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JP3868136B2 - Gallium nitride compound semiconductor light emitting device - Google Patents

Gallium nitride compound semiconductor light emitting device Download PDF

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Publication number
JP3868136B2
JP3868136B2 JP1142199A JP1142199A JP3868136B2 JP 3868136 B2 JP3868136 B2 JP 3868136B2 JP 1142199 A JP1142199 A JP 1142199A JP 1142199 A JP1142199 A JP 1142199A JP 3868136 B2 JP3868136 B2 JP 3868136B2
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nitride semiconductor
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JP2000216432A (en
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公二 谷沢
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Nichia Corp
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Nichia Corp
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Description

【0001】
【産業上の利用分野】
本発明は窒化物半導体InAlGa1−x−yN(0≦x、0≦y、x+y≦1)よりなり、発光ダイオード素子、レーザダイオード素子等の発光素子に用いられる窒化物半導体発光素子に関する。
【0002】
【従来の技術】
窒化物半導体は高輝度純緑色発光LED、青色LEDとして、既にフルカラーLEDディスプレイ、交通信号灯、イメージスキャナ光源等の各種光源で実用化されている。これらのLED素子は基本的に、サファイア基板上にGaNよりなるn型コンタクト層と、単一量子井戸構造、若しくは多重量子井戸構造のInGaN層を包含する活性層と、MgドープAlGaNよりなるp型クラッド層と、MgドープGaNよりなるp型コンタクト層とが順に積層された構造を有しており、20mA、発光波長450nmの青色LEDで、活性層が単一量子井戸構造の場合、2.5mW、外部量子効率5パーセント、活性層が多重量子井戸構造の場合、5mW、外部量子効率9.1パーセント、また発光波長520nmの緑色LEDで、単一量子井戸構造の場合、2.2mW、外部量子効率4.3パーセント、多重量子井戸構造の場合、3mW、外部量子効率6.3パーセントと非常に優れた特性を示す。
【0003】
【発明が解決しようとする課題】
しかしながら、上記従来の窒化物半導体素子は、近年では屋外用の大型ディスプレイ等にも使用されるようになり、今後種々の応用製品への適用を考えると、さらなる発光出力の向上が求められる。発光出力を高くする方法として、n型コンタクト層をn型不純物をドープしたGaNとすると、低抵抗構造の素子が得られる。しかし、このn型不純物のドープ量を多くしていくと、n型コンタクト層の結晶性が悪くなってしまう。n型コンタクト層の結晶性が悪くなってしまうと、さらにその上に積層する活性層、p型クラッド層およびp型コンタクト層のすべての層の結晶性も悪くなってしまい、発光出力を高くするという効果が打ち消されてしまう。
【0004】
【課題を解決するための手段】
そこで本発明では、n型不純物をドープしたGaNからなるn型コンタクト層と、In、Gaを含み量子井戸を有する活性層と、p型不純物が添加されたp型AlGaNを含んでなるp型クラッド層と、p型不純物をドープしたGaNからなるp型コンタクト層とを順に有する窒化物半導体素子において、前記n型コンタクト層と活性層との間に、活性層に接して、膜厚が10オングストロームから0.2μmであるアンドープの第1の窒化物半導体層が形成され、さらに前記p型クラッド層と活性層との間に、前記p型クラッド層と活性層に接して、膜厚が10オングストロームから100オングストロームであるAlGaNから成るアンドープの第2の窒化物半導体層が形成されており、前記p型クラッド層はMgドープのAl Ga 1−b N(0<b<1)とMgドープのIn Ga 1−c N(0≦c<1)との超格子からなる層であることを特徴とする。
【0010】
本発明の発光素子は、例えば、n型コンタクト層をSi濃度が1×1018/cm以上の高濃度の不純物がドープされた低抵抗構造の窒化物半導体において、活性層に接してn側に、アンドープのInAlGa1−g−hN(0≦g、0≦h、g+h≦1)を0.2μm以下で形成し、さらに活性層に接してp側にも、アンドープのInAlGa1−i−jN(0≦i、0≦j、i+j≦1)を100オングストローム以下の膜厚で形成することで高い発光出力で結晶性の良い素子を得ることができる。さらにp型クラッド層をMgドープのAlGa1−bN(0≦b<1)とMgドープのInGa1−cN(0≦c<1)との超格子構造とすることで、高い発光出力を維持できる。また、第1および第2の窒化物半導体の膜厚は、大きくすればするほど、その上に形成する層の結晶性は良くなるが、厚くしすぎるとキャリアの注入効率が悪くなってしまい、発光しなくなってしまう。そこで、n側の第1の窒化物半導体の膜厚を0.2μm以下に、p側の第2の窒化物半導体の膜厚を100オングストローム以下にすることによって、n型コンタクト層にn型不純物としてSiを1×1021/cmと高ドープにしても20mAにおいて2.5mWを維持したLED素子ができる。
【0011】
【発明の実施の形態】
以下に本発明の一実施の形態である窒化物半導体素子の構造を示す窒化物半導体素子の模式的断面図である図1を用いて、本発明を詳細に説明する。
図1は基板1上に、バッファ層2、アンドープのGaN層3、n型不純物を含むn型コンタクト層4、アンドープからなる第1の窒化物半導体層5、単一量子井戸構造の活性層6、アンドープからなる第2の窒化物半導体層7、p型不純物を含むp型クラッド層8、p型不純物を含むp型コンタクト層9が順に積層された構造を有する。さらに、n型クラッド層4上にn電極10、p型コンタクト層9上にp電極11がそれぞれ形成されている。
【0012】
本発明において、基板1としては、サファイアC面、R面またはA面を主面とするサファイア、その他スピネル(MgAl)のような絶縁性の基板の他、SiC(6H、4H、3Cを含む)、Si、ZnO、GaAs、GaN等の半導体基板を用いることができる。
【0013】
本発明において、バッファ層2としては、AlGaNからなる窒化物半導体であり、好ましくはAlの割合が小さい組成ほど結晶性の改善が顕著となり、より好ましくはGaNからなるバッファ層2が挙げられる。
【0014】
次に本発明において、アンドープGaN層3は、成長する際にn型不純物を添加せずに成長してなる層を示す。バッファ層2上にアンドープのGaN層3を成長させるとアンドープGaN層の結晶性が良好となり、アンドープGaN層3上に成長させるn型コンタクト層4などの結晶性も良好となる。
【0015】
次に本発明において、n型不純物を含むn型コンタクト層4は、n型不純物としてSiをドープしたGaNとし、不純物濃度は1×1018/cm以上、1×1021/cm以下、好ましくは5×1018/cm以上、5×1020/cm以下に調整する。このようにn型不純物を多くドープし、この層をn型コンタクト層とすると、Vおよび閾値を低下させることができる。不純物濃度が上記範囲を逸脱するとVが低下しにくくなる傾向にある。また、n型コンタクト層4は、結晶性の良好なアンドープのGaN3上に形成されると、高濃度のn型不純物を有しているにもかかわらず結晶性を良好にすることができる。
【0016】
またn型コンタクト層4の組成は、InAlGa1−k−mN(0≦k、0≦m、k+m≦1)で構成でき、その組成は特に問うものではないが、好ましくはGaN、m値0.2以下のAlGa1−mNとすると結晶性の少ない窒化物半導体層が得られやすい。
【0017】
次に本発明においてn側の第1の窒化物半導体層5は、アンドープのInAlGa1−g−hN(0≦g、0≦h、g+h≦1)とし、10オングストロームから0.5μmの範囲で、好ましくは10オングストロームから0.2μmの範囲で、活性層に接して形成する。n側にはキャリア濃度が高濃度で存在するが、第1の窒化物半導体層の膜厚が0.5μmを越えてしまうとキャリアの注入効率が悪くなってしまい、充分な発光出力が得られない。また、10オングストロームより小さいとその上に形成する層の結晶性が悪くなってしまい、同様に充分な発光出力が得られない。
【0018】
また本発明において活性層6は、In、Gaを含むアンドープの窒化物半導体、好ましくはInGaNよりなる井戸層を有する単一または多重の量子井戸構造とすることが望ましい。また本発明における低抵抗構造の窒化物半導体発光素子は、特に単一量子井戸構造の時に顕著な効果がある。
【0019】
次に本発明においてp側の第2の窒化物半導体層7は、アンドープのInAlGa1−i−jN(0≦i、0≦j、i+j≦1)とし、10オングストロームから、0.1μmの範囲で、好ましくは10オングストロームから100オングストロームの範囲で、活性層に接して形成する。
【0020】
次に本発明においてp型クラッド層8は、p型不純物としてMgをドープしたAlGa1−bN(0≦b<1)の単層からなる層でも良いが、好ましくはAlGa1−bN(0≦b<1)とMgドープのInGa1−cN(0≦c<1)との超格子構造とすることが望ましい。p型クラッド層を超格子構造とすると抵抗率が低下するため、Vおよび閾値が低下できると共に発光出力の高い素子を得ることができる。またこの層を超格子構造とする場合、超格子を構成する窒化物半導体層の膜厚は100オングストローム以下、さらに好ましくは70オングストローム以下、さらに最も好ましくは50オングストローム以下に調整する。
【0021】
次に本発明においてp型コンタクト層9は、p型不純物としてMgをドープしたGaNとし、不純物濃度を1×1018〜1×1021/cm、より好ましくは5×1018〜5×1020/cm、より好ましくは5×1019〜1×1020/cmとすることで良好なp型膜ができ好ましい。
【0022】
【実施例】
以下に、本発明の一実施の形態である実施例を示すが、本発明はこれに限定されない。
[実施例1]
図1を元に実施例1について説明する。
サファイア(C面)よりなる基板1をMOVPEの反応容器内にセットし、水素を流しながら、基板の温度を1050℃まで上昇させ、基板のクリーニングを行う。
【0023】
(バッファ層2)
続いて、温度を510℃まで下げ、キャリアガスに水素、原料ガスにアンモニアとTMG(トリメチルガリウム)とを用い、基板1上にGaNよりなるバッファ層2を150オングストロームの膜厚で成長させる。
(アンドープGaN層3)
バッファ層2成長後、TMGのみ止めて、温度を1050℃まで昇温させる。続いて1050℃で、同じく原料ガスに、TMG、アンモニアを用い、アンドープGaN層3を1.5μmの膜厚で成長させる。
【0024】
(n型コンタクト層4)
続いて1050℃で、同じく原料ガスにTMG、アンモニア、不純物ガスとしてシランガスを用い、Siを4.5×1018/cmドープしたGaNよりなるn型コンタクト層4を2.25μmの膜厚で成長させる。
【0025】
(n側窒化物半導体層5)
次にシランガスを止め、1050℃で、TMG、TMA、アンモニアを用い、アンドープAlGaN層5を0.15μmの膜厚で成長させる。
(活性層6)
次に、温度を800℃まで下げ、TMG、TMI(トリメチルインジウム)、アンモニアを用い、アンドープIn0.35Ga0.65Nよりなる活性層6を30オングストロームの膜厚で成長させる。
【0026】
(p側窒化物半導体層7)
次に窒素、TMIを止め、温度を1050℃まで昇温し、TMG、TMA、アンモニアを用い、アンドープAlGaN層7を10オングストロームの膜厚で成長させる。
【0027】
(p型クラッド層8)
続いて1050℃で、TMG、TMA、アンモニア、CpMgを用い、Mgを1×1020/cmドープしたAlGaNよりなる層を40オングストローム成長させ、次に温度を800℃にして、TMAを止めTMIを流し、同じくMgを1×1020/cmドープしたInGaNよりなる層を25オングストロームの膜厚で成長させる。そしてこれらの操作を交互に繰り返し、5層ずつ積層させた、超格子からなるp型クラッド層8を成長させる。
【0028】
(p型コンタクト層9)
続いて1050℃で、TMG、アンモニア、CpMgを用い、Mgを1×1020/cmドープしたp型GaNよりなるp型コンタクト層9を0.15μmの膜厚で成長させる。
【0029】
反応終了後、温度を室温まで下げ、更に窒素雰囲気中、ウエハーを反応容器内において、700℃でアニーリングを行い、p型層を更に低抵抗化する。
アニーリング後、ウエハーを反応容器から取り出し、最上層のp型コンタクト層9の表面に所定のマスクを形成し、RIE(反応性イオンエッチング)装置でp型コンタクト層側からエッチングを行い、図1に示すようにn型コンタクト層4の表面を露出させる。
【0030】
エッチング後、最上層にあるp型コンタクト層のほぼ全面に膜厚200オングストロームのNi、Auを含む透光性のp電極10を0.5μmの膜厚で形成し、一方エッチングにより露出させたn型コンタクト層4の表面にはWとAlを含むn電極11を形成してLED素子とした。
このLED素子は順方向電圧20mAにおいて、順方向電圧3.4V、468nmの青色発光を示し、発光出力は3mWであった。
【0031】
[実施例2]
実施例1において活性層6を以下のようにした他は同様にしてLED素子を作製した。
(活性層6)
1050℃でアンドープのGaNよりなる障壁層を200オングストロームの膜厚で成長させ、続いて温度を800℃にしてTMG、TMI(トリメチルインジウム)、アンモニアを用い、アンドープIn0.35Ga0.65Nよりなる井戸層を30オングストロームの膜厚で成長させる。そして障壁+井戸+障壁+井戸+・・・+障壁の順で障壁層を5層、井戸層を4層交互に積層して総膜厚1120オングストロームの多重量子井戸構造よりなる活性層6を成長させる。
その結果、このLED素子は順方向電圧20mAにおいて、順方向電圧3.6V、470nmの青色発光を示し、発光出力は6.0mWであった。
【0032】
[実施例3]
実施例1において活性層6を以下のようにした他は同様にしてLED素子を作製した。
(活性層6)
800℃で、TMG、TMI(トリメチルインジウム)、アンモニアを用い、アンドープIn0.45Ga0.55Nよりなる活性層6を30オングストロームの膜厚で成長させる。
その結果、このLED素子は順方向電圧20mAにおいて、順方向電圧3.4V、500nmの青緑色発光を示し、発光出力は2.5mWであった。
【0033】
[実施例4]
実施例1において、p側の第2の窒化物半導体層7を除いた他は同様にしてLED素子を作製したところ、実施例1よりは少し劣るが同等の特性を有するLED素子が得られた。
【0034】
[実施例5]
実施例1において、p型クラッド層8を以下のようにした他は同様にしてLED素子を作製した。
(p型クラッド層8)
1050℃で、TMG、TMA、アンモニア、CpMgを用い、Mgを1×1020/cmドープしたAlGaNよりなるp型クラッド層8を250オングストロームの膜厚で成長させた。
その他は実施例1と同様にしてLED素子を作製したところ、実施例1よりは少し劣るが同等の特性を有するLED素子が得られた。
【0035】
【発明の効果】
以上説明したように、本発明によれば、n型コンタクト層を高濃度の不純物がドープされた窒化物半導体とした低抵抗構造の窒化物半導体素子において、n型コンタクト層と活性層との間にアンドープの第1の窒化物半導体層を2000オングストローム以下の膜厚で設け、さらにp型クラッド層と活性層との間にアンドープの第2の窒化物半導体層を100オングストローム以下の膜厚で設ける。このような構造にしたことによって、Vfおよび閾値が低下し、高い発光出力の素子が得られる。例えば、n型コンタクト層にn型不純物としてSiを1×1021/cmと高ドープにしても20mAにおいて2.5mWを維持したLED素子ができる。
【図面の簡単な説明】
【図1】本発明の一実施例にかかるLED素子の構造を示す模式断面図。
【符号の簡単な説明】
1・・・基板、
2・・・バッファ層、
3・・・GaN層、
4・・・n型コンタクト層、
5・・・n側窒化物半導体層、
6・・・活性層、
7・・・p側窒化物半導体層、
8・・・p型クラッド層、
9・・・p型コンタクト層、
10・・・p電極、
11・・・n電極。
[0001]
[Industrial application fields]
The present invention comprises a nitride semiconductor In x Al y Ga 1-xy N (0 ≦ x, 0 ≦ y, x + y ≦ 1), and is used for a light emitting element such as a light emitting diode element and a laser diode element. The present invention relates to a light emitting element.
[0002]
[Prior art]
Nitride semiconductors have already been put to practical use in various light sources such as full-color LED displays, traffic signal lights, and image scanner light sources as high-luminance pure green light-emitting LEDs and blue LEDs. These LED elements basically include an n-type contact layer made of GaN on a sapphire substrate, an active layer including an InGaN layer having a single quantum well structure or a multiple quantum well structure, and a p-type made of Mg-doped AlGaN. It has a structure in which a clad layer and a p-type contact layer made of Mg-doped GaN are stacked in order, and if the active layer is a single quantum well structure with a blue LED of 20 mA and an emission wavelength of 450 nm, 2.5 mW The external quantum efficiency is 5%, the active layer has a multiple quantum well structure, 5 mW, the external quantum efficiency is 9.1%, and the green light emission wavelength is 520 nm, and the single quantum well structure is 2.2 mW. In the case of an efficiency of 4.3 percent, a multiple quantum well structure, 3 mW and an external quantum efficiency of 6.3 percent exhibit very excellent characteristics.
[0003]
[Problems to be solved by the invention]
However, in recent years, the conventional nitride semiconductor element has been used for outdoor large-sized displays and the like, and further improvement in light emission output is required in consideration of application to various application products in the future. If the n-type contact layer is GaN doped with an n-type impurity as a method for increasing the light output, an element having a low resistance structure can be obtained. However, when the doping amount of the n-type impurity is increased, the crystallinity of the n-type contact layer is deteriorated. If the crystallinity of the n-type contact layer is deteriorated, the crystallinity of all the active layer, p-type cladding layer and p-type contact layer laminated thereon is also deteriorated, and the light emission output is increased. The effect will be countered.
[0004]
[Means for Solving the Problems]
Therefore, in the present invention, an n-type contact layer made of GaN doped with an n-type impurity, an active layer containing In and Ga and having a quantum well, and a p-type cladding containing p-type AlGaN doped with a p-type impurity. In a nitride semiconductor device having a layer and a p-type contact layer made of GaN doped with a p-type impurity in order, the film thickness is 10 angstroms between the n-type contact layer and the active layer and in contact with the active layer To 0.2 μm of undoped first nitride semiconductor layer is formed, and further, between the p-type cladding layer and the active layer, is in contact with the p-type cladding layer and the active layer and has a thickness of 10 Å a second nitride semiconductor layer of undoped made of AlGaN is formed is 100 Å, the p-type cladding layer of Mg doped Al b Ga Characterized in that a layer consisting of a superlattice of -b N (0 <b <1 ) and Mg-doped In c Ga 1-c N ( 0 ≦ c <1).
[0010]
The light-emitting element of the present invention is, for example, a nitride semiconductor having a low resistance structure in which an n-type contact layer is doped with a high-concentration impurity having a Si concentration of 1 × 10 18 / cm 3 or more. In addition, undoped In g Al h Ga 1-gh N (0 ≦ g, 0 ≦ h, g + h ≦ 1) is formed with a thickness of 0.2 μm or less, and is further in contact with the active layer on the p side. By forming In i Al j Ga 1-ij N (0 ≦ i, 0 ≦ j, i + j ≦ 1) with a film thickness of 100 angstroms or less, an element with high light emission output and good crystallinity can be obtained. . Furthermore, the p-type cladding layer has a superlattice structure of Mg-doped Al b Ga 1-b N (0 ≦ b <1) and Mg-doped In c Ga 1-c N (0 ≦ c <1). High light output can be maintained. Further, the larger the film thickness of the first and second nitride semiconductors, the better the crystallinity of the layer formed thereon, but if it is too thick, the carrier injection efficiency will deteriorate, It stops emitting light. Therefore, by reducing the thickness of the first nitride semiconductor on the n side to 0.2 μm or less and the thickness of the second nitride semiconductor on the p side to 100 angstroms or less, the n-type impurity is added to the n-type contact layer. As a result, even if Si is highly doped to 1 × 10 21 / cm 3 , an LED element can be maintained that maintains 2.5 mW at 20 mA.
[0011]
DETAILED DESCRIPTION OF THE INVENTION
Hereinafter, the present invention will be described in detail with reference to FIG. 1 which is a schematic cross-sectional view of a nitride semiconductor device showing the structure of a nitride semiconductor device according to an embodiment of the present invention.
FIG. 1 shows a substrate 1, a buffer layer 2, an undoped GaN layer 3, an n-type contact layer 4 containing an n-type impurity, an undoped first nitride semiconductor layer 5, and an active layer 6 having a single quantum well structure. , A second nitride semiconductor layer 7 made of undoped, a p-type cladding layer 8 containing a p-type impurity, and a p-type contact layer 9 containing a p-type impurity are sequentially stacked. Further, an n-electrode 10 is formed on the n-type cladding layer 4, and a p-electrode 11 is formed on the p-type contact layer 9.
[0012]
In the present invention, as the substrate 1, in addition to sapphire whose main surface is the sapphire C-plane, R-plane or A-plane, other insulating substrates such as spinel (MgAl 2 O 4 ), SiC (6H, 4H, 3C Semiconductor substrates such as Si, ZnO, GaAs, and GaN can be used.
[0013]
In the present invention, the buffer layer 2 is a nitride semiconductor made of AlGaN, and the crystallinity improvement becomes more remarkable as the composition having a smaller Al ratio, more preferably, the buffer layer 2 made of GaN.
[0014]
Next, in the present invention, the undoped GaN layer 3 is a layer formed without adding an n-type impurity during growth. When the undoped GaN layer 3 is grown on the buffer layer 2, the crystallinity of the undoped GaN layer is improved, and the crystallinity of the n-type contact layer 4 grown on the undoped GaN layer 3 is also improved.
[0015]
Next, in the present invention, the n-type contact layer 4 containing an n-type impurity is made of GaN doped with Si as an n-type impurity, and the impurity concentration is 1 × 10 18 / cm 3 or more, 1 × 10 21 / cm 3 or less, Preferably, it is adjusted to 5 × 10 18 / cm 3 or more and 5 × 10 20 / cm 3 or less. Thus, if a large amount of n-type impurity is doped and this layer is an n-type contact layer, V f and the threshold can be lowered. When the impurity concentration deviates from the above range, V f tends to be difficult to decrease. Further, when the n-type contact layer 4 is formed on undoped GaN 3 having good crystallinity, the crystallinity can be improved despite having a high concentration of n-type impurities.
[0016]
The composition of the n-type contact layer 4 can be composed of In k Al m Ga 1-km N (0 ≦ k, 0 ≦ m, k + m ≦ 1), and the composition is not particularly limited, When GaN is Al m Ga 1-m N having an m value of 0.2 or less, a nitride semiconductor layer with low crystallinity is easily obtained.
[0017]
Next, in the present invention, the n-side first nitride semiconductor layer 5 is undoped In g Al h Ga 1-gh N (0 ≦ g, 0 ≦ h, g + h ≦ 1). It is formed in contact with the active layer in the range of 0.5 μm, preferably in the range of 10 Å to 0.2 μm. Although there is a high carrier concentration on the n side, the carrier injection efficiency deteriorates when the film thickness of the first nitride semiconductor layer exceeds 0.5 μm, and a sufficient light emission output is obtained. Absent. On the other hand, if the thickness is smaller than 10 angstroms, the crystallinity of the layer formed thereon deteriorates, and a sufficient light output cannot be obtained.
[0018]
In the present invention, the active layer 6 desirably has a single or multiple quantum well structure having a well layer made of an undoped nitride semiconductor containing In and Ga, preferably InGaN. The nitride semiconductor light emitting device having a low resistance structure according to the present invention has a remarkable effect particularly in a single quantum well structure.
[0019]
Next, in the present invention, the second nitride semiconductor layer 7 on the p side is undoped In i Al j Ga 1-ij N (0 ≦ i, 0 ≦ j, i + j ≦ 1), from 10 angstroms, It is formed in contact with the active layer in the range of 0.1 μm, preferably in the range of 10 Å to 100 Å.
[0020]
Next, in the present invention, the p-type cladding layer 8 may be a layer composed of a single layer of Al b Ga 1-b N (0 ≦ b <1) doped with Mg as a p-type impurity, but is preferably Al b Ga 1. -b N (0 ≦ b <1 ) and it is desirable that the super lattice structure of the Mg-doped in c Ga 1-c N ( 0 ≦ c <1). When the p-type cladding layer has a superlattice structure, the resistivity decreases, so that an element having a high light emission output can be obtained while V f and the threshold value can be decreased. When this layer has a superlattice structure, the thickness of the nitride semiconductor layer constituting the superlattice is adjusted to 100 angstroms or less, more preferably 70 angstroms or less, and most preferably 50 angstroms or less.
[0021]
Next, in the present invention, the p-type contact layer 9 is made of GaN doped with Mg as a p-type impurity, and the impurity concentration is 1 × 10 18 to 1 × 10 21 / cm 3 , more preferably 5 × 10 18 to 5 × 10. A preferable p-type film can be obtained by adjusting to 20 / cm 3 , more preferably 5 × 10 19 to 1 × 10 20 / cm 3 .
[0022]
【Example】
Examples of the present invention will be described below, but the present invention is not limited thereto.
[Example 1]
A first embodiment will be described with reference to FIG.
The substrate 1 made of sapphire (C-plane) is set in a MOVPE reaction vessel, and the temperature of the substrate is raised to 1050 ° C. while flowing hydrogen to clean the substrate.
[0023]
(Buffer layer 2)
Subsequently, the temperature is lowered to 510 ° C., hydrogen is used as the carrier gas, ammonia and TMG (trimethyl gallium) are used as the source gas, and a buffer layer 2 made of GaN is grown on the substrate 1 to a thickness of 150 Å.
(Undoped GaN layer 3)
After growing the buffer layer 2, only TMG is stopped and the temperature is raised to 1050 ° C. Subsequently, at 1050 ° C., TMG and ammonia are similarly used as source gases, and the undoped GaN layer 3 is grown to a thickness of 1.5 μm.
[0024]
(N-type contact layer 4)
Subsequently, at 1050 ° C., the n-type contact layer 4 made of GaN doped with 4.5 × 10 18 / cm 3 of Si is used with a source gas of TMG, ammonia, and silane gas as an impurity gas, with a thickness of 2.25 μm. Grow.
[0025]
(N-side nitride semiconductor layer 5)
Next, the silane gas is stopped and an undoped AlGaN layer 5 is grown to a thickness of 0.15 μm at 1050 ° C. using TMG, TMA, and ammonia.
(Active layer 6)
Next, the temperature is lowered to 800 ° C., and an active layer 6 made of undoped In 0.35 Ga 0.65 N is grown to a thickness of 30 Å using TMG, TMI (trimethylindium), and ammonia.
[0026]
(P-side nitride semiconductor layer 7)
Next, nitrogen and TMI are stopped, the temperature is raised to 1050 ° C., and an undoped AlGaN layer 7 is grown to a thickness of 10 Å using TMG, TMA, and ammonia.
[0027]
(P-type cladding layer 8)
Subsequently, at 1050 ° C., a layer made of AlGaN doped with Mg at 1 × 10 20 / cm 3 is grown at 40 Å using TMG, TMA, ammonia, Cp 2 Mg, and then the temperature is set at 800 ° C. A stop TMI is flown and a layer made of InGaN doped with 1 × 10 20 / cm 3 of Mg is grown to a thickness of 25 Å. These operations are alternately repeated to grow a p-type cladding layer 8 made of a superlattice in which five layers are stacked.
[0028]
(P-type contact layer 9)
Subsequently, at 1050 ° C., a p-type contact layer 9 made of p-type GaN doped with 1 × 10 20 / cm 3 of Mg is grown to a thickness of 0.15 μm using TMG, ammonia, and Cp 2 Mg.
[0029]
After completion of the reaction, the temperature is lowered to room temperature, and the wafer is annealed in a reaction vessel at 700 ° C. in a nitrogen atmosphere to further reduce the resistance of the p-type layer.
After annealing, the wafer is taken out from the reaction vessel, a predetermined mask is formed on the surface of the uppermost p-type contact layer 9, and etching is performed from the p-type contact layer side with an RIE (reactive ion etching) apparatus. As shown, the surface of the n-type contact layer 4 is exposed.
[0030]
After etching, a light-transmitting p-electrode 10 containing Ni and Au having a thickness of 200 angstroms is formed on almost the entire surface of the p-type contact layer as the uppermost layer with a thickness of 0.5 μm, while n is exposed by etching. An n-electrode 11 containing W and Al was formed on the surface of the mold contact layer 4 to obtain an LED element.
This LED element emitted blue light with a forward voltage of 3.4 V and 468 nm at a forward voltage of 20 mA, and the light emission output was 3 mW.
[0031]
[Example 2]
An LED element was fabricated in the same manner as in Example 1 except that the active layer 6 was changed as follows.
(Active layer 6)
A barrier layer made of undoped GaN is grown at a temperature of 1050 ° C. to a thickness of 200 Å. Subsequently, the temperature is set to 800 ° C., and TMG, TMI (trimethylindium), and ammonia are used, and undoped In 0.35 Ga 0.65 N A well layer composed of 30 Å is grown to a thickness of 30 Å. Then, five barrier layers and four well layers are alternately stacked in the order of barrier + well + barrier + well +... + Barrier to grow an active layer 6 having a multiple quantum well structure with a total thickness of 1120 angstroms. Let
As a result, this LED element emitted blue light with a forward voltage of 3.6 V and 470 nm at a forward voltage of 20 mA, and the light emission output was 6.0 mW.
[0032]
[Example 3]
An LED element was fabricated in the same manner as in Example 1 except that the active layer 6 was changed as follows.
(Active layer 6)
At 800 ° C., an active layer 6 made of undoped In 0.45 Ga 0.55 N is grown to a thickness of 30 Å using TMG, TMI (trimethylindium), and ammonia.
As a result, this LED element emitted blue-green light with a forward voltage of 3.4 V and 500 nm at a forward voltage of 20 mA, and the light emission output was 2.5 mW.
[0033]
[Example 4]
In Example 1, except that the second nitride semiconductor layer 7 on the p side was removed, an LED element was produced in the same manner. As a result, an LED element having the same characteristics as that of Example 1 was obtained. .
[0034]
[Example 5]
An LED element was fabricated in the same manner as in Example 1 except that the p-type cladding layer 8 was changed as follows.
(P-type cladding layer 8)
A p-type cladding layer 8 made of AlGaN doped with Mg at 1 × 10 20 / cm 3 was grown at a thickness of 250 Å at 1050 ° C. using TMG, TMA, ammonia, and Cp 2 Mg.
Other than that, an LED element was produced in the same manner as in Example 1. As a result, an LED element having the same characteristics was obtained although it was slightly inferior to Example 1.
[0035]
【The invention's effect】
As described above, according to the present invention, in a nitride semiconductor device having a low resistance structure in which an n-type contact layer is a nitride semiconductor doped with a high concentration of impurities, the n-type contact layer is provided between the n-type contact layer and the active layer. An undoped first nitride semiconductor layer is provided with a thickness of 2000 angstroms or less, and an undoped second nitride semiconductor layer is provided with a thickness of 100 angstroms or less between the p-type cladding layer and the active layer. . With such a structure, Vf and the threshold value are reduced, and an element with high light emission output can be obtained. For example, an LED element that maintains 2.5 mW at 20 mA can be obtained even if the n-type contact layer is highly doped with Si as 1 × 10 21 / cm 3 as an n-type impurity.
[Brief description of the drawings]
FIG. 1 is a schematic cross-sectional view showing the structure of an LED element according to an embodiment of the present invention.
[Brief description of symbols]
1 ... substrate
2 ... buffer layer,
3 ... GaN layer,
4 ... n-type contact layer,
5 ... n-side nitride semiconductor layer,
6 ... active layer,
7... P-side nitride semiconductor layer,
8 ... p-type cladding layer,
9: p-type contact layer,
10 ... p electrode,
11: n electrode.

Claims (5)

n型不純物をドープしたGaNからなるn型コンタクト層と、In、Gaを含み量子井戸を有する活性層と、p型不純物が添加されたp型AlGaNを含んでなるp型クラッド層と、p型不純物をドープしたGaNからなるp型コンタクト層とを順に有する窒化物半導体素子において、
前記n型コンタクト層と活性層との間に、活性層に接して、膜厚が10オングストロームから0.2μmであるアンドープの第1の窒化物半導体層が形成され、
さらに前記p型クラッド層と活性層との間に、前記p型クラッド層と活性層に接して、膜厚が10オングストロームから100オングストロームであるAlGaNから成るアンドープの第2の窒化物半導体層が形成されており、
前記p型クラッド層はMgドープのAl Ga 1−b N(0<b<1)とMgドープのIn Ga 1−c N(0≦c<1)との超格子からなる層であることを特徴とする窒化物半導体発光素子。
an n-type contact layer made of GaN doped with an n-type impurity, an active layer containing In and Ga and having a quantum well, a p-type cladding layer containing p-type AlGaN doped with a p-type impurity, and a p-type In a nitride semiconductor device having a p-type contact layer made of GaN doped with impurities in order,
An undoped first nitride semiconductor layer having a thickness of 10 angstroms to 0.2 μm is formed between the n-type contact layer and the active layer in contact with the active layer,
Further, an undoped second nitride semiconductor layer made of AlGaN having a thickness of 10 angstroms to 100 angstroms is formed between the p-type cladding layer and the active layer in contact with the p-type cladding layer and the active layer. Has been
The p-type cladding layer is a layer made of a superlattice of Mg-doped Al b Ga 1-b N (0 <b <1) and Mg-doped In c Ga 1-c N (0 ≦ c <1). A nitride semiconductor light emitting device characterized by that.
前記n型コンタクト層はn型不純物として、Siが1×1018/cm以上、1×1021/cm以下でドープされていることを特徴とする請求項1に記載の窒化物半導体発光素子。2. The nitride semiconductor light emitting device according to claim 1, wherein the n-type contact layer is doped with Si as 1 × 10 18 / cm 3 or more and 1 × 10 21 / cm 3 or less as an n-type impurity. element. 前記第1の窒化物半導体層は、アンドープAlGaN層であることを特徴とする請求項1又は2に記載の窒化物半導体発光素子。The nitride semiconductor light-emitting element according to claim 1, wherein the first nitride semiconductor layer is an undoped AlGaN layer. 前記活性層は単一量子井戸構造であることを特徴とする請求項1から請求項のいずれかに記載の窒化物半導体発光素子。The nitride semiconductor light emitting device according to any one of claims 1 to 3 , wherein the active layer has a single quantum well structure. 前記p側のアンドープからなる第2の窒化物半導体層の膜厚は、10オングストロームであることを特徴とする請求項1から請求項のいずれかに記載の窒化物半導体発光素子The thickness of the second semiconductor layer made of the p-side of the undoped nitride semiconductor light emitting device according to any one of claims 1 to 4, characterized in that the 10 Å
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Publication number Priority date Publication date Assignee Title
US6635904B2 (en) * 2001-03-29 2003-10-21 Lumileds Lighting U.S., Llc Indium gallium nitride smoothing structures for III-nitride devices
US6489636B1 (en) 2001-03-29 2002-12-03 Lumileds Lighting U.S., Llc Indium gallium nitride smoothing structures for III-nitride devices
US6958497B2 (en) 2001-05-30 2005-10-25 Cree, Inc. Group III nitride based light emitting diode structures with a quantum well and superlattice, group III nitride based quantum well structures and group III nitride based superlattice structures
KR20030053290A (en) * 2001-12-22 2003-06-28 엘지이노텍 주식회사 Nitrogen-Compound Semiconductor Device and Method for manufacturing a Nitrogen-Compound Semiconductor Device
TWI271877B (en) 2002-06-04 2007-01-21 Nitride Semiconductors Co Ltd Gallium nitride compound semiconductor device and manufacturing method
KR100489039B1 (en) * 2002-08-19 2005-05-11 엘지이노텍 주식회사 Fabrication method for GaN semiconductor LED
JP4571372B2 (en) * 2002-11-27 2010-10-27 ローム株式会社 Semiconductor light emitting device
US9153645B2 (en) 2005-05-17 2015-10-06 Taiwan Semiconductor Manufacturing Company, Ltd. Lattice-mismatched semiconductor structures with reduced dislocation defect densities and related methods for device fabrication
US8324660B2 (en) 2005-05-17 2012-12-04 Taiwan Semiconductor Manufacturing Company, Ltd. Lattice-mismatched semiconductor structures with reduced dislocation defect densities and related methods for device fabrication
US7777250B2 (en) 2006-03-24 2010-08-17 Taiwan Semiconductor Manufacturing Company, Ltd. Lattice-mismatched semiconductor structures and related methods for device fabrication
EP2062290B1 (en) 2006-09-07 2019-08-28 Taiwan Semiconductor Manufacturing Company, Ltd. Defect reduction using aspect ratio trapping
WO2008039534A2 (en) 2006-09-27 2008-04-03 Amberwave Systems Corporation Quantum tunneling devices and circuits with lattice- mismatched semiconductor structures
US8502263B2 (en) 2006-10-19 2013-08-06 Taiwan Semiconductor Manufacturing Company, Ltd. Light-emitter-based devices with lattice-mismatched semiconductor structures
US8304805B2 (en) 2009-01-09 2012-11-06 Taiwan Semiconductor Manufacturing Company, Ltd. Semiconductor diodes fabricated by aspect ratio trapping with coalesced films
US9508890B2 (en) 2007-04-09 2016-11-29 Taiwan Semiconductor Manufacturing Company, Ltd. Photovoltaics on silicon
US7825328B2 (en) 2007-04-09 2010-11-02 Taiwan Semiconductor Manufacturing Company, Ltd. Nitride-based multi-junction solar cell modules and methods for making the same
US8237151B2 (en) 2009-01-09 2012-08-07 Taiwan Semiconductor Manufacturing Company, Ltd. Diode-based devices and methods for making the same
US8329541B2 (en) 2007-06-15 2012-12-11 Taiwan Semiconductor Manufacturing Company, Ltd. InP-based transistor fabrication
JP2010538495A (en) 2007-09-07 2010-12-09 アンバーウェーブ・システムズ・コーポレーション Multi-junction solar cell
US8183667B2 (en) 2008-06-03 2012-05-22 Taiwan Semiconductor Manufacturing Co., Ltd. Epitaxial growth of crystalline material
US8274097B2 (en) 2008-07-01 2012-09-25 Taiwan Semiconductor Manufacturing Company, Ltd. Reduction of edge effects from aspect ratio trapping
US8981427B2 (en) 2008-07-15 2015-03-17 Taiwan Semiconductor Manufacturing Company, Ltd. Polishing of small composite semiconductor materials
US20100072515A1 (en) 2008-09-19 2010-03-25 Amberwave Systems Corporation Fabrication and structures of crystalline material
EP2528087B1 (en) 2008-09-19 2016-06-29 Taiwan Semiconductor Manufacturing Company, Ltd. Formation of devices by epitaxial layer overgrowth
US8253211B2 (en) 2008-09-24 2012-08-28 Taiwan Semiconductor Manufacturing Company, Ltd. Semiconductor sensor structures with reduced dislocation defect densities
WO2010114956A1 (en) 2009-04-02 2010-10-07 Taiwan Semiconductor Manufacturing Company, Ltd. Devices formed from a non-polar plane of a crystalline material and method of making the same
US8575592B2 (en) 2010-02-03 2013-11-05 Cree, Inc. Group III nitride based light emitting diode structures with multiple quantum well structures having varying well thicknesses
JP5682716B2 (en) * 2014-01-09 2015-03-11 三菱化学株式会社 Nitride semiconductor
US9425351B2 (en) * 2014-10-06 2016-08-23 Wisconsin Alumni Research Foundation Hybrid heterostructure light emitting devices
US9899556B2 (en) 2015-09-14 2018-02-20 Wisconsin Alumni Research Foundation Hybrid tandem solar cells with improved tunnel junction structures
CN115004390A (en) * 2019-12-24 2022-09-02 密歇根大学董事会 Group III nitride exciton heterostructures

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