not adjacent are a face (11_2〇). These are crystal planes having a right angle to the c-plane, and since they are orthogonal to the polarization direction, they are surfaces having no polarity, that is, a non-polar plane (N〇np〇lar plane). Further, the crystal faces of the c-plane tilt (non-parallel or non-right angle) intersect obliquely with respect to the polarization direction, and thus are planes having a slight polarity, that is, semi-polar planes. Specific examples of the semipolar surface are a surface, a (10-1-3) plane, a (11-22) plane, and the like. The eccentricity of the surface and the crystal surface are shown in Non-Patent Document 1 as a relationship between the polarization of the normal direction of the crystal of the c-plane. From the non-patent literature 1, it can be said that the (1)% plane, the (1〇-12) plane, and the like are also minute crystal planes, which is a promising crystal plane which may be used for taking out light in a large polarized state. 127612.doc •16- 200840095 For example, a GaN single crystal substrate having an m-plane as a main surface can be cut and produced from a GaN single crystal having a facet as a main surface. The m-plane of the cut substrate is polished by, for example, chemical mechanical polishing to produce an azimuth error of ±1 for both the (0001) direction and the (11_2〇) direction. Within (should be ±〇3.). Thus, a GaN single crystal substrate having a crystal front defect and having no indexing or lamination defects is obtained. On the surface of such a GaN single crystal substrate, only the step of the atomic level is generated.

於如此獲传之GaN單晶基板上,可藉由m〇CVD法來使 GaN半導體層2成長。 圖3係用以說明為了使構成GaN半導體層2之各層成長之 處理裝置之結構之圖解圖。於處理室3〇内,配置有内建加 熱益31之基座32。基座32係結合於旋轉軸33,此旋轉軸33 係由配置於處理室30外之旋轉驅動機構34旋轉。藉此,於 基座32保持處理對象之晶圓35,以便可於處理㈣内,將 晶圓35升溫至特定溫度,且可使其旋轉。晶圓⑽、構成前 现urarsi丞槪1之例如GaN單晶晶圓。 於處理室观接有排氣配f 36。排氣配f 36連接於轉式 泵等排氣設備。藉此,處理室3G内之壓力成為ι/ι〇氣壓〜 常壓(宜為職壓程度),始終將處理室則之氣氛進行排 氣0 另一方面,於處理室3G導人有原料氣體供給路4〇, I係 用以朝向保持於基座32之晶圓35之表面,供給原料氣體。 於此原料氣體供給路4〇i拿技女., 路運接有:供給作為氮原料氣體 之氣原料配管41、供給作為錄㈣*之三甲二:) 127612.doc -17- 200840095 之鎵原料配管42、供給作為鋁原料氣體之 之鋁原料配管43、供給作為銦原 7竹轧骽之二甲基銦(TMIn) 之铜原料配管44、作為餻;5> μ 下為鎮原枓亂體之乙基環戊二烯鎂 (EtChMg)之鎂原料配管4S、 次作為矽之原料氣體之矽烷 卿4)之石夕原料配管46。於此等原料配管41〜46分別介裝有 闕51〜56。各原料氣體均與由氫或氮、或由此等雙方所組 成之載子氣體一同供給。On the GaN single crystal substrate thus obtained, the GaN semiconductor layer 2 can be grown by the m〇CVD method. Fig. 3 is a schematic view for explaining the structure of a processing apparatus for growing the layers constituting the GaN semiconductor layer 2. A susceptor 32 having a built-in heating benefit 31 is disposed in the processing chamber 3A. The base 32 is coupled to a rotating shaft 33 that is rotated by a rotary drive mechanism 34 disposed outside the processing chamber 30. Thereby, the wafer 35 to be processed is held on the susceptor 32 so that the wafer 35 can be heated to a specific temperature and rotated in the process (4). The wafer (10), for example, a GaN single crystal wafer constituting the front urarsi丞槪1. An exhaust gas distribution f 36 is observed in the processing chamber. The exhaust gas is equipped with f 36 connected to an exhaust device such as a rotary pump. Thereby, the pressure in the processing chamber 3G becomes ι/ι〇 atmospheric pressure to normal pressure (it is the degree of occupational pressure), and the atmosphere in the processing chamber is always exhausted. On the other hand, the raw material gas is introduced in the processing chamber 3G. The supply path 4 is for supplying the material gas toward the surface of the wafer 35 held by the susceptor 32. The raw material gas supply path 4〇i is taken by the technical woman. The road transport is provided with a gas raw material supply pipe 41 as a nitrogen source gas, and a gallium raw material supplied as a recording material (4)*: 127612.doc -17- 200840095 The pipe 42 is supplied with an aluminum raw material pipe 43 as an aluminum raw material gas, and a copper raw material pipe 44 as a dimethyl indium (TMIn) of the indium raw material 7 is rolled as a crucible; 5 > μ is a Zhenyuan disorder The magnesium raw material piping 4S of the ethyl cyclopentadienyl magnesium (EtChMg) and the Shixi raw material piping 46 of the decane-clearing material 4). These raw material pipes 41 to 46 are respectively provided with 阙51 to 56. Each of the material gases is supplied together with a carrier gas composed of hydrogen or nitrogen or the like.

例如將以m面作為主面之GaN單晶晶圓,作為晶圓加 保持於基座32。於此狀態下,預先將閥關閉,打開 ^原料闊51 ’將載子氣體及氨氣(氮原料氣體)供給至處理 室30内。進-步進行對於加熱器31之通電,晶圓溫度升溫 至1000°C〜1100°C(例如l〇5(TC)e藉此,可不產生表面紊亂 並使GaN半導體成長。 待機至晶圓温度達到1〇00。(:〜1100。(:後,氮原料閥51' 鎵原料閥52及矽原料閥56打開。藉此,從原料氣體供給路 4〇,與載子氣體一同供給有氨、三甲基鎵及矽烷。其結 果’於晶圓35之表面,成長有由摻雜矽之GaN層所組成之 N型接觸層21。 於形成N型接觸層21後,接著矽原料閥56會關閉,進行 第一多重量子井層22之成長。第一多重量子井層22之成長 係藉由交互地執行以下步驟來進行:藉由打開氮原料閥 51、鎵原料閥52及銦原料闊54,並將氨、三甲基鎵及三甲 基銦供給往晶圓35,來使InGaN層(量子井層)成長之步 驟;及關閉銦原料閥54,打開氮原料閥51及鎵原料閥52, 127612.doc -18 - 200840095 將錢及二甲基鎵供給至晶圓35,來使無添加之GaN層(P章壁For example, a GaN single crystal wafer having an m-plane as a main surface is held as a wafer on the susceptor 32. In this state, the valve is closed in advance, and the raw material width 51 is opened to supply the carrier gas and the ammonia gas (nitrogen source gas) into the processing chamber 30. Stepping on the heater 31, the wafer temperature is raised to 1000 ° C to 1100 ° C (for example, l 〇 5 (TC) e, thereby preventing surface turbulence and GaN semiconductor growth. Standby to wafer temperature 〇 。 。 。 ( 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮 氮Trimethylgallium and decane. As a result, on the surface of the wafer 35, an N-type contact layer 21 composed of a GaN layer doped with germanium is grown. After the formation of the N-type contact layer 21, the germanium material valve 56 is formed. Closing, the growth of the first multiple quantum well layer 22 is performed. The growth of the first multiple quantum well layer 22 is performed by interactively performing the following steps: by opening the nitrogen material valve 51, the gallium material valve 52, and the indium material a step 54 of supplying ammonia, trimethylgallium, and trimethylindium to the wafer 35 to grow the InGaN layer (quantum well layer); and closing the indium material valve 54, opening the nitrogen material valve 51 and the gallium material Valve 52, 127612.doc -18 - 200840095 Supply money and dimethyl gallium to wafer 35 for unadded GaN layer (P chapter wall

層)成長之步驟。例如首先形成GaN層,於其上形成inGaNLayer) steps to grow. For example, a GaN layer is first formed, and inGaN is formed thereon.

^歷、二5夂重複進行此之後,最後於InGaN層上形成GaN 最終障壁層25。於第一多重量子井層22及GaN最終障壁層 25之形成日守,晶圓35之溫度宜為例如7⑽⑽。◦(例如 730°〇 〇 接著,形成P型電子阻止層23。亦即,氮原料閥5丨、鎵 原料閥52、鋁原料閥53及鎂原料閥55打開,其他閥“,% 關閉。藉此,朝向晶圓35供給氨、三甲基鎵、三甲基鋁及 乙基壞戊二烯鎂,形成由摻雜鎂之AlGaN層所組成之P型 電子阻止層23。於此P型電子阻止層23之形成時,晶圓35 之溫度宜為800°C以上(例如1〇〇〇。〇)。 接著,形成P型接觸層24。亦即,氮原料閥5丨、鎵原料 閥52及鎂原料閥55打開’其他閥53、5[ %關閉。藉此, 朝向晶圓35供給氨、三甲基鎵及乙基環戊二烯鎂,形成由 掺雜鎂之GaN層所組成之p型接觸層24。於此p型接觸層以 之形成時,晶圓35之溫度宜為80(rc以上(例如1〇〇〇。〇。 然後,接著於P型接觸層24上,與第一多重量子井層22 之情況相同地形成第二多重量子井層26。於第一及第二多 重置子井層22、26之形成時,藉由調節銦原料氣體、鎵原 料氣體及氮原料氣體之流量比,來調節InGaN層之組成。 藉此來調節InGaN層之帶隙,其結果會控制第一及第二多 重量子井層22、26之各發光波長。 如此,若於晶圓35上使GaN半導體層2成長,將此晶圓 127612.doc -19· 200840095 35移至蝕刻裝置,藉由例如電漿蝕刻,如圖i所示形成用 以使N型接觸層21露出之凹部7、及使N型接觸層以露出之 凹部8。凹部7亦可形成如島狀地包圍第一多重量子井層 22、P型電子阻止層23及p型接觸層以,藉此將第一多重量 - 子井層22、P型電子阻止層23及?型接觸層24整形為台地形 • 亦可。同樣地,凹部8亦可形成如包圍第二多重量子井層 26,藉此將第二多重量子井層%整形為台地形亦可。 φ 並且,藉由電阻加熱或利用電子線射束之金屬蒸鍍裝 置,來形成陽極電極3、連接部4及陰極電極5。藉此,可 獲得圖1所示之發光二極體構造。 於此晶圓製程後,藉由劈開晶圓35來切出個別元件,此 個別元件藉由晶粒接合及金屬線接合而連接於引線電極 後,被密封於環氧樹脂等透明樹脂中。如此來製作氮化物 半導體發光元件。 如前述,第二多重量子井層26係於III族氮化物半導體疊 • 層構造’即於GaN半導體層2之構成層中最後形成。更具 體而έ,於形成以N型接觸層21及p型接觸層24夾住第一多 、 重置子井層22之發光二極體構造後,形成第二多重量子井 層26。因此,第二多重量子井層26不會經歷ρ型接觸層24 • 之形成時之溫度8〇〇。(:以上(例如100(rc)。進一步來說,第 一多重ϊ子井層26係於GaN半導體層2之構成層中,較其 形成溫度咼之所有層形成後再形成。因此,第二多重量子 井層26不會於其他層之形成時受到熱損傷。故,第二多重 夏子井層26儘管是發光波長較長之發光層,仍可具有良好 127612.doc -20- 200840095 之發光效率。另-方面,由於第一多重量子井層22為發光 波長短之發光層,因此可耐受P型接觸層24形成時之高 溫’因此依然具有良好之發光效率。 第-及第二多重量子井層22、26均是進行偏光發光之發 光層,其偏光方向亦相同。因此’藉由來自第一及第二多 重量子井層22、26之發光光線混合並被觀測,視覺上會觀 測到其等之混色之偏光光線。如此’可從氮化物半導體發 光元件取出發光色受到控制之偏光。 圖4係用以說明有關本發明之其他實施型態之氮化物半 導體發光元件之構造之圖解圖。於此圖4,與前述圖1所示 之各部相對應之部分係附上同一參考符號來表示。 於此實施型態’作為III族氮化物半導體疊層構造之GaN 半導體層2係於GaN基板1之一方主面(第一主面)側,具有 包含第一多重量子井層22之第一部分2A,於GaN基板 另一主面(第二主面)側,具有包含第二多重量子井層26之 第二部分2B。前述另一方主面(第二主面)為鏡面。 第一部分2A係從GaN基板1側,依序疊層n型接觸層21、 第一多重量子井層22、最終障壁層25、P型電子阻止層23 及P型接觸層24而構成。 於此實施型態,第二部分2B僅包含第二多重量子井層 26。第二多重量子井層26係對於N型接觸層21位在與第一 多重量子井層22相反侧,配置於以N型及P型接觸層21、24 夾住之第一多重量子井層22之發光二極體構造之外側。此 第二多重量子井層26側為光取出面。 127612.doc -21- 200840095 形成於P型接觸層24之表面之陽極電極3接合於支持基板 1 0上之布線11 (晶粒接合)。藉此,發光二極體構造係以與 圖1之情況反轉之姿勢固定於支持基板10。After repeating this, the GaN final barrier layer 25 is finally formed on the InGaN layer. The temperature of the wafer 35 is preferably, for example, 7 (10) (10), in the formation of the first multiple quantum well layer 22 and the GaN final barrier layer 25. ◦ (for example, 730 ° 〇〇, then, a P-type electron blocking layer 23 is formed. That is, the nitrogen raw material valve 5 丨, the gallium raw material valve 52, the aluminum raw material valve 53 and the magnesium raw material valve 55 are opened, and the other valves are "closed." Thus, ammonia, trimethylgallium, trimethylaluminum, and ethylpentadienyl magnesium are supplied toward the wafer 35 to form a P-type electron blocking layer 23 composed of a magnesium-doped AlGaN layer. When the formation of the stopper layer 23 is formed, the temperature of the wafer 35 is preferably 800 ° C or more (for example, 1 Å.) Next, the P-type contact layer 24 is formed. That is, the nitrogen raw material valve 5 丨, the gallium raw material valve 52 And the magnesium material valve 55 opens 'other valves 53, 5 [% closed. Thereby, ammonia, trimethylgallium and ethylcyclopentadienyl magnesium are supplied toward the wafer 35 to form a GaN layer doped with magnesium. The p-type contact layer 24. When the p-type contact layer is formed thereon, the temperature of the wafer 35 is preferably 80 (rc or more (for example, 1 Å. 〇. Then, next to the P-type contact layer 24, and The second multiple quantum well layer 26 is formed identically in the case of a multiple quantum well layer 22. By adjusting the indium during the formation of the first and second multiple reset subwell layers 22, The flow ratio of the source gas, the gallium source gas, and the nitrogen source gas adjusts the composition of the InGaN layer. Thereby, the band gap of the InGaN layer is adjusted, and as a result, the first and second multiple quantum well layers 22, 26 are controlled. Thus, if the GaN semiconductor layer 2 is grown on the wafer 35, the wafer 127612.doc -19·200840095 35 is moved to an etching apparatus, for example, by plasma etching, as shown in FIG. The concave portion 7 exposing the N-type contact layer 21 and the concave portion 8 exposing the N-type contact layer. The concave portion 7 may also form the first multiple quantum well layer 22, the P-type electron blocking layer 23, and the p. The contact layer is formed so that the first multi-weight sub-layer 22, the P-type electron blocking layer 23 and the ?-type contact layer 24 can be shaped into a topography. Similarly, the recess 8 can also be formed to surround the second Multiple quantum well layers 26, whereby the second multiple quantum well layer % can be shaped into a topography. φ Also, the anode electrode 3 is formed by resistance heating or a metal vapor deposition device using an electron beam beam. The connecting portion 4 and the cathode electrode 5. Thereby, the light emitting diode structure shown in Fig. 1 can be obtained. After the wafer process, individual wafers are cut by opening the wafer 35. The individual components are connected to the lead electrodes by die bonding and metal wire bonding, and then sealed in a transparent resin such as an epoxy resin. Thus, a nitride semiconductor light-emitting device is fabricated. As described above, the second multiple quantum well layer 26 is formed in the group III nitride semiconductor stacked layer structure, that is, finally formed in the constituent layers of the GaN semiconductor layer 2. More specifically, After the formation of the light-emitting diode structure in which the first plurality of reset sub-well layers 22 are sandwiched by the N-type contact layer 21 and the p-type contact layer 24, the second multiple quantum well layer 26 is formed. Therefore, the second multiple quantum well layer 26 does not experience a temperature of 8 时 when the p-type contact layer 24 is formed. (: above (for example, 100 (rc). Further, the first multiple dice well layer 26 is formed in the constituent layer of the GaN semiconductor layer 2, and is formed after all the layers forming the temperature 咼 are formed. Therefore, The two multiple quantum well layers 26 are not thermally damaged during the formation of other layers. Therefore, the second multiple Xiazi well layer 26, although it is a light-emitting layer with a longer wavelength of light, can still have good 127612.doc -20- 200840095 In other respects, since the first multiple quantum well layer 22 is a light-emitting layer having a short emission wavelength, it can withstand the high temperature at the time of formation of the P-type contact layer 24, and thus still has good luminous efficiency. The second multiple quantum well layers 22, 26 are all luminescent layers that emit polarized light, and their polarization directions are also the same. Therefore, the illuminating rays from the first and second multiple quantum well layers 22, 26 are mixed and observed. The polarized light of the mixed color is visually observed. Thus, the polarized light whose color is controlled can be taken out from the nitride semiconductor light-emitting element. FIG. 4 is a view for explaining the nitride semiconductor light emission according to another embodiment of the present invention. Component BRIEF DESCRIPTION OF THE DRAWINGS In Fig. 4, portions corresponding to the respective portions shown in Fig. 1 are denoted by the same reference numerals. This embodiment is a GaN semiconductor layer which is a group III nitride semiconductor stacked structure. 2 is a main surface (first main surface) side of the GaN substrate 1, and has a first portion 2A including the first multiple quantum well layer 22 on the other main surface (second main surface) side of the GaN substrate. The second portion 2B of the second multiple quantum well layer 26. The other main surface (second main surface) is a mirror surface. The first portion 2A is from the GaN substrate 1 side, sequentially laminating the n-type contact layer 21, first The multiple quantum well layer 22, the final barrier layer 25, the P-type electron blocking layer 23, and the P-type contact layer 24 are formed. In this embodiment, the second portion 2B includes only the second multiple quantum well layer 26. The multiple quantum well layer 26 is disposed on the opposite side of the first multiple quantum well layer 22 from the N-type contact layer 21, and is disposed on the first multiple quantum well layer sandwiched by the N-type and P-type contact layers 21, 24. The outer side of the light-emitting diode structure of 22. The second multiple quantum well layer 26 side is a light extraction surface. 127612.doc -21- 20 0840095 The anode electrode 3 formed on the surface of the P-type contact layer 24 is bonded to the wiring 11 (die bonding) on the support substrate 110. Thereby, the light-emitting diode structure is reversed in the same manner as in FIG. It is fixed to the support substrate 10.

GaN半導體層2之第一部分2A係被蝕刻(例如電漿蝕刻) 至從支持基板10側露出N型接觸層21,形成有凹部17。於 此凹部17,形成有相接於N型接觸層21之陰極電極5。此陰 極電極5與支持基板1〇上之布線12係由金屬柱18連接。 藉由此結構’於GaN半導體層2之第一部分2A,形成以N 型接觸層21及P型接觸層24夾住之第一多重量子井層22之 二極體構造。因此,若於陽極電極3與陰極電極5間施加順 向電壓,則第一多重量子井層22會由電流注入激發,產生 取決於其主面之結晶面之偏光。此光係穿透GaN基板1並 到達第二多重量子井層26,藉此將此第二多重量子井層26 予以光激發,產生取決於其主面之結晶面之偏光。 由於GaN基板1之兩主面均為c面以外之共同結晶面,因 此第一及第二多重量子井層22、26之偏光方向相等。因 此,於第二多重量子井層26側,觀測到第一及第二多重量 子井層22、26之發光色混色之偏光。 為了抑制於第一多重量子井層22產生之偏光光線被GaN 基板1吸收,GaN基板1宜具有比第一多重量子井層22寬之 帶隙。而且,基板1更宜對於第一多重量子井層22之發光 波長呈透明(宜為90%以上之光穿透率)。 製作此構造之氮化物半導體發光元件時,於GaN基板1 之一方主面側,使GaN半導體層2之第一部分2A進行磊晶 127612.doc -22- 200840095 成長後,於GaN基板1之另一方主面側,使構成第二部分 2B之第一夕重里子井層26進行蠢晶成長。因此,由於第二 夕重里子井層26較第一部分2A之發光二極體構造更晚形 成口此不會文到P型接觸層24等形成時之高溫所造成之 • 熱損傷。藉此,能以良好效率來發光。 • 以上說月有關本發明之實施型態,但本發明可進一步以 其他型態來實施。例如於前述實施型態說明有關於發光二 • ㉟體構造適用本中請發明之例,但本發明亦可適用於雷射 二極體等其他發光元件。 而且,於前述實施型態主要說明有關使用以瓜面作為主 面之GaN基板1之例,但亦可使用以a面作為主面之GaN* 板而且,亦可使用以(10-11)面、(10-13)面、(11-22)等該 類半極性面為主面之GaN基板。 而且,於前述例說明有關於GaN基板1上,使GaN半導體 層2再成長之例,但例如於以m面為主面之碳化矽基板上, • 冑以m面作為成長主面之GaN半導體成|,或於心面為主 面之孤貝石基板上,使以a面為主面之GaN半導體成長均 可。 並且,於W述實施形態說明有關藉由M〇CVD法,於 - GaN基板1上使GaN半導體進行磊晶成長之例,但亦可適用 H VPE法專其他蠢晶成長法。 而且,於前述實施型態說明有關具有第一及第二多重量 子井層(發光層)22、26之結構,但例如圖j及圖4所示,於 第二多重量子井層26疊層第三活性層27亦可。此第三活性 127612.doc -23- 200840095 層27係例如第一及第二多重量子井層22、%之任一均由發 光波長不同之III族氮化物半導體層(更具體而言為多重量 子井層)組成,其接受來自第一多重量子井層22之光之射 入,進行光激發而發光。藉此,3色偏光光線在視覺上混 口而被觀測。當然,進—步亦可疊層第四活性層或第五活 性層’進行4色以上混色之偏光發光。 詳細地說明有關本發明之實施型態,但此等僅是為了闡 明本發明之技術内容所利用之具體例,本發明不應限定於 此等具體例來解釋,本發明之精神及範圍僅由添附之申請 專利範圍來限定。 本申請案對應於2006年12月20日向日本專利廳提出之曰 本特願2006-343090號,該申請案之所有揭示係藉由於此 引用來組入。 【圖式簡單說明】 圖1係用以說明本發明之一實施型態之氮化物半導體發 光元件之構造之圖解剖面圖。 圖2係表示ΙΠ族氮化物半導體之結晶構造之單元胞之圖 解圖。 圖3係用以說明用以使構成GaN半導體層之各層成長之 處理裝置之結構之圖解圖。 圖4係用以說明有關本發明之其他實施型態之氮化物半 導體發光元件之構造之圖解剖面圖。 【主要元件符號說明】 1 GaN基板 127612.doc -24- 200840095 2 GaN半導體層 2A 第一部分 2B 第二部分 3 1%極電極 4 連接部 5 陰極 7, 8 凹部 10 支持基板 11,12 布線 13, 14 接合金屬線 17 凹部 18 金屬柱 21 N型接觸層 22 第一多重量子井層(第一活性層) 23 P型電子阻止層 • 24 P型接觸層 25 最終障壁層 26 第二多重量子井層(第二活性層) - 27 第三活性層 . 30 處理室 31 加熱器 32 基座 33 旋轉軸 34 旋轉驅動機構 127612.doc -25- 200840095The first portion 2A of the GaN semiconductor layer 2 is etched (for example, plasma etched) to expose the N-type contact layer 21 from the side of the support substrate 10, and the recess 17 is formed. In the recess 17, a cathode electrode 5 which is in contact with the N-type contact layer 21 is formed. The cathode electrode 5 and the wiring 12 on the support substrate 1 are connected by a metal post 18. By the structure of the first portion 2A of the GaN semiconductor layer 2, the diode structure of the first multiple quantum well layer 22 sandwiched by the N-type contact layer 21 and the P-type contact layer 24 is formed. Therefore, if a forward voltage is applied between the anode electrode 3 and the cathode electrode 5, the first multiple quantum well layer 22 is excited by current injection, resulting in polarization depending on the crystal plane of the principal surface. This light penetrates the GaN substrate 1 and reaches the second multiple quantum well layer 26, thereby photoexciting the second multiple quantum well layer 26 to produce a polarization depending on the crystal plane of the major surface. Since both main faces of the GaN substrate 1 are co-crystal faces other than the c-plane, the polarization directions of the first and second multiple quantum well layers 22, 26 are equal. Therefore, on the side of the second multiple quantum well layer 26, the polarization of the luminescent color mixing of the first and second multi-weight sub-well layers 22, 26 is observed. In order to suppress the polarized light generated by the first multiple quantum well layer 22 from being absorbed by the GaN substrate 1, the GaN substrate 1 preferably has a wider band gap than the first multiple quantum well layer 22. Further, the substrate 1 is preferably transparent to the light-emitting wavelength of the first multiple quantum well layer 22 (preferably having a light transmittance of 90% or more). When the nitride semiconductor light-emitting device having such a structure is produced, the first portion 2A of the GaN semiconductor layer 2 is grown on one of the main surface sides of the GaN substrate 1 by epitaxial growth 127612.doc-22-200840095, and then on the other side of the GaN substrate 1. On the main surface side, the first ridge layer 26 constituting the second portion 2B is subjected to stray crystal growth. Therefore, since the second radiant well layer 26 is formed later than the light-emitting diode structure of the first portion 2A, it does not cause thermal damage caused by the high temperature at the time of formation of the P-type contact layer 24 or the like. Thereby, it is possible to emit light with good efficiency. • The above description relates to the embodiment of the present invention, but the present invention can be further implemented in other forms. For example, in the above-described embodiment, an example in which the invention is applied to the light-emitting body structure is described. However, the present invention is also applicable to other light-emitting elements such as a laser diode. Further, in the above-described embodiment, an example in which the GaN substrate 1 having the melon surface as the main surface is used is mainly described, but a GaN* plate having the a-plane as the main surface may be used, and (10-11) plane may also be used. , such as (10-13) plane, (11-22) and the like, such a semi-polar surface is the main surface of the GaN substrate. Further, in the above-described example, an example is described in which the GaN semiconductor layer 2 is grown again on the GaN substrate 1. However, for example, on a tantalum carbide substrate having an m-plane as a main surface, and a GaN semiconductor having an m-plane as a growth main surface The GaN semiconductor having the a-plane as the main surface can be grown on the orphanite substrate on the main surface of the core surface. Further, an example in which the GaN semiconductor is epitaxially grown on the GaN substrate 1 by the M CVD method will be described in the above-described embodiment, but other stray crystal growth methods using the H VPE method may be applied. Moreover, in the foregoing embodiment, the structure having the first and second multiple quantum well layers (light emitting layers) 22, 26 is illustrated, but as shown in, for example, FIGS. j and 4, the second multiple quantum well layer 26 is stacked. The third active layer 27 may also be used. The third activity 127612.doc -23- 200840095 layer 27 is, for example, any of the first and second multiple quantum well layers 22, % of which are composed of a group III nitride semiconductor layer having a different emission wavelength (more specifically, multiple A quantum well layer consisting of receiving light from the first multiple quantum well layer 22 and performing photoexcitation to emit light. Thereby, the three-color polarized light is visually mixed and observed. Of course, the fourth active layer or the fifth active layer may be laminated in a stepwise manner to perform polarized light emission of a mixed color of four or more colors. The embodiments of the present invention are described in detail, but are merely intended to clarify the specific examples of the technical contents of the present invention. The present invention is not limited to the specific examples, and the spirit and scope of the present invention are only The scope of the patent application is limited. The present application is hereby incorporated by reference in its entirety to the entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire entire all BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a schematic cross-sectional view showing the structure of a nitride semiconductor light-emitting device according to an embodiment of the present invention. Fig. 2 is a view showing a unit cell of a crystal structure of a lanthanum nitride semiconductor. Fig. 3 is a schematic view for explaining the structure of a processing apparatus for growing the layers constituting the GaN semiconductor layer. Fig. 4 is a schematic cross-sectional view for explaining the configuration of a nitride semiconductor light-emitting element according to another embodiment of the present invention. [Major component symbol description] 1 GaN substrate 127612.doc -24- 200840095 2 GaN semiconductor layer 2A First portion 2B Second portion 3 1% pole electrode 4 Connection portion 5 Cathode 7, 8 Recessed portion 10 Support substrate 11, 12 wiring 13 , 14 bonding wire 17 recess 18 metal column 21 N-type contact layer 22 first multiple quantum well layer (first active layer) 23 P-type electron blocking layer • 24 P-type contact layer 25 final barrier layer 26 second multiple Quantum well layer (second active layer) - 27 third active layer. 30 processing chamber 31 heater 32 base 33 rotating shaft 34 rotary drive mechanism 127612.doc -25- 200840095

35 36 40 41 42 43 44 45 51 52 53 54 55 56 晶圓 排氣配管 原料氣體供給路 氮原料配管 鎵原料配管 鋁原料配管 錮原料配管 鎂原料配管 矽原料配管 氮原料閥 鎵原料閥 崔呂原料闊 銦原料閥 鎂原料閥 矽原料閥35 36 40 41 42 43 44 45 51 52 53 54 55 56 Wafer exhaust pipe raw material gas supply route nitrogen raw material piping gallium raw material piping aluminum raw material piping raw material piping magnesium raw material piping raw material piping nitrogen raw material valve gallium raw material valve Cui Lu raw material Wide indium raw material valve magnesium raw material valve 矽 raw material valve

1276I2.doc -26-1276I2.doc -26-

Claims (1)

200840095 十、申請專利範圍: 1 · 一種氮化物半導體發光元件,其係包含具有c面以外之 疊層主面之III族氮化物半導體疊層構造; 前述III族氮化物半導體疊層構造包含: 第一活性層,其係具有C面以外之特定結晶面之主 面,產生第一波長之光;及 第二活性層,其係具有前述特定結晶面之主面,產 生與前述第一波長不同之第二波長之光。 2.如請求項1之氮化物半導體發光元件,其中前述第一及 第二活性層係由 AlxIriyGa^yN (OSxgl,OSy^l, 〇Sx+y $ 1)組成。 3·如請求項1之氮化物半導體發光元件,其中前述ΠΙ族氮 化物半導體疊層構造進一步包含:Ν型氮化物半導體層 及Ρ型氮化物半導體層; 前述第一活性層係位於前述Ν型氮化物半導體層及ρ型 氮化物半導體層間; 前述第二活性層係位於前述Ν型氮化物半導體層及ρ型 氮化物半導體層間以外之場所。 4.如請求項3之氮化物半導體發光元件,其中前述第二活 性層係對於前述Ρ型氮化物半導體層位於與前述第一活 性層相反側。 5·如請求項3之氮化物半導體發光元件,其中前述第二活 性層係對於前述Ν型氮化物半導體層位於與前述第一活 性層相反側。 127612.doc 200840095 6.如請求項1之氮化物半導體發光元件,复击^ /、T進一步包含 基板’其係具有均為别述特定結晶面之繁 心弟—主面及第二 主面; 前述III族氮化物半導體疊層構造包含·给 弟一部分,其 • 係包含疊層於前述基板之第一主面之前述第一活性層·' 及第二部分,其係包含疊層於前述基板 - • 〜币一王面之前 述第二活性層。 籲 7·如凊求項6之氮化物半導體發光元件,其中前述第一主 面為鏡面。 8.如請求項6之氮化物半導體發光元件,其中前述基板具 有比前述第一活性層寬之帶隙。 9·如請求項6之氮化物半導體發光元件,其中前述基板係 對於前述第一活性層之發光波長呈透明。 10·如請求項1之氮化物半導體發光元件,其中前述第一活 性層係藉由電流注入而發光,前述第二活性層係藉由來 # 自前述第一活性層之光所造成之光激發而發光。 11·如請求項1之氮化物半導體發光元件,其中前述第一活 性層係包含帶隙比前述第二活性層大之ΠΙ族氮化物半導 ^ 體。 12·如請求項!至丨〗中任一項之氮化物半導體發光元件,其 中兩述特疋結晶面為無極性面或半極性面。 13· 一種氮化物半導體發光元件之製造方法,其中該氮化物 半導體發光元件係包含具有c面以外之疊層主面之III族 氮化物半導體疊層構造; 127612.doc 200840095 形成前述πι族氮化物半導體疊層構造之步驟包含以下 步驟: 形成具有c面以外之特定結晶面之主面,產生第一波 長之光之第一活性層之步驟;及 . 於前述111族氮化物半導體疊層構造之構成層中之形成 . 溫度比該第二活性層之形成溫度高之所有層形成後广形 成具有前述特定結晶面之主面且產生比前述第一波長長 之弟*一波長之光之弟二活性層之步驟。 14· 一種氮化物半導體發光元件之製造方法,其中該氮化物 半導體發光元件係包含具有c面以外之疊層主面之出族 氮化物半導體疊層構造; ' 形成鈾述III族氮化物半導體疊層構造之步驟包含以下 步驟: 形成弟一導電型之氮化物半導體層之步驟; 於前述第一導電型之氮化物半導體層上,形成具有e • 面以外之特定結晶面之主面,產生第一波長之光之第一 活性層之步驟; 於前述第一活性層上,形成第二導電型之氮化物半導 體層之步驟;及 ’ 於形成前述第一導電型之氮化物半導體層、前述第— 活性層及前述第二導電型之氮化物半導體層後,形成具 有前述特定結晶面之主面且產生比前述第一波長長之第 二波長之光之第二活性層之步驟。 15·如請求項13或14之氮化物半導體發光元件之製造方法, 127612.doc 200840095 前述III族氮化 形成該第二活 其中形成前述第 > 活性層之步驟係於形成 物半導體疊層構造之其他所有構成層後, 性層之步驟。 16·如請求項13或14之氮化物半導體發光元件之製造方法, 其中前述第二波長為500 nm以上。200840095 X. Patent Application Range: 1 . A nitride semiconductor light-emitting device comprising a group III nitride semiconductor stacked structure having a laminated main surface other than a c-plane; the III-nitride semiconductor stacked structure comprises: An active layer having a major surface of a specific crystal plane other than the C plane to generate light of a first wavelength; and a second active layer having a major surface of the specific crystal plane, which is different from the first wavelength Light of the second wavelength. 2. The nitride semiconductor light-emitting device of claim 1, wherein the first and second active layers are composed of AlxIriyGa^yN (OSxgl, OSy^l, 〇Sx+y$1). 3. The nitride semiconductor light-emitting device of claim 1, wherein the bismuth nitride semiconductor stacked structure further comprises: a bismuth nitride semiconductor layer and a bismuth nitride semiconductor layer; wherein the first active layer is located in the Ν type The second active layer is located between the nitride semiconductor layer and the p-type nitride semiconductor layer. 4. The nitride semiconductor light-emitting device of claim 3, wherein the second active layer is located on a side opposite to the first active layer to the germanium-type nitride semiconductor layer. The nitride semiconductor light-emitting device of claim 3, wherein the second active layer is located on a side opposite to the first active layer to the germanium-type nitride semiconductor layer. 127612.doc 200840095 6. The nitride semiconductor light-emitting device of claim 1, wherein the re-attack ^ /, T further comprises a substrate having a plurality of main faces and a second main surface which are specific crystal faces; The III-nitride semiconductor stacked structure includes a part of the first active layer ′′ and a second portion laminated on the first main surface of the substrate, and includes a layer stacked on the substrate - • The second active layer of the aforementioned coin. The nitride semiconductor light-emitting device of claim 6, wherein the first main surface is a mirror surface. 8. The nitride semiconductor light-emitting device of claim 6, wherein the substrate has a band gap wider than the first active layer. 9. The nitride semiconductor light-emitting device of claim 6, wherein the substrate is transparent to an emission wavelength of the first active layer. 10. The nitride semiconductor light-emitting device of claim 1, wherein the first active layer emits light by current injection, and the second active layer is excited by light caused by light from the first active layer. Glowing. The nitride semiconductor light-emitting device of claim 1, wherein the first active layer comprises a lanthanide nitride semiconductor having a larger band gap than the second active layer. 12·If requested! A nitride semiconductor light-emitting device according to any one of the preceding claims, wherein the two characteristic crystal faces are non-polar or semi-polar faces. 13. A method of fabricating a nitride semiconductor light-emitting device, wherein the nitride semiconductor light-emitting device comprises a group III nitride semiconductor stacked structure having a laminated main surface other than a c-plane; 127612.doc 200840095 forming the aforementioned πι nitride The step of constructing the semiconductor laminate structure comprises the steps of: forming a main surface having a specific crystal plane other than the c-plane, generating a first active layer of light of a first wavelength; and forming the layer 111 nitride semiconductor stacked structure Forming in the constituent layer. The temperature is higher than the formation temperature of the second active layer, and all the layers are formed to form a main surface having the specific crystal face and generating a light longer than the first wavelength. The step of the active layer. 14. A method of fabricating a nitride semiconductor light-emitting device, wherein the nitride semiconductor light-emitting device comprises a nitride nitride semiconductor stacked structure having a laminated main surface other than a c-plane; 'forming a uranium-group III nitride semiconductor stack The step of the layer structure includes the steps of: forming a nitride-type semiconductor layer of a conductivity type; forming a main surface having a specific crystal plane other than the e • surface on the nitride semiconductor layer of the first conductivity type a step of forming a first active layer of light of a wavelength; a step of forming a nitride semiconductor layer of a second conductivity type on the first active layer; and a step of forming a nitride semiconductor layer of the first conductivity type, the foregoing — a step of forming a second active layer having a principal surface of the specific crystal plane and generating light of a second wavelength longer than the first wavelength, after the active layer and the nitride semiconductor layer of the second conductivity type. 15. The method of manufacturing a nitride semiconductor light-emitting device according to claim 13 or 14, 127,612.doc 200840095, wherein the step of forming the second active portion to form the first active layer is performed on the formed semiconductor stacked structure After all other constituent layers, the steps of the sexual layer. The method of producing a nitride semiconductor light-emitting device according to claim 13 or 14, wherein the second wavelength is 500 nm or more. 127612.doc127612.doc
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