JP2007294985A - Light emitting device and manufacturing method thereof - Google Patents

Light emitting device and manufacturing method thereof Download PDF

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JP2007294985A
JP2007294985A JP2007159140A JP2007159140A JP2007294985A JP 2007294985 A JP2007294985 A JP 2007294985A JP 2007159140 A JP2007159140 A JP 2007159140A JP 2007159140 A JP2007159140 A JP 2007159140A JP 2007294985 A JP2007294985 A JP 2007294985A
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light emitting
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nitride semiconductor
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JP4958288B2 (en
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Hideki Hirayama
秀樹 平山
Katsushi Akita
勝史 秋田
Takao Nakamura
孝夫 中村
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Sumitomo Electric Industries Ltd
RIKEN Institute of Physical and Chemical Research
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RIKEN Institute of Physical and Chemical Research
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Abstract

<P>PROBLEM TO BE SOLVED: To provide a light emitting device using a nitride semiconductor for realizing a high power light emission with a high efficient light emission, and to provide a method of manufacturing the same. <P>SOLUTION: A GaN substrate 1 is formed, and a first conductive type Alx1Ga1-x1N layer (0≤x1≤1) is formed on the first main plane of the GaN substrate 1. A light emitting layer containing an InAlGaN quaternary mixed crystal is formed on the first conductive type Alx1Ga1-x1N layer. A second conductive type Alx2Ga1-x2N layer (0≤x2≤1) is formed on the light emitting layer. <P>COPYRIGHT: (C)2008,JPO&INPIT

Description

本発明は、発光素子およびその製造方法に関し、より具体的には紫外光を発する窒化物半導体を用いた発光素子およびその製造方法に関するものである。   The present invention relates to a light emitting device and a method for manufacturing the same, and more specifically to a light emitting device using a nitride semiconductor that emits ultraviolet light and a method for manufacturing the same.

GaN系化合物半導体はバンドギャップが大きいために、青色LED(Light Emitting Diode)や紫外光LEDとして機能し、白色LEDの励起光源に多く用いられている。これら波長の短い紫外光を発光するGaN系LEDは、その性能を向上させるために、たとえば下記の提案がなされてきた。
(d1)SiC基板を用い、InAlGaN層を発光層として、そのInAlGaN層におけるInなどの組成比を調整することにより波長360nm以下の紫外域での発光を高効率化する(特許文献1)。
(d2)GaN基板上に形成したAl0.1Ga0.9N層/Al0.4Ga0.6N層からなる単層量子井戸構造を発光層として高輝度化をはかる(非特許文献1)。
特開2001−237455号公報 T.Nishida, H.Saito, N.Kobayashi; Appl. Phys. Lett., Vol.79(2001) 711
Since GaN-based compound semiconductors have a large band gap, they function as blue LEDs (Light Emitting Diodes) and ultraviolet LEDs, and are often used as excitation light sources for white LEDs. In order to improve the performance of these GaN-based LEDs that emit ultraviolet light having a short wavelength, for example, the following proposals have been made.
(D1) Using an SiC substrate, using an InAlGaN layer as a light emitting layer, and adjusting the composition ratio of In or the like in the InAlGaN layer, light emission in the ultraviolet region with a wavelength of 360 nm or less is made highly efficient (Patent Document 1).
(D2) High luminance is achieved by using a single-layer quantum well structure composed of Al 0.1 Ga 0.9 N layer / Al 0.4 Ga 0.6 N layer formed on a GaN substrate as a light emitting layer (Non-patent Document 1).
JP 2001-237455 A T.Nishida, H.Saito, N.Kobayashi; Appl.Phys. Lett., Vol.79 (2001) 711

しかしながら上記の紫外発光素子は、発光効率が低く、また照明などに用いるために大電流を流すと発熱のために発光効率が低下してしまうという問題があった。上記の紫外発光素子の発光効率が低い理由として、基板や発光層などにおける転位密度が高いために、これら転位が非発光中心として働くことを挙げることができる。とくにサファイア基板を用いた場合、放熱性が悪く、発光効率が入力に比例してリニアに上がらずに途中で飽和する傾向が強い。   However, the above-described ultraviolet light emitting element has a problem in that the light emission efficiency is low and the light emission efficiency is lowered due to heat generation when a large current is passed for use in illumination or the like. The reason why the light emitting efficiency of the ultraviolet light emitting element is low is that the dislocation density in the substrate, the light emitting layer, etc. is high, so that these dislocations work as non-light emitting centers. In particular, when a sapphire substrate is used, the heat dissipation is poor, and the luminous efficiency tends to saturate in the middle without increasing linearly in proportion to the input.

本発明は、高効率発光および高出力発光を実現することができる発光素子およびその製造方法を提供することを目的とする。   An object of the present invention is to provide a light-emitting element capable of realizing high-efficiency light emission and high-output light emission, and a method for manufacturing the same.

本発明の発光素子は、窒化物半導体基板の第1の主表面の側に、InAlGaN4元混晶を含む発光層を備える。   The light emitting device of the present invention includes a light emitting layer containing an InAlGaN quaternary mixed crystal on the first main surface side of the nitride semiconductor substrate.

上記の構成によれば、低転位密度の窒化物半導体基板を用いることにより、発光素子内において非発光中心として作動する貫通転位密度を抑制し、発光効率を高めることができる。また、InAlGaN4元混晶に含まれるInによる組成変調効果により、発光効率をさらに高めることができる。なお、窒化物半導体基板は、第1導電型の導電性を有し、GaN基板、AlxGa1-xN基板(0<x≦1)、該AlxGa1-xN基板に含まれるAlN基板など、窒化物半導体であれば何でもよい。 According to the above configuration, by using the nitride semiconductor substrate having a low dislocation density, it is possible to suppress the threading dislocation density that operates as a non-luminescent center in the light emitting element, and to increase the light emission efficiency. Further, the luminous efficiency can be further increased by the composition modulation effect by In contained in the InAlGaN quaternary mixed crystal. The nitride semiconductor substrate has conductivity of the first conductivity type, and is included in the GaN substrate, the Al x Ga 1-x N substrate (0 <x ≦ 1), and the Al x Ga 1-x N substrate. Any nitride semiconductor such as an AlN substrate may be used.

本発明の別の発光素子は、第1導電型のAlx1Ga1-x1N層(0≦x1≦1)と、第1導電型のAlx1Ga1-x1N層の上に位置する第2導電型のAlx2Ga1-x2N層(0≦x2≦1)と、第1導電型のAlx1Ga1-x1N層および第2導電型のAlx2Ga1-x2N層の間に位置し、InAlGaN4元混晶を含む発光層とを有し、発光層から見て第1導電型のAlx1Ga1-x1N層より遠くに、厚みが100μm以下の、窒化物半導体層を備える。 Another light emitting device of the present invention includes a first conductivity type Al x1 Ga 1-x1 N layer (0 ≦ x1 ≦ 1) and a first conductivity type Al x1 Ga 1-x1 N layer. Between the two conductivity type Al x2 Ga 1-x2 N layer (0 ≦ x2 ≦ 1) and the first conductivity type Al x1 Ga 1-x1 N layer and the second conductivity type Al x2 Ga 1-x2 N layer And a light emitting layer containing an InAlGaN quaternary mixed crystal, and a nitride semiconductor layer having a thickness of 100 μm or less and far from the first conductivity type Al x1 Ga 1-x1 N layer as viewed from the light emitting layer Prepare.

上記の厚みが100μm以下の、窒化物半導体層は、前記本発明における窒化物半導体基板がエッチングまたは剥離されたものである。この構成により、非発光中心として作動する貫通転位密度を抑制し、またInAlGaN4元混晶に含まれるInによる組成変調効果を得たうえで、窒化物半導体基板による吸収を防止することができる。   The nitride semiconductor layer having a thickness of 100 μm or less is obtained by etching or peeling the nitride semiconductor substrate in the present invention. With this configuration, the threading dislocation density that operates as a non-luminescent center can be suppressed, and the composition modulation effect by In contained in the InAlGaN quaternary mixed crystal can be obtained, and absorption by the nitride semiconductor substrate can be prevented.

本発明の発光素子の製造方法は、窒化物半導体基板の第1の主表面の側に、第1導電型のAlx1Ga1-x1N層(0≦x1≦1)を形成する工程と、第1導電型のAlx1Ga1-x1N層の上にInAlGaN4元混晶を含んだ発光層を形成する工程と、発光層の上に第2導電型のAlx2Ga1-x2N層(0≦x2≦1)とを形成する工程と、第2導電型のAlx2Ga1-x2N層を形成した後に、窒化物半導体基板を除去する工程とを備える。 The method for manufacturing a light emitting device according to the present invention includes a step of forming a first conductivity type Al x1 Ga 1-x1 N layer (0 ≦ x1 ≦ 1) on the first main surface side of a nitride semiconductor substrate; Forming a light emitting layer containing an InAlGaN quaternary mixed crystal on the first conductivity type Al x1 Ga 1-x1 N layer; and a second conductivity type Al x2 Ga 1-x2 N layer on the light emission layer ( 0 ≦ x2 ≦ 1) and a step of removing the nitride semiconductor substrate after forming the second conductivity type Al x2 Ga 1-x2 N layer.

たとえばGaNは波長360nm以下の紫外光を吸収するので、上記の方法にしたがって、GaN基板を除去または剥離することによって光出力を向上させることができる。この結果、光出力をさらに大きく向上させることができる。また、他の窒化物半導体においても採り出したい波長域の光を吸収する場合があり、そのような場合には、その窒化物半導体基板を除去することにより光出力を向上させることができる。   For example, since GaN absorbs ultraviolet light having a wavelength of 360 nm or less, the light output can be improved by removing or peeling the GaN substrate according to the above method. As a result, the light output can be further improved. Also, other nitride semiconductors may absorb light in a wavelength range desired to be extracted. In such a case, the light output can be improved by removing the nitride semiconductor substrate.

なお、A層の上にB層が位置するとは、窒化物半導体基板から見てA層よりも遠い位置にB層が位置することをさし、B層はA層に接していてもよいし、接していなくてもよい。   The B layer being positioned on the A layer means that the B layer is positioned farther from the A layer as viewed from the nitride semiconductor substrate, and the B layer may be in contact with the A layer. , You do not have to touch.

次に本発明の実施例について説明する。
(実施例1)
図1は、本発明の実施例1のLEDを示す図である。図1において、GaN基板1の上に、(n型GaN層2/n型AlxGa1-xN層3/InAlGaN発光層4/p型AlxGa1-xN層5/p型GaN層6)の積層構造が形成されている。GaN基板1の第2の主平面である裏面にはn電極11が、また、p型GaN層6の上にはp電極12が配置されている。これら対のn電極11とp電極12とに電流を印加することにより、InAlGaN発光層から紫外光が発光される。InAlGaN発光層は、InxaAlyaGa1-xa-yaNの組成を有する。
Next, examples of the present invention will be described.
Example 1
FIG. 1 is a diagram showing an LED according to Example 1 of the present invention. In FIG. 1, on a GaN substrate 1, (n-type GaN layer 2 / n-type Al x Ga 1-x N layer 3 / InAlGaN light emitting layer 4 / p-type Al x Ga 1-x N layer 5 / p-type GaN A layered structure of layer 6) is formed. An n-electrode 11 is disposed on the back surface, which is the second main plane of the GaN substrate 1, and a p-electrode 12 is disposed on the p-type GaN layer 6. By applying a current to the pair of n electrode 11 and p electrode 12, ultraviolet light is emitted from the InAlGaN light emitting layer. InAlGaN emitting layer has a composition of In xa Al ya Ga 1-xa -ya N.

図1に示すGaN系LEDは、次の処理工程により製造される。厚み400μm、転位密度5E6cm-2、比抵抗1E−2ΩcmのGaN基板をMOCVD(有機金属気相成長法:Metal Organic Chemical Vapor Deposition)成膜装置内のサセプタ上に配置し、成膜装置内を減圧に保ち、下記のMOCVD法により積層構造を形成し、紫外発光ダイオードを作製した。 The GaN LED shown in FIG. 1 is manufactured by the following processing steps. A GaN substrate having a thickness of 400 μm, a dislocation density of 5E6 cm −2 , and a specific resistance of 1E-2 Ωcm is placed on a susceptor in a MOCVD (Metal Organic Chemical Vapor Deposition) film forming apparatus, and the pressure in the film forming apparatus is reduced. Then, a laminated structure was formed by the following MOCVD method to produce an ultraviolet light emitting diode.

MOCVDの原料にはトリメチルガリウム、トリメチルアルミニウム、トリメチルインジウムアダクト、アンモニア、テトラエチルシラン、ビスエチルシクロペンタジニチルマグネシウムを用いた。まず、成長温度1050℃で、GaN基板1の上に厚さ0.1μmのn型GaN層2を下地層として形成し、次いでその上に厚さ0.2μmのn型Al0.18Ga0.82N層3を成膜した。 As raw materials for MOCVD, trimethylgallium, trimethylaluminum, trimethylindium adduct, ammonia, tetraethylsilane, and bisethylcyclopentadinylmagnesium were used. First, an n-type GaN layer 2 having a thickness of 0.1 μm is formed on the GaN substrate 1 as a base layer at a growth temperature of 1050 ° C., and then an n-type Al 0.18 Ga 0.82 N layer having a thickness of 0.2 μm is formed thereon. 3 was deposited.

その後、成長温度を830℃に降下し、60nmのInAlGaN発光層4を成長した。このときの原料ガスの流量はアンモニアが2l/min、トリメチルガリウム3μmol/min、トリメチルアルミニウム0.5μmol/min、トリメチルインジウムアダクト60μmol/min、であった。その後、再び成長温度を1050℃に上昇し、厚さ0.2μmのp型Al0.18Ga0.82N層5を形成した。さらに、この上に厚さ30nmのp型GaN層をコンタクト層として成長した。 Thereafter, the growth temperature was lowered to 830 ° C., and a 60 nm InAlGaN light emitting layer 4 was grown. The flow rate of the raw material gas at this time was 2 l / min for ammonia, 3 μmol / min trimethylgallium, 0.5 μmol / min trimethylaluminum, and 60 μmol / min trimethylindium adduct. Thereafter, the growth temperature was raised again to 1050 ° C., and a p-type Al 0.18 Ga 0.82 N layer 5 having a thickness of 0.2 μm was formed. Further, a p-type GaN layer having a thickness of 30 nm was grown thereon as a contact layer.

こうして成長したLEDエピタキシャル構造に、適当な金属材料によりp型GaN層6上に半透明のp電極12、GaN基板の第2面の主平面でエピタキシャル層とは反対側の面(裏面)にn電極11を形成した。こうして作製した紫外発光ダイオードは図1に示す構造を取る。   The LED epitaxial structure grown in this manner is made of an appropriate metal material, a translucent p-electrode 12 on the p-type GaN layer 6, and n on the surface opposite to the epitaxial layer (back surface) of the second surface of the GaN substrate. An electrode 11 was formed. The ultraviolet light emitting diode thus fabricated has the structure shown in FIG.

上記の紫外発光ダイオードに連続電流印加を行なったところ、図2に示すように、波長360nmのInAlGaN発光層のバンド端発光が得られた。印加電流値を300mAまで上げても、図3に示すように、光出力は飽和することなく線形に増加した。このことからGaN基板上の高い放熱性が実証された。また、本実施例では、GaN基板に転位密度が低い基板を用いたために、貫通転位密度が低下し、発光効率を高めることができた。   When continuous current was applied to the ultraviolet light emitting diode, band edge emission of an InAlGaN light emitting layer having a wavelength of 360 nm was obtained as shown in FIG. Even when the applied current value was increased to 300 mA, the light output increased linearly without saturation as shown in FIG. This demonstrated high heat dissipation on the GaN substrate. Further, in this example, since a substrate having a low dislocation density was used as the GaN substrate, the threading dislocation density was reduced, and the luminous efficiency could be increased.

(実施例2)
図4は、本発明の実施例2の紫外発光ダイオードを示す図である。この紫外発光ダイオードは、図1に示す紫外LEDの積層構造と比べて、発光層4と接してGaN基板1に近い側に緩衝層のInxAlyGa1-x-yN層17を配置した点に特徴がある。また、発光層も多重量子井戸構造としているが、発光層についてはこの後に説明する。
(Example 2)
FIG. 4 is a diagram showing an ultraviolet light-emitting diode according to Example 2 of the present invention. This ultraviolet light emitting diode has a buffer layer In x Al y Ga 1 -xy N layer 17 disposed on the side close to the GaN substrate 1 in contact with the light emitting layer 4 as compared with the laminated structure of the ultraviolet LED shown in FIG. There is a feature. The light emitting layer also has a multiple quantum well structure. The light emitting layer will be described later.

本実施例の紫外LEDの製造方法は次のとおりである。GaN基板1としては、厚み400μm、貫通転位密度5E6/cm2の基板を用いた。実施例1と同様の方法により、GaN基板1の上にn型GaN層2およびn型AlxGa1-xN層3を順に形成した。次いで、n型AlxGa1-xN層3に接して、成長温度830℃で厚み50nmのInxAlyGa1-x-yN緩衝層17を成長させる。 The manufacturing method of the ultraviolet LED of this example is as follows. As the GaN substrate 1, a substrate having a thickness of 400 μm and a threading dislocation density of 5E6 / cm 2 was used. An n-type GaN layer 2 and an n-type Al x Ga 1-x N layer 3 were formed in this order on the GaN substrate 1 by the same method as in Example 1. Next, an In x Al y Ga 1-xy N buffer layer 17 having a thickness of 50 nm is grown at a growth temperature of 830 ° C. in contact with the n-type Al x Ga 1-x N layer 3.

その後、そのInxAlyGa1-x-yN緩衝層17の上に、図5に示すように(Inx5Aly5Ga1-x5-y5N障壁層4a/Inx4Aly4Ga1-x4-y4N井戸層4b)の2層構造を3周期積層しての多重量子井戸構造を形成した。実施例2では、この多重量子井戸構造が発光層4を構成する。 Then, on top of the In x Al y Ga 1-xy N buffer layer 17, as shown in FIG. 5 (In x5 Al y5 Ga 1 -x5-y5 N barrier layer 4a / In x4 Al y4 Ga 1 -x4- A multi-quantum well structure was formed by laminating two layers of y4 N well layer 4b) in three cycles. In Example 2, the multiple quantum well structure constitutes the light emitting layer 4.

InxAlyGa1-x-yN緩衝層を成長させるとき、およびInx4Aly4Ga1-x4-y4N障壁層を成長させるときの原料ガスの流量は、アンモニアが2l/min、トリメチルガリウム1.5μmol/min、トリメチルアルミニウム0.65μmol/min、トリメチルインジウムアダクト30μmol/min、とした。 In x Al y Ga 1-xy N when growing the buffer layer, and the In x4 Al y4 Ga 1-x4 -y4 flow rate of the source gas when growing the N barrier layer, ammonia 2l / min, trimethyl gallium 1 0.5 μmol / min, trimethylaluminum 0.65 μmol / min, and trimethylindium adduct 30 μmol / min.

Inx4Aly4Ga1-x4-y4N井戸層を成長させるときの原料ガスの流量は、アンモニアが2l/min、トリメチルガリウム1.5μmol/min、トリメチルアルミニウム0.52μmol/min、トリメチルインジウムアダクト53μmol/min、であった。 The flow rate of the source gas when growing the In x4 Al y4 Ga 1-x4-y4 N well layer is as follows: ammonia is 2 l / min, trimethylgallium 1.5 μmol / min, trimethylaluminum 0.52 μmol / min, trimethylindium adduct 53 μmol / Min.

本実施例では、緩衝層のInxAlyGa1-x-yN層を配置したこと、および発光層を、InAlGaN層の多重量子井戸構造にしたこと、の2点で、実施例1と相違する。 The present embodiment is different from the first embodiment in that the buffer layer In x Al y Ga 1-xy N layer is disposed and the light emitting layer has a multiple quantum well structure of an InAlGaN layer. .

上記の2点の改良により、図6に示すように、発光出力は飛躍的に向上した。たとえば、図3では100mAの印加電流に対する光出力は0.01mW程度であったが、図6では100mAの印加電流に対する光出力は1.7mWと150倍強の大幅な向上が得られた。また、図7に示すように、発光スペクトルの半値幅は12nmと小さくなった。これは発光層を多重量子井戸としたことによって量子準位間での発光が支配的となるためである。   As a result of the above two improvements, the light emission output has been dramatically improved as shown in FIG. For example, in FIG. 3, the optical output with respect to the applied current of 100 mA was about 0.01 mW, but in FIG. 6, the optical output with respect to the applied current of 100 mA was 1.7 mW, which is a significant improvement of 150 times. Moreover, as shown in FIG. 7, the half width of the emission spectrum was as small as 12 nm. This is because light emission between the quantum levels becomes dominant because the light emitting layer is a multiple quantum well.

(実施例3)
本発明の実施例3では、GaN基板上に形成した紫外LED(本発明例)と、GaNテンプレート(サファイア基板上に低温成長GaNバッファ層を介してn型GaNを3μm成長した基板)上に形成した紫外LED(比較例)との光出力の比較を行なった。GaNテンプレートは予め作製したものを用いた。上記本発明例および比較例ともに、図4および図5に示す積層構造を形成した。ただし、GaNテンプレートは裏面側は絶縁体なので、n電極は予め露出させたn型GaN層上に形成した。
(Example 3)
In Example 3 of the present invention, an ultraviolet LED formed on a GaN substrate (example of the present invention) and a GaN template (a substrate obtained by growing 3 μm of n-type GaN on a sapphire substrate through a low-temperature grown GaN buffer layer). The light output was compared with the ultraviolet LED (comparative example). A GaN template prepared in advance was used. The laminated structure shown in FIG. 4 and FIG. 5 was formed in both the above inventive examples and comparative examples. However, since the back side of the GaN template is an insulator, the n-electrode was formed on the n-type GaN layer exposed in advance.

まず、製造にあたり、GaN基板およびGaNテンプレートの両方をともにMOCVD成膜装置内のサセプタ上に配置した。次いで、GaN基板と、GaNテンプレートとにn型GaN層、n型Alx1Ga1-x1N層および緩衝層のInxAlyGa1-x-yN層を成膜した。この後、実施例2と同様に、(Inx4Aly4Ga1-x4-y4N障壁層/Inx3Aly3Ga1-x3-y3N井戸層)の2層構造を3周期積層して、多重量子井戸構造を作製した。この後、p型Alx2Ga1-x2N層/p型GaN層を形成し、p電極およびn電極を形成した。上記の成膜処理を通じて、成長温度、原料ガスの流量は実施例2と同じに揃えた。ただし、GaNテンプレートへのn電極は上述したように、n型GaN層上に形成する。 First, in manufacturing, both the GaN substrate and the GaN template were placed on the susceptor in the MOCVD film forming apparatus. Then, a GaN substrate, n-type GaN layer on the GaN template was formed In x Al y Ga 1-xy N layer of n-type Al x1 Ga 1-x1 N layer and a buffer layer. Thereafter, as in Example 2, a two-layer structure of (In x4 Al y4 Ga 1-x4-y4 N barrier layer / In x3 Al y3 Ga 1-x3-y3 N well layer) was laminated in three cycles, A multiple quantum well structure was fabricated. Thereafter, a p-type Al x2 Ga 1-x2 N layer / p-type GaN layer was formed, and a p-electrode and an n-electrode were formed. Through the film formation process described above, the growth temperature and the flow rate of the source gas were made the same as in Example 2. However, the n-electrode to the GaN template is formed on the n-type GaN layer as described above.

上記のようにして作製した本発明例および比較例の両方に、電流を印加して光出力を測定した。結果を比較できるようにして、図8に示す。図8では、GaNテンプレートを用いた比較例は、実際の光出力の5倍の値が表示されている。   A current was applied to both the inventive example and the comparative example produced as described above, and the light output was measured. The results are shown in FIG. In FIG. 8, the comparative example using the GaN template displays a value five times the actual light output.

図8によれば、電流50mAでGaN基板上のLEDでGaNテンプレート上の約10倍の出力が得られている。またGaNテンプレートを用いたLEDでは電流100mAで出力が飽和傾向を示すのに対し、GaN基板上では出力が線形に増加した。よって低転位GaN基板はInAlGaN発光層を用いた紫外LEDの高効率化、高電流注入によるLEDの高出力化に有効である。本発明例のLEDでは、熱伝導の良好なGaN基板を用いているため発熱による高温化が抑制されること、および貫通転位密度が低いために非発光中心が抑制されること、の2点により上記の高出力が得られた。   According to FIG. 8, about 10 times the output on the GaN template is obtained with the LED on the GaN substrate at a current of 50 mA. In the LED using the GaN template, the output tends to be saturated at a current of 100 mA, whereas the output increased linearly on the GaN substrate. Therefore, the low dislocation GaN substrate is effective for increasing the efficiency of the ultraviolet LED using the InAlGaN light emitting layer and increasing the output of the LED by high current injection. In the LED of the present invention, a GaN substrate with good thermal conductivity is used, so that the high temperature due to heat generation is suppressed, and the non-luminescent center is suppressed because the threading dislocation density is low. The above high output was obtained.

(実施例4)
図9は、本発明の実施例4における発光素子の積層構造を示す図である。まず、製造方法について説明する。AlxGa1-xN基板(x=0.18)をサセプタ上に配置し、有機金属気相成長法の成膜装置内を減圧に保ちながら積層構造を作製し、紫外発光ダイオード構造を得た。原料には、トリメチルガリウム、トリメチルアルミニウム、トリメチルインジウムアダクト、アンモニア、テトラエチルシラン、ビスエチルシクロペンタジエニルマグネシウムを用いた。まず、成長温度1050℃で、厚さ0.5μmのn型Al0.18Ga0.82Nバッファ層22を成長させた。
Example 4
FIG. 9 is a view showing a laminated structure of light emitting elements in Example 4 of the present invention. First, the manufacturing method will be described. An Al x Ga 1-x N substrate (x = 0.18) is placed on the susceptor, and a laminated structure is produced while keeping the inside of the metal organic vapor phase deposition apparatus under reduced pressure, thereby obtaining an ultraviolet light emitting diode structure. It was. As raw materials, trimethylgallium, trimethylaluminum, trimethylindium adduct, ammonia, tetraethylsilane, and bisethylcyclopentadienylmagnesium were used. First, an n-type Al 0.18 Ga 0.82 N buffer layer 22 having a thickness of 0.5 μm was grown at a growth temperature of 1050 ° C.

その後、成長温度を830℃に降下させ、上述の実施例2と同様に、InAlGaN障壁層24aおよびInAlGaN井戸層24bを3周期有する多重量子井戸構造の発光層24を形成した。その後、再び成長温度を1050℃に上昇させ、厚さ20nmのp型Al0.30Ga0.70N層25および厚さ50nmのp型Al0.18Ga0.82N層26を成長した。 Thereafter, the growth temperature was lowered to 830 ° C., and the light emitting layer 24 having a multiple quantum well structure having three cycles of the InAlGaN barrier layer 24a and the InAlGaN well layer 24b was formed in the same manner as in Example 2 described above. Thereafter, the growth temperature was raised again to 1050 ° C., and a p-type Al 0.30 Ga 0.70 N layer 25 having a thickness of 20 nm and a p-type Al 0.18 Ga 0.82 N layer 26 having a thickness of 50 nm were grown.

上記のように形成したLEDエピタキシャル構造のp型AlGaN層26の上に、金属材料により半透明p電極12を形成し、またAlGaN基板21の裏面側にn電極11を形成した。   On the p-type AlGaN layer 26 having the LED epitaxial structure formed as described above, a semitransparent p-electrode 12 was formed from a metal material, and an n-electrode 11 was formed on the back side of the AlGaN substrate 21.

上記のように形成した紫外発光ダイオードに連続電流を印加したところ、波長351nmのInAlGaNのバンド端発光を得ることができた。このバンド端発光の光出力として電流100mAのとき8mWを得ることができた。   When a continuous current was applied to the ultraviolet light emitting diode formed as described above, InAlGaN band edge emission with a wavelength of 351 nm could be obtained. As the optical output of the band edge emission, 8 mW was obtained when the current was 100 mA.

以上本発明の実施例について説明したが、上記の実施例も含めて本発明の実施の形態について羅列的に説明する。   Although the embodiments of the present invention have been described above, the embodiments of the present invention including the above embodiments will be described enumerated.

上記の窒化物半導体基板をGaN基板とすることができる。GaN基板は大型で安価なものが入手可能なため、量産に適している。   The nitride semiconductor substrate can be a GaN substrate. GaN substrates are suitable for mass production because they are large and inexpensive.

また上記の窒化物半導体基板をAlxGa1-xN基板(0<x≦1)としてもよい。AlxGa1-xN基板を用いることによりInAlGaN発光層の結晶性を高めることができる。すなわち、発光層と窒化物半導体基板との結晶格子の違いを小さくすることができ、発光層に生じる格子不整を抑制することができる。 The nitride semiconductor substrate may be an Al x Ga 1-x N substrate (0 <x ≦ 1). The crystallinity of the InAlGaN light emitting layer can be enhanced by using an Al x Ga 1-x N substrate. That is, the difference in crystal lattice between the light emitting layer and the nitride semiconductor substrate can be reduced, and the lattice irregularity generated in the light emitting layer can be suppressed.

上記のAlxGa1-xN基板(0<x≦1)のバンドギャップエネルギーを、InAlGaN4元混晶を含む発光層が発する光の波長に対応するエネルギー以下とすることができる。このような窒化物半導体基板のバンドギャップとすることにより、発光層から発した光が窒化物半導体基板に吸収されず、有効に利用することができる。 The band gap energy of the Al x Ga 1-x N substrate (0 <x ≦ 1) can be set to be equal to or lower than the energy corresponding to the wavelength of light emitted from the light emitting layer containing the InAlGaN quaternary mixed crystal. By setting the band gap of such a nitride semiconductor substrate, light emitted from the light emitting layer is not absorbed by the nitride semiconductor substrate and can be used effectively.

上記の窒化物半導体基板の第1の主表面の側に、第1導電型のAlx1Ga1-x1N層(0≦x1≦1)と、窒化物半導体基板から見て第1導電型のAlx1Ga1-x1N層より遠くに位置する第2導電型のAlx2Ga1-x2N層(0≦x2≦1)とを備え、第1導電型のAlx1Ga1-x1N層および第2導電型のAlx2Ga1-x2N層の間に、上記のInAlGaN4元混晶を含む構成としてもよい。 A first conductivity type Al x1 Ga 1-x1 N layer (0 ≦ x1 ≦ 1) and a first conductivity type as viewed from the nitride semiconductor substrate are formed on the first main surface side of the nitride semiconductor substrate. A second conductivity type Al x2 Ga 1-x2 N layer (0 ≦ x2 ≦ 1) located farther than the Al x1 Ga 1-x1 N layer, and the first conductivity type Al x1 Ga 1-x1 N layer The above-described InAlGaN quaternary mixed crystal may be included between the second conductivity type Al x2 Ga 1 -x2 N layer.

上記の構成により、p導電型層とn導電型層とから、その間に挟むInAlGaN4元混晶に電流を注入することにより、高い効率の発光を得ることができる。   With the above configuration, high-efficiency light emission can be obtained by injecting current from the p-conductivity type layer and the n-conductivity type layer into the InAlGaN quaternary mixed crystal sandwiched therebetween.

上記の発光素子は、発光層における発光により波長330nm〜370nmの範囲の光を発することができる。   The light emitting element can emit light having a wavelength in the range of 330 nm to 370 nm by light emission in the light emitting layer.

上記範囲の波長が放射されるように発光層を調整することにより、発光効率の優れた紫外線域の発光素子を得ることができる。   By adjusting the light emitting layer so that a wavelength in the above range is emitted, a light emitting element in the ultraviolet region with excellent light emission efficiency can be obtained.

上記の窒化物半導体基板の貫通転位密度は1E7cm-2以下とするのがよい。
この構成により、本発明の発光素子中の貫通転位密度を減らすことができ、非発光中心密度を低減することができる。
The threading dislocation density of the nitride semiconductor substrate is preferably 1E7 cm −2 or less.
With this configuration, the threading dislocation density in the light emitting element of the present invention can be reduced, and the non-light emitting center density can be reduced.

また、上記の窒化物半導体基板と第1導電型のAlx1Ga1-x1N層との間に、第1導電型の窒化物半導体基板と同種の窒化物半導体層を有する構成にしてもよい。 Further, the same type of nitride semiconductor layer as that of the first conductive type nitride semiconductor substrate may be provided between the nitride semiconductor substrate and the first conductive type Al x1 Ga 1-x1 N layer. .

この構成によれば、窒化物半導体基板に接して第1導電型のAlx1Ga1-x1N層を形成する構造よりも、上記の第1導電型の窒化物半導体基板と同種の窒化物半導体層を緩衝層として機能させることにより第1導電型のAlx1Ga1-x1N層の結晶性を高めることができる。 According to this configuration, the same type of nitride semiconductor as that of the first conductivity type nitride semiconductor substrate is formed, rather than the structure in which the first conductivity type Al x1 Ga 1-x1 N layer is formed in contact with the nitride semiconductor substrate. By making the layer function as a buffer layer, the crystallinity of the first conductivity type Al x1 Ga 1 -x1 N layer can be enhanced.

上記の第2導電型のAlx2Ga1-x2N層の上に、厚み1nm〜500nmの第2導電型のAlx3Ga1-x3N層(0≦x3<1、x3<x2)を有する構成にしてもよい。 On the second conductivity type Al x2 Ga 1-x2 N layer of the above, with Al x3 Ga 1-x3 N layer of the second conductivity type having a thickness 1nm~500nm a (0 ≦ x3 <1, x3 <x2) It may be configured.

上記の構成によれば、第2導電型のAlx2Ga1-x2N層に接して電極を形成するよりも接触抵抗を低くでき、電力−光変換効率を高めることができる。第2導電型のAlx3Ga1-x3N層は、厚み1nm未満では接触抵抗を低下できるほど良好な層を得ることができず、また厚みが500nmを超えると波長360nm以下の紫外光の吸収量が増える。このため、第2導電型のAlx3Ga1-x3N層の厚みは1nm〜500nmの範囲とする。 According to said structure, contact resistance can be made lower than forming an electrode in contact with the 2nd conductivity type Alx2Ga1 -x2N layer, and power-light conversion efficiency can be improved. When the thickness of the second conductivity type Al x3 Ga 1-x3 N layer is less than 1 nm, it is difficult to obtain a layer that can reduce the contact resistance. When the thickness exceeds 500 nm, absorption of ultraviolet light having a wavelength of 360 nm or less is not possible. The amount increases. For this reason, the thickness of the second conductivity type Al x3 Ga 1-x3 N layer is in the range of 1 nm to 500 nm.

上記の第1の主表面とは反対側の第2の主表面に第1の電極が、また第2導電型のAlx2Ga1-x2N層の上に第1の電極と対をなす第2の電極が形成される構成をとることができる。 The first electrode is paired with the first electrode on the second main surface opposite to the first main surface and on the second conductivity type Al x2 Ga 1-x2 N layer. A configuration in which two electrodes are formed can be employed.

上記の構成によれば、窒化物半導体基板の第2の主表面である裏面に第1の電極を配置することができるので、直列抵抗を小さくすることができる。このため、電圧効率を向上させ、発熱を小さくできるので、発光効率を高めることができる。さらに、窒化物半導体は熱伝導率が良好なので発熱の影響を受けにくいことも良い方向に作用する。   According to said structure, since a 1st electrode can be arrange | positioned at the back surface which is the 2nd main surface of a nitride semiconductor substrate, series resistance can be made small. For this reason, voltage efficiency can be improved and heat generation can be reduced, so that luminous efficiency can be increased. Further, since nitride semiconductors have good thermal conductivity, they are less likely to be affected by heat generation.

上記の発光層が、Inx4Aly4Ga1-x4-y4N(0<x4<0.2、0<y4<0.5)で表される井戸層と、Inx5Aly5Ga1-x5-y5N(0≦x5<0.2、0<y5<0.5)で表される障壁層とを含む量子井戸構造を有する構成をとってもよい。 The light-emitting layer includes a well layer represented by In x4 Al y4 Ga 1-x4-y4 N (0 <x4 <0.2, 0 <y4 <0.5), In x5 Al y5 Ga 1-x5 A structure having a quantum well structure including a barrier layer represented by −y5 N (0 ≦ x5 <0.2, 0 <y5 <0.5) may be employed.

上記のように、発光層を量子井戸構造にすることにより発光効率を大幅に向上させることができる。そして、井戸層および障壁層ともにInAlGaNの結晶を用いることにより、歪みを小さくでき、発光効率を高めることができる。   As described above, the light emission efficiency can be greatly improved by making the light emitting layer have a quantum well structure. By using InAlGaN crystals for both the well layer and the barrier layer, the strain can be reduced and the light emission efficiency can be increased.

上記の発光層と窒化物半導体基板との間に、厚み10nm〜200nmのInxAlyGa1-x-yN(0<x<0.2、0<y<0.5)層を有する構成をとってもよい。 Between the light-emitting layer and the nitride semiconductor substrate, a structure having a In x Al y Ga 1-xy N (0 <x <0.2,0 <y <0.5) layer having a thickness of 10nm~200nm It may be taken.

上記の構成により、発光層にかかる歪みを小さくすることができ、ピエゾ効果による電子と正孔の空間的分離を防止し、発光効率を向上させることができる。   With the above structure, distortion applied to the light-emitting layer can be reduced, spatial separation of electrons and holes due to the piezoelectric effect can be prevented, and light emission efficiency can be improved.

上記の第1導電型のAlx1Ga1-x1N層(0≦x1≦1)と、第2導電型のAlx2Ga1-x2N層(0≦x2≦1)層との厚みの合計が0.4μm以下であるようにしてもよい。 Total thickness of the first conductivity type Al x1 Ga 1-x1 N layer (0 ≦ x1 ≦ 1) and the second conductivity type Al x2 Ga 1-x2 N layer (0 ≦ x2 ≦ 1) May be 0.4 μm or less.

第1導電型Alx1Ga1-x1N層および第2導電型Alx2Ga1-x2N層の厚みの合計が0.4μmを超えるとクラックが発生し、これらの層の一部に対応する部分でしか発光しなくなるので、上記厚み合計を0.4μm以下とするのがよい。 When the total thickness of the first conductivity type Al x1 Ga 1-x1 N layer and the second conductivity type Al x2 Ga 1-x2 N layer exceeds 0.4 μm, a crack is generated and corresponds to a part of these layers. Since the light is emitted only at the portion, the total thickness is preferably 0.4 μm or less.

上記別の本発明の発光素子では、窒化物半導体基板がエッチングまたは剥離されて発光層から見て第1導電型のAlx1Ga1-x1N層より遠くに、窒化物半導体層を有しないようにしてもよい。 In another light emitting device of the present invention, the nitride semiconductor substrate is etched or peeled off so that the nitride semiconductor layer does not have a distance from the first conductivity type Al x1 Ga 1 -x1 N layer when viewed from the light emitting layer. It may be.

この構成により、窒化物半導体基板(窒化物半導体層)による短波長域の吸収をなくすことができる。   With this configuration, absorption in the short wavelength region by the nitride semiconductor substrate (nitride semiconductor layer) can be eliminated.

上記において、本発明の実施の形態および実施例について説明を行ったが、上記に開示された本発明の実施の形態および実施例は、あくまで例示であって、本発明の範囲はこれら発明の実施の形態に限定されない。本発明の範囲は、特許請求の範囲の記載によって示され、さらに特許請求の範囲の記載と均等の意味および範囲内でのすべての変更を含むものである。   Although the embodiments and examples of the present invention have been described above, the embodiments and examples of the present invention disclosed above are merely examples, and the scope of the present invention is the implementation of these inventions. It is not limited to the form. The scope of the present invention is indicated by the description of the scope of claims, and further includes meanings equivalent to the description of the scope of claims and all modifications within the scope.

本発明の発光素子およびその製造方法を用いることにより、高効率発光により高出力発
光を実現することができるので、白色発光素子の励起用光源などとして照明用途などに広範に適用されることが期待される。
By using the light emitting device of the present invention and the method for manufacturing the same, high output light emission can be realized by high efficiency light emission. Therefore, the light emitting device is expected to be widely applied to lighting applications as a light source for exciting white light emitting devices. Is done.

本発明の実施例1における紫外LEDを示す図である。It is a figure which shows ultraviolet LED in Example 1 of this invention. 図1の紫外LEDの発光スペクトルを示す図である。It is a figure which shows the emission spectrum of ultraviolet LED of FIG. 図1の紫外LEDの印加電流と光出力との関係を示す図である。It is a figure which shows the relationship between the applied current and optical output of ultraviolet LED of FIG. 本発明の実施例2における紫外LEDを示す図である。It is a figure which shows ultraviolet LED in Example 2 of this invention. 図4の発光層の拡大図である。It is an enlarged view of the light emitting layer of FIG. 図4の紫外LEDの印加電流と光出力との関係を示す図である。It is a figure which shows the relationship between the applied current and optical output of ultraviolet LED of FIG. 図4の紫外LEDの発光スペクトルを示す図である。It is a figure which shows the emission spectrum of ultraviolet LED of FIG. 本発明の実施例3における本発明例の紫外LEDと、比較例の紫外LEDの印加電流と光出力との関係を示す図である。It is a figure which shows the relationship between the applied current and light output of ultraviolet LED of the example of this invention in Example 3 of this invention, and ultraviolet LED of a comparative example. 本発明の実施例4における紫外LEDの積層構造を示す図である。It is a figure which shows the laminated structure of ultraviolet LED in Example 4 of this invention.

符号の説明Explanation of symbols

1 GaN基板、2 n型GaN層、3 n型Alx1Ga1-x1N層、4 InAlGaN発光層、4a Inx5Aly5Ga1-x5-y5N層(障壁層)、4b Inx4Aly4Ga1-x4-y4N層(井戸層)、5 p型Alx2Ga1-x2N層、6 p型GaN層、11 n電極、12 p電極、17 InxAlyGa1-x-yN緩衝層、21 n型Al0.18Ga0.82N基板、22 n型Al0.18Ga0.82N層、24a InAlGaN障壁層、24b InAlGaN井戸層、24 InAlGaN発光層、25 p型Al0.30Ga0.70N層、26 p型Al0.18Ga0.82N層。 1 GaN substrate, 2 n-type GaN layer, 3 n-type Al x1 Ga 1-x1 N layer, 4 InAlGaN light emitting layer, 4a In x5 Al y5 Ga 1-x5-y5 N layer (barrier layer), 4b In x4 Al y4 Ga 1-x4-y4 n layer (well layer), 5 p-type Al x2 Ga 1-x2 n layer, 6 p-type GaN layer, 11 n electrode, 12 p electrode, 17 In x Al y Ga 1 -xy n buffer Layer, 21 n-type Al 0.18 Ga 0.82 N substrate, 22 n-type Al 0.18 Ga 0.82 N layer, 24a InAlGaN barrier layer, 24b InAlGaN well layer, 24 InAlGaN light emitting layer, 25 p-type Al 0.30 Ga 0.70 N layer, 26 p-type Al 0.18 Ga 0.82 N layer.

Claims (4)

窒化物半導体基板の第1の主表面の側に、第1導電型のAlx1Ga1-x1N層(0≦x1≦1)を形成する工程と、
前記第1導電型のAlx1Ga1-x1N層の上にInAlGaN4元混晶を含んだ発光層を形成する工程と、
前記発光層の上に第2導電型のAlx2Ga1-x2N層(0≦x2≦1)とを形成する工程と、
前記第2導電型のAlx2Ga1-x2N層を形成した後に、前記窒化物半導体基板を除去する工程とを備える、発光素子の製造方法。
Forming a first conductivity type Al x1 Ga 1-x1 N layer (0 ≦ x1 ≦ 1) on the first main surface side of the nitride semiconductor substrate;
Forming a light emitting layer containing an InAlGaN quaternary mixed crystal on the Al x1 Ga 1-x1 N layer of the first conductivity type;
Forming a second conductivity type Al x2 Ga 1-x2 N layer (0 ≦ x2 ≦ 1) on the light emitting layer;
And a step of removing the nitride semiconductor substrate after forming the second conductivity type Al x2 Ga 1-x2 N layer.
前記窒化物半導体基板がGaN基板である、請求項1に記載の発光素子の製造方法。   The method for manufacturing a light-emitting element according to claim 1, wherein the nitride semiconductor substrate is a GaN substrate. 前記窒化物半導体基板がAlxGa1-xN基板(0<x≦1)である、請求項1に記載の発光素子の製造方法。 The method for manufacturing a light emitting element according to claim 1, wherein the nitride semiconductor substrate is an Al x Ga 1-x N substrate (0 <x ≦ 1). 第1導電型のAlx1Ga1-x1N層(0≦x1≦1)と、前記第1導電型のAlx1Ga1-x1N層の上に位置する第2導電型のAlx2Ga1-x2N層(0≦x2≦1)と、前記第1導電型のAlx1Ga1-x1N層および第2導電型のAlx2Ga1-x2N層の間に位置し、InAlGaN4元混晶を含む発光層とを有し、
前記発光層から見て前記第1導電型のAlx1Ga1-x1N層より遠くに、窒化物半導体層を有しない、発光素子。
A first conductivity type Al x1 Ga 1-x1 N layer (0 ≦ x1 ≦ 1) and a second conductivity type Al x2 Ga 1 located on the first conductivity type Al x1 Ga 1-x1 N layer. -x2 N layer (0 ≦ x2 ≦ 1) and the first conductivity type Al x1 Ga 1-x1 N layer and the second conductivity type Al x2 Ga 1-x2 N layer, And a light emitting layer containing crystals,
A light emitting device having no nitride semiconductor layer farther from the first conductivity type Al x1 Ga 1 -x1 N layer when viewed from the light emitting layer.
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