JP2004235473A - Compound semiconductor element and method for manufacturing the same - Google Patents

Compound semiconductor element and method for manufacturing the same Download PDF

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JP2004235473A
JP2004235473A JP2003022685A JP2003022685A JP2004235473A JP 2004235473 A JP2004235473 A JP 2004235473A JP 2003022685 A JP2003022685 A JP 2003022685A JP 2003022685 A JP2003022685 A JP 2003022685A JP 2004235473 A JP2004235473 A JP 2004235473A
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layer
semiconductor element
boundary
mixed crystal
buffer layer
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JP4458223B2 (en
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Yukari Suzuki
由佳里 鈴木
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Shin Etsu Handotai Co Ltd
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Shin Etsu Handotai Co Ltd
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Abstract

<P>PROBLEM TO BE SOLVED: To provide a compound semiconductor element structure wherein crystal defects are reluctant to occur along the boundary between a buffer zone and a semiconductor element layer and wherein high-quality element layers are realized with stability, and to provide a method for manufacturing the same. <P>SOLUTION: For the heteroepitaxial growth of a semiconductor element layer 50 constituted of In<SB>x</SB>Ga<SB>y</SB>Al<SB>1-x-y</SB>N on a single crystal substrate 1 of SiC, sapphire, or silicon, an Al<SB>1-a</SB>In<SB>a</SB>N layer is used as a buffer layer 2 wherein the mixed crystal ratio a of InN is higher on the side of the boundary with the semiconductor layer 50 than on the side of the boundary with the single crystal substrate 1. By adjusting the mixed crystal ratio a of InN whose lattice constant is larger than that of GaN, the lattice constant of the buffer layer 2 is made to be nearer to the lattice constant of the semiconductor element layer 50 on the side of the boundary with the semiconductor element layer 50, as compared with a conventional buffer layer constituted of GaN, AlN, or their combination. On the side of the boundary with the single crystal substrate 1, difference in lattice constant from that of the single crystal substrate 1 is effectively reduced by lowering the mixed crystal ratio a of InN. <P>COPYRIGHT: (C)2004,JPO&NCIPI

Description

【0001】
【発明の属する技術分野】
この発明は、化合物半導体素子及びその製造方法に関する。
【0002】
【従来の技術】
【特許文献1】
特開平5−110138号公報
【特許文献2】
特開平5−206513号公報
【0003】
化合物半導体の多層構造は、周知の通り、MESFET(Metal−Semiconductor Field Effect Transistor)やHEMT(High Electron Mobility Transistor)などの超高速トランジスタや、発光ダイオードやレーザーなどの発光素子に応用され、多くの需要を獲得するに至っている。近年注目を集めている半導体多層構造に、GaN系化合物系半導体を用いたヘテロ接合構造がある。GaN系化合物系半導体は室温におけるバンドギャップが2.0eV〜6.2eVまで変化可能であり、化学的にも安定であることから、青色等の発光素子に応用され、普及しつつある。また、GaN系化合物系半導体はバンドギャップの広さに加え、高い電子移動度を有し、かつヘテロ接合形成が容易であることから、高温環境での動作が可能であり、より高速・高出力の次世代型超高速トランジスタへの応用も注目されており、研究が重ねられている。
【0004】
GaN系化合物系半導体は、GaAs系化合物などと異なり、ホモエピタキシャル成長を可能とする半絶縁性単結晶基板を製造することが困難であるため、ヘテロ接合構造を有する素子層を形成するに際しては、SiC単結晶基板やサファイア(単結晶アルミナ)基板が使用されている。この際、GaN(特許文献1)あるいはAlNをバッファ層として単結晶基板上に成長させ、その後、素子層をヘテロエピタキシャル成長させることにより、素子層の品質を高めることがなされている。
【0005】
【発明が解決しようとする課題】
GaN系化合物系半導体のヘテロエピタキシャル成長においては、単結晶基板として用いるSiCあるいはサファイアとGaNとの格子定数差が非常に大きい(SiCでは約5%、サファイアでは約15%)。従って、成長に用いるバッファ層は、この格子定数差を吸収ないし緩和できるものでなければ、高品質の素子層を安定して製造することはできない。また、単結晶基板と化合物半導体層とは線膨張係数の差が大きいので(特に、絶縁性のサファイア基板を用いた場合)、これに由来した熱応力により、結晶欠陥の発生や成長がより助長されやすい傾向にあるので、注意が必要である。
【0006】
従来、バッファ層の材料として使用されてきたGaNは、基板との格子定数差が大きいため、バッファ層と基板との境界付近から結晶欠陥が生じやすい傾向にある。他方、AlNは基板との格子定数差はGaNよりも縮小するものの、逆にGaN系化合物系半導体よりなる素子層との格子不整合率が大きくなるので、バッファ層と素子層との境界ないし素子層内に結晶欠陥が生じやすくなる。なお、特許文献2に開示されているように、GaN層とAlN層とが交互に積層されたバッファ層、あるいはGaNとAlNとの混晶よりなるバッファ層を用いる方法も考えられるが、GaNとAlNとの組合せを用いる限り、バッファ層と素子層との格子不整合に由来した結晶欠陥の発生は避け難い。
【0007】
本発明の課題は、バッファ層と素子層との境界において結晶欠陥が発生しにくく、ひいては高品質の素子層を安定的に実現できる半導体素子構造とその製造方法とを提供することにある。
【0008】
【課題を解決するための手段及び作用・効果】
上記の課題を解決するために、本発明の化合物半導体素子は、InGaAl1−x−yN(ただし、0≦x<1、0≦y≦1、0<x+y≦1)よりなる半導体素子層が、層厚方向の少なくとも一部区間がAl1−aInN(aはInN混晶比、0<a<1)よりなるAlInN層とされたバッファ層を介して、単結晶基板上にエピタキシャル成長されてなることを特徴とする。このようなバッファ層を用いて半導体素子層を成長することにより、結晶欠陥密度の低い高品質の素子層を安定的に実現できる。
【0009】
バッファ層中のAlInN層は、半導体素子層との境界側にて単結晶基板との境界側よりもInN混晶比aが大となるように形成することができ、該バッファ層を介して半導体素子層を、SiC、サファイア及びシリコンのいずれかよりなる単結晶基板上にエピタキシャル成長することができる。
【0010】
上記構成によると、SiC、サファイア及びシリコンのいずれかよりなる単結晶基板上にInGaAl1−x−yNにより構成された半導体素子層をヘテロエピタキシャル成長させるに際して、半導体素子層との境界側にて単結晶基板との境界側よりもInN混晶比aが大となるように形成されたAl1−aInN層をバッファ層として用いる。InNはGaNよりも格子定数が大であり、InN混晶比aを調整することにより、GaNやAlN又はそれらを組合せた従来のバッファ層と比較して、半導体素子層との境界側にてバッファ層の格子定数を半導体素子層の格子定数により近づけることができる。その結果、バッファ層と素子層との境界において結晶欠陥が発生しにくくなり、ひいては高品質の素子層を安定的に実現できる。特に、SiC単結晶基板を用いる場合は、バッファ層の基板側InN混晶比aを減ずることで、単結晶基板との格子定数差も効果的に縮小できる。
【0011】
InGaAl1−x−yNよりなる半導体素子層は、InN混晶比x、GaN混晶比y及びAlN混晶比1−x−yの調整により、格子定数とバンドギャップエネルギーとを所望の値に調整可能である。例えばGaN系化合物を用いたHEMT構造においては、二次元電子ガス層形成のため、n型にドープしたGaAlN電子供給層に、GaNチャネル層をヘテロ接合したものが多く試みられている。また、電子供給層は、さらにGaNチャネル層との格子整合性を高めるために、InGaAlN層として形成されることもある。
【0012】
半導体素子層が、GaNとの格子定数差が±1%以内となるように、InN混晶比x、GaN混晶比y及びAlN混晶比1−x−yが調整されたものである場合(例えば、GaNチャネル層の場合はy=1、x=0である)、バッファ層中のAlInN層は、半導体素子層との境界を含む部分が、InN混晶比aが0.1以上0.25以下に調整されたAl1−aInNよりなるものとすることで、当該境界にて半導体素子層と格子定数を略一致させることができる。これにより、バッファ層と半導体素子層との境界付近での結晶欠陥発生をより効果的に防止できる。
【0013】
バッファ層中のAlInN層は、単結晶基板側の境界から半導体素子層側の境界に向けて、InN混晶比aが段階的(好ましくは3段階以上)又は連続的に増加するものとして形成することが望ましい。このようにすると、バッファ層は層厚方向において、単結晶基板側から半導体素子層側に向けて格子定数が漸増し、格子定数が途中で不連続に大きく増加することがない。その結果、バッファ層の層厚方向の特定位置に格子定数変化に基づく応力が集中しにくくなり、結晶欠陥発生をより効果的に防止することができる。
【0014】
なお,本発明においては、半導体素子層の結晶性を改善するためにAlInN層を有するバッファ層を使用することもできる。この場合、AlInN層は非晶質であってもよい。
【0015】
また、本発明の化合物半導体素子の製造方法は、
単結晶基板上に、層厚方向の少なくとも一部区間がAl1−aInN(aはInN混晶比、0<a<1)よりなるAlInN層とされたバッファ層をエピタキシャル成長する工程と、
InGaAl1−x−yN(ただし、0≦x<1、0≦y≦1、0<x+y≦1)よりなる半導体素子層を、バッファ層上にエピタキシャル成長する工程と、
を含むことを特徴とする。このようなバッファ層を用いて半導体素子層を成長することにより、結晶欠陥密度の低い高品質の素子層を有した化合物半導体素子を簡便かつ安定的に製造できる。
【0016】
【発明の実施の形態】
図1は、本発明の半導体素子をHEMTとして構成した例を示す。該HEMT200は、SiCからなる単結晶基板101上に、バッファ層102を介して、半導体素子層103を、MOVPE法を用いたヘテロエピタキシャル成長法により形成したものである。なお、単結晶基板101は、SiC基板に代えてサファイア基板あるいはシリコン基板を用いてもよい。
【0017】
半導体素子層103は、バッファ層102に近い側から、ノンドープのGaNチャネル層119、ノンドープのGaAlNスペーサ層105、Si等によりn型にドープされたGaAlN電子供給層110、電極とのコンタクト層として機能するn型GaN層111がこの順序にて積層されたものである。そして、n型GaN層111上には、ドレイン電極106、ソース電極107が形成され、n型GaN層111の非形成領域に露出するn型GaAlN層110にゲート電極108が形成されている。ドレイン電極106とソース電極107とはn型GaN層111との間でオーミック接合を形成する金属(例えばTi/Al)により、ゲート電極108はn型GaAlN電子供給層110との間でショットキー(Schottky)接合を形成する金属(例えばPd/Au)により、それぞれ構成されている。GaAlNスペーサ層105は、n型GaAlN電子供給層110を成長する際に、すでに形成されているGaNチャネル層119にn型ドーパントであるSi等の不純物が拡散することを防止するためのものである。
【0018】
GaAlNスペーサ層105とGaNチャネル層119との間には、電子移動度の高い二次元電子ガス(2DEG)層が形成される。そして、ドレイン電極106とソース電極107との間に電圧を印加し、ゲート電極108でその電流値を制御しながら、ドレイン電極106とソース電極107との間でGaNチャネル層119を経由した通電を行なうことができる。
【0019】
次に、バッファ層102は、少なくとも該半導体素子層103との境界を含む部分がAl1−aInN(aはInN混晶比、0<a<1)とされ、かつ半導体素子層103との境界側にてSiC単結晶基板101との境界側よりもInN混晶比aが大となるように形成されている。本実施形態においては、図2に示すように、それぞれInN混晶比aがa1,a2,‥,an(ただし、a1<a2<‥<an)とされたAl1−aInNよりなる単位層2−1,2−2,‥,2−nが、基板101側からこの順序に積層されている。これにより、例えば図3に示すように、バッファ層102は、層厚方向においてInN混晶比aが、基板101との境界側での値a1(本実施形態では0である)から半導体素子層103側での値an(本実施形態では0.17である)に向けて、階段状に増加する分布を有したものとなる。なお、単位層の数nは3以上であり、個々の単位層の厚さは例えばバッファ層102の層厚が50nm〜200nmとなるように、単位層の数に応じて適宜定められる。
【0020】
以下、上記のHEMT200の製造方法について説明する。バッファ層102及び半導体素子層103の形成は、公知のMOVPE法あるいはMBE(Molecular Beam Epitaxy)法を用いた気相成長法により行なうことができる。MOVPE法を採用する場合、原料ガスとしては次のようなものを用いることができる。・Ga源:トリメチルガリウム(TMGa)、トリエチルガリウム(TEGa)など
・In源:トリメチルインジウム(TMIn)、トリエチルインジウム(TEIn)など。
・Al源;トリメチルアルミニウム(TMAl)、トリエチルアルミニウム(TEAl)など;
・N源:アンモニア(NH)など。
また、p型ドーパント源及びn型ドーパント源となるドーパントガスは、以下のものが使用可能である。
・Mg源:ビスシクロペンタジエニルマグネシウム(CpMg)など。
・Si源:シランなどのシリコン水素化物など;
なお、本実施例においては、ドーパント元素としてSiおよびMgを採用しているが、n型ドーパントとしてC、Ge、SnなどのIV族元素を、p型ドーパントとしてCa、Sr、ZnなどのII族元素を用いることができる。
上記の各原料ガスは、キャリアガス(例えば窒素ガス)により適度に希釈した形で、基板101を配置した反応容器内に供給される。
【0021】
具体的には、SiC単結晶基板(結晶主軸が[0001]のもの)1の主表面上に、図2に示すバッファ層102を、上記のMOVPE法を用いて成長させる。バッファ層102の各単位層2−1,2−2,‥,2−nは、InN混晶比aの違いに応じて、層毎にIn源及びAl源となる有機金属ガスの流量比を、マスフローコントローラ等により段階的に変化するように制御する。なお、バッファ層102の少なくとも最初の1層ないし複数層は、多結晶層あるいはアモルファス層となっていてもよい。また、バッファ層102の最後の1層ないし複数の単位層は、半導体素子層103のエピタキシャル成長に適した単結晶となっていることが望ましい(単位層は、形成を繰り返す毎に結晶性が順次向上する)。
【0022】
結晶性改善の観点から、InNは比較的低温での成長(例えば400℃以上900℃以下)が望ましいとされ、AlNは逆に比較的高温での成長(例えば900℃以上1100℃以下)が望ましいとされている。従って、両者の混晶よりなるバッファ層2は、その中間の温度域である500℃以上1000℃以下で成長を行なうことが望ましい。
【0023】
次に、バッファ層102の形成が終了すれば、反応容器内にて引き続き、原料ガス及びドーパントガスとなる有機金属ガスの流量比を層毎に調整することにより、GaNチャネル層119、GaAlNスペーサ層105、GaAlN電子供給層110及びn型GaN層111を順次エピタキシャル成長させる。その後、n型GaN層111の一部をフォトリソグラフィー等により一部除去し、露出したGaAlN電子供給層110にゲート電極108を、また、残留したn型GaN層111上にドレイン電極106及びソース電極107を形成する。その後、基板101とともにダイシングしてチップとなし、各電極に導通するリードフレームとともに樹脂モールドすることにより、最終的なHEMT200となる。
【0024】
上記方法により得られるHEMT200は、半導体素子層103が、GaNとの格子定数差が±1%以内のInGaAl1−x−yNにより構成されている。そして、バッファ層102は、該半導体素子層103と接する単位層2−n(図2)が、InN混晶比aが0.1以上0.25以下のAl1−aInNよりなる。該単位層2−nは、半導体素子層103と格子定数が略一致するものとり、バッファ層102と半導体素子層103との境界付近での結晶欠陥発生を効果的に防止できる。また、バッファ層102のSiC単結晶基板101と接する単位層2−1(図2)を、InN混晶比aが0のAl1−aInN、すなわちAlN層とすることで、SiC単結晶基板101との格子定数差が縮小し、ひいては、SiC単結晶基板101との境界付近において結晶欠陥が発生することを効果的に抑制できる。
【0025】
以下、本発明の種々の変形例について説明する。
バッファ層102のInN混晶比aは、図4に示すように、層厚方向において連続的に変化するものとしてもよい。このようなバッファ層102を形成するには、MOVPE法による成長時に、In源及びAl源となる有機金属ガスの流量比を、マスフローコントローラ等により連続的に変化するように制御すればよい。
【0026】
また、バッファ層102は、図5に示すように、基板(単結晶基板)との境界近傍におけるInN混晶比をa1とし、半導体素子層との境界近傍におけるInN混晶比をan(ただし、an>a1)として、層厚方向のInN混晶比aの分布が、an−a1よりも小さい変動幅にて増加と減少とを繰り返しながら、単結晶基板側から半導体素子層側に向けて増加傾向を示すものとなるように形成することもできる。半導体素子層側に向けて、先行する層上に、それよりもInN混晶比の高い層を形成すると、InN混晶比の増分だけ格子定数が拡大するので、先行する層にはある程度強い引張応力が作用する。この引張応力レベルが高いと、隣接する層間にてクラックや剥離などの結晶欠陥を生じやすくなる。そこで、InN混晶比の高い層を形成したあと、該層上に格子定数の縮小した低InN混晶比の層を成長すれば、該層による圧縮応力により、先の高InN混晶比の層による引張応力が相殺され、層間での結晶欠陥の発生をより生じにくくすることができる。図5のバッファ層は、具体的には、各々InN混晶比が一定の複数の単位層が、半導体素子層側に向けて、InN混晶比が交互に増減を繰り返す形で積層された構造となっている。
【0027】
また、上記実施形態においてバッファ層2は、いずれも基板101との境界近傍がAlNとなっている以外は、そのほぼ全体がAlInN層として構成され、かつ該AlInN層が、半導体素子層と接して配置されていたが、図6に示すように、バッファ層は、AlInN層と半導体素子層との間に、GaN層と、InGaAlN層とが交互に積層された補助層を有するものとして形成することもできる。これにより、半導体素子層に、基板との格子不整合に由来した結晶欠陥が発生する不具合をより効果的に防止することができる。
【0028】
以上説明した実施形態では、化合物半導体素子をHEMTとして構成したが、それ以外の超高速トランジスタ、例えばMESFET(Metal−Semiconductor Field Effect Transistor)やHBT(Hetero Bipolar Transistor)などにも本発明を適用することもできる。さらに、化合物半導体素子を、図7に示すような発光素子として構成することもできる。該発光素子1(要部の模式断面にて示す)は、単結晶基板としてのサファイア基板(以下、単に基板ともいう)1上にバッファ層2を介して、InGaAl1−x−yN(ただし、0≦x<1、0≦y≦1、0<x+y≦1)よりなる半導体素子層50を形成したものである。このバッファ層2は、図2、図3、図4あるいは図5に示したバッファ層102と同様に構成されるものである。半導体素子層50の要部をなすのは、InGaAl1−a−bN活性層(ノンドープ)5を、p型InGaAl1−x−yNクラッド層(p型ドーパントは例えばMg:以下、p型クラッド層ともいう)6及びn型InGaAl1−x−yN層(n型ドーパントは例えばSi:以下、n型クラッド層ともいう)4にて挟み込んだダブルへテロ構造よりなる発光層部24である。p型クラッド層6及びn型クラッド層4は、本実施形態ではAlNを含有するものとされ、GaN活性層5に対して該活性層5へのキャリア閉じ込めに有利に作用するポテンシャル障壁を形成している。
【0029】
なお、本実施形態ではp型クラッド層6側から光が取り出されるようになっており、p型クラッド層6上には、該p型クラッド層6よりもp型ドーパント濃度の高い電流拡散層(例えばGaNよりなる:半導体素子層50の一部をなすものとみなす)7が形成され、電流拡散層7上に発光駆動用の電極9が設けられている。他方、バッファ層2とn型クラッド層4との間には、n型クラッド層4よりもn型ドーパント濃度の高い裏面低抵抗層(例えばGaNよりなる:半導体素子層50の一部をなすものとみなす)3が配置されている。裏面低抵抗層3は、基板1の主表面上にて発光層部24の面内方向外側に延出し、その延出領域に、発光駆動用の電極15が設けられている。
【0030】
また、図7の発光素子100においては、サファイア基板1が素子構造の一部として取り込まれる形となっているが、絶縁性のサファイア基板1を剥離して、発光層部の剥離面側に電極形成した素子構造とすることもできる。
【0031】
また、サファイア基板1に代えてSiC基板を用いてもよい。SiC基板は導電性が高いので、裏面低抵抗層3を省略する一方、SiC基板の裏面に電極15を設け、SiC基板の厚さ方向に導通経路を形成する形で発光駆動のための通電を行なうことが可能である。
【図面の簡単な説明】
【図1】本発明の化合物半導体素子の一例であるHEMTを模式的に示す断面図。
【図2】図1のHEMTの、バッファ層の詳細を示す模式断面図。
【図3】図2のバッファ層の、InN混晶比の層厚方向分布を示す模式図。
【図4】バッファ層のInN混晶比の、層厚方向分布の第一変形例を示す模式図。
【図5】バッファ層のInN混晶比の、層厚方向分布の第二変形例を示す模式図。
【図6】バッファ層のさらに別の変形例を示す模式図。
【図7】本発明の化合物半導体素子の別例である発光素子を模式的に示す断面図。
【符号の説明】
1 サファイア基板(単結晶基板)
2 バッファ層
50,103 半導体素子層
100 発光素子(化合物半導体素子)
101 SiC単結晶基板
200 HEMT(化合物半導体素子)
[0001]
TECHNICAL FIELD OF THE INVENTION
The present invention relates to a compound semiconductor device and a method for manufacturing the same.
[0002]
[Prior art]
[Patent Document 1]
JP-A-5-110138 [Patent Document 2]
JP-A-5-206513
As is well known, a multi-layer structure of a compound semiconductor is applied to ultra-high-speed transistors such as MESFET (Metal-Semiconductor Field Transistor) and HEMT (High Electron Mobility Transistor), and light-emitting elements such as light-emitting diodes and lasers. Has been earned. As a semiconductor multilayer structure that has been receiving attention in recent years, there is a heterojunction structure using a GaN-based compound semiconductor. GaN-based compound semiconductors can be changed in bandgap at room temperature from 2.0 eV to 6.2 eV and are chemically stable, so that they are applied to light-emitting elements such as blue light and are becoming popular. In addition, the GaN-based compound-based semiconductor has a wide band gap, high electron mobility, and easy heterojunction formation, so that it can be operated in a high-temperature environment, and has a higher speed and higher output. Its application to next-generation ultra-high-speed transistors has also attracted attention and has been studied.
[0004]
Unlike a GaAs-based compound, it is difficult to manufacture a semi-insulating single-crystal substrate that enables homoepitaxial growth of a GaN-based compound-based semiconductor. Single crystal substrates and sapphire (single crystal alumina) substrates are used. At this time, GaN (Patent Document 1) or AlN is grown as a buffer layer on a single crystal substrate, and then the element layer is heteroepitaxially grown to improve the quality of the element layer.
[0005]
[Problems to be solved by the invention]
In heteroepitaxial growth of a GaN-based compound semiconductor, the lattice constant difference between GaN and SiC or sapphire used as a single crystal substrate is very large (about 5% for SiC and about 15% for sapphire). Therefore, a high-quality device layer cannot be stably manufactured unless the buffer layer used for growth can absorb or reduce the lattice constant difference. In addition, since the difference in linear expansion coefficient between the single crystal substrate and the compound semiconductor layer is large (especially when an insulating sapphire substrate is used), the generation and growth of crystal defects are further promoted by the thermal stress derived from this. Care must be taken, as they tend to be susceptible.
[0006]
Conventionally, GaN, which has been used as a material for the buffer layer, has a large lattice constant difference from the substrate, so that crystal defects tend to occur near the boundary between the buffer layer and the substrate. On the other hand, although the lattice constant difference between AlN and the substrate is smaller than that of GaN, the lattice mismatch ratio between the AlN and the element layer made of a GaN-based compound semiconductor increases. Crystal defects easily occur in the layer. As disclosed in Patent Document 2, a method using a buffer layer in which a GaN layer and an AlN layer are alternately stacked or a buffer layer made of a mixed crystal of GaN and AlN is also conceivable. As long as the combination with AlN is used, generation of crystal defects due to lattice mismatch between the buffer layer and the element layer is inevitable.
[0007]
An object of the present invention is to provide a semiconductor device structure and a method of manufacturing the same, which are less likely to generate crystal defects at the boundary between the buffer layer and the device layer, and can stably realize a high-quality device layer.
[0008]
[Means for Solving the Problems and Functions / Effects]
In order to solve the above problems, a compound semiconductor device of the present invention, from the In x Ga y Al 1-x -y N ( However, 0 ≦ x <1,0 ≦ y ≦ 1,0 <x + y ≦ 1) comprising a semiconductor element layer is at least partially interval Al 1-a in a N layer thickness direction (a is InN mixed crystal ratio, 0 <a <1) via a buffer layer and AlInN layer made of a single It is characterized by being epitaxially grown on a crystal substrate. By growing a semiconductor element layer using such a buffer layer, a high-quality element layer having a low crystal defect density can be stably realized.
[0009]
The AlInN layer in the buffer layer can be formed so that the InN mixed crystal ratio a is larger at the boundary side with the semiconductor element layer than at the boundary side with the single crystal substrate, and the semiconductor layer is formed via the buffer layer. The element layer can be epitaxially grown on a single crystal substrate made of any of SiC, sapphire, and silicon.
[0010]
According to the above configuration, SiC, when to hetero-epitaxially growing a semiconductor element layer formed of sapphire and an In x Ga either become more single crystal substrate of silicon y Al 1-x-y N , the boundary between the semiconductor element layer The Al 1-a In a N layer formed so that the InN mixed crystal ratio a is higher on the side than on the boundary side with the single crystal substrate is used as a buffer layer. InN has a larger lattice constant than GaN, and the InN mixed crystal ratio a is adjusted to make the buffer at the boundary side with the semiconductor element layer, as compared with the conventional buffer layer of GaN, AlN, or a combination thereof. The lattice constant of the layer can be made closer to the lattice constant of the semiconductor element layer. As a result, crystal defects hardly occur at the boundary between the buffer layer and the element layer, and a high-quality element layer can be stably realized. In particular, when a SiC single crystal substrate is used, the difference in lattice constant between the buffer layer and the single crystal substrate can be effectively reduced by reducing the substrate side InN mixed crystal ratio a.
[0011]
In x Ga y Al 1-x -y N semiconductor device layer of the, InN mixed crystal ratio x, by adjusting the GaN mole fraction y and AlN mixed crystal ratio 1-x-y, the lattice constant and band gap energy Can be adjusted to a desired value. For example, in a HEMT structure using a GaN-based compound, many attempts have been made to form a two-dimensional electron gas layer by hetero-junctioning a GaN channel layer with an n-type doped GaAlN electron supply layer. Further, the electron supply layer may be formed as an InGaAlN layer in order to further improve lattice matching with the GaN channel layer.
[0012]
In the case where the semiconductor element layer has an InN mixed crystal ratio x, a GaN mixed crystal ratio y, and an AlN mixed crystal ratio 1-xy adjusted such that the lattice constant difference from GaN is within ± 1%. (For example, in the case of a GaN channel layer, y = 1 and x = 0). In the AlInN layer in the buffer layer, the portion including the boundary with the semiconductor element layer has an InN mixed crystal ratio a of 0.1 or more and 0 or less. By using Al 1-a In a N adjusted to be .25 or less, the semiconductor element layer and the lattice constant can be substantially matched at the boundary. As a result, generation of crystal defects near the boundary between the buffer layer and the semiconductor element layer can be more effectively prevented.
[0013]
The AlInN layer in the buffer layer is formed such that the InN mixed crystal ratio a increases stepwise (preferably three or more steps) or continuously from the boundary on the single crystal substrate side to the boundary on the semiconductor element layer side. It is desirable. By doing so, the lattice constant of the buffer layer gradually increases from the single crystal substrate side to the semiconductor element layer side in the layer thickness direction, and the lattice constant does not increase discontinuously largely in the middle. As a result, stress based on a change in lattice constant hardly concentrates at a specific position in the thickness direction of the buffer layer, and the occurrence of crystal defects can be more effectively prevented.
[0014]
In the present invention, a buffer layer having an AlInN layer can be used to improve the crystallinity of the semiconductor element layer. In this case, the AlInN layer may be amorphous.
[0015]
Further, the method of manufacturing a compound semiconductor device of the present invention,
Epitaxially growing a buffer layer on the single crystal substrate, the buffer layer being an AlInN layer in which at least a part of the layer thickness direction is Al 1-a In a N (a is an InN mixed crystal ratio, 0 <a <1). ,
In x Ga y Al 1-x -y N ( However, 0 ≦ x <1,0 ≦ y ≦ 1,0 <x + y ≦ 1) semiconductor element layer consisting of the steps of epitaxially grown on the buffer layer,
It is characterized by including. By growing a semiconductor element layer using such a buffer layer, a compound semiconductor element having a high-quality element layer with a low crystal defect density can be easily and stably manufactured.
[0016]
BEST MODE FOR CARRYING OUT THE INVENTION
FIG. 1 shows an example in which the semiconductor device of the present invention is configured as a HEMT. In the HEMT 200, a semiconductor element layer 103 is formed on a single crystal substrate 101 made of SiC via a buffer layer 102 by a heteroepitaxial growth method using a MOVPE method. Note that the single crystal substrate 101 may be a sapphire substrate or a silicon substrate instead of the SiC substrate.
[0017]
The semiconductor element layer 103 functions as a non-doped GaN channel layer 119, a non-doped GaAlN spacer layer 105, a GaAlN electron supply layer 110 doped n-type with Si or the like, and a contact layer with an electrode from the side close to the buffer layer 102. The n-type GaN layers 111 are stacked in this order. Then, a drain electrode 106 and a source electrode 107 are formed on the n-type GaN layer 111, and a gate electrode 108 is formed on the n-type GaAlN layer 110 exposed in a region where the n-type GaN layer 111 is not formed. The drain electrode 106 and the source electrode 107 are made of a metal (for example, Ti / Al) that forms an ohmic junction with the n-type GaN layer 111, and the gate electrode 108 is Schottky-connected to the n-type GaAlN electron supply layer 110. (Schottky) junctions are formed of a metal (for example, Pd / Au). The GaAlN spacer layer 105 is for preventing impurities such as Si, which is an n-type dopant, from diffusing into the GaN channel layer 119 that has already been formed when the n-type GaAlN electron supply layer 110 is grown. .
[0018]
A two-dimensional electron gas (2DEG) layer having high electron mobility is formed between the GaAlN spacer layer 105 and the GaN channel layer 119. Then, a voltage is applied between the drain electrode 106 and the source electrode 107, and while the current value is controlled by the gate electrode 108, a current is applied between the drain electrode 106 and the source electrode 107 via the GaN channel layer 119. Can do it.
[0019]
Next, in the buffer layer 102, at least a portion including a boundary with the semiconductor element layer 103 is set to Al 1−a In a N (a is an InN mixed crystal ratio, 0 <a <1), and the semiconductor element layer 103 is formed. Is formed such that the InN mixed crystal ratio a is larger at the boundary side with the SiC single crystal substrate 101 than at the boundary side with the SiC single crystal substrate 101. In the present embodiment, as shown in FIG. 2, the InN mixed crystal ratio a is composed of Al 1-a In a N with a1, a2, ‥, and an (where a1 <a2 <‥ <an). The unit layers 2-1, 2-2,..., 2-n are stacked in this order from the substrate 101 side. Thereby, as shown in FIG. 3, for example, the buffer layer 102 has a semiconductor element layer whose InN mixed crystal ratio a in the layer thickness direction changes from a value a1 (0 in the present embodiment) on the boundary side with the substrate 101. The distribution has a stepwise increasing distribution toward the value an (0.17 in the present embodiment) on the 103 side. The number n of the unit layers is 3 or more, and the thickness of each unit layer is appropriately determined according to the number of the unit layers so that the buffer layer 102 has a thickness of 50 nm to 200 nm, for example.
[0020]
Hereinafter, a method for manufacturing the HEMT 200 will be described. The formation of the buffer layer 102 and the semiconductor element layer 103 can be performed by a known MOVPE method or a vapor phase growth method using an MBE (Molecular Beam Epitaxy) method. When the MOVPE method is employed, the following can be used as a source gas. Ga source: trimethyl gallium (TMGa), triethyl gallium (TEGa), etc. In source: trimethyl indium (TMIn), triethyl indium (TEIn), etc.
-Al source; trimethyl aluminum (TMAl), triethyl aluminum (TEAl), etc .;
· N source: ammonia (NH 3), such as.
The following can be used as the dopant gas serving as the p-type dopant source and the n-type dopant source.
· Mg source: such as biscyclopentadienyl magnesium (Cp 2 Mg).
-Si source: silicon hydride such as silane;
In this embodiment, Si and Mg are employed as dopant elements, but a group IV element such as C, Ge, and Sn is used as an n-type dopant, and a group II element such as Ca, Sr, and Zn is used as a p-type dopant. Elements can be used.
Each of the above-mentioned source gases is supplied to the inside of the reaction vessel in which the substrate 101 is arranged in a form appropriately diluted with a carrier gas (for example, nitrogen gas).
[0021]
Specifically, buffer layer 102 shown in FIG. 2 is grown on the main surface of SiC single crystal substrate (having a crystal main axis of [0001]) 1 by using the MOVPE method described above. Each of the unit layers 2-1, 2-2,..., 2-n of the buffer layer 102 has a flow rate ratio of an organometallic gas serving as an In source and an Al source for each layer according to the difference in the InN mixed crystal ratio a. , Is controlled by a mass flow controller or the like so as to change stepwise. Note that at least the first one or more layers of the buffer layer 102 may be a polycrystalline layer or an amorphous layer. It is desirable that the last one or more unit layers of the buffer layer 102 be a single crystal suitable for epitaxial growth of the semiconductor element layer 103 (the crystallinity of the unit layer is sequentially improved each time the formation is repeated). Do).
[0022]
From the viewpoint of improving crystallinity, InN is preferably grown at a relatively low temperature (eg, 400 ° C. or more and 900 ° C. or less), and AlN is preferably grown at a relatively high temperature (eg, 900 ° C. or more and 1100 ° C. or less). It has been. Therefore, it is desirable that the buffer layer 2 made of a mixed crystal of the two grows at an intermediate temperature range of 500 ° C. or more and 1000 ° C. or less.
[0023]
Next, when the formation of the buffer layer 102 is completed, the GaN channel layer 119 and the GaAlN spacer layer are continuously adjusted in the reaction vessel by adjusting the flow rate ratio of the source gas and the organic metal gas serving as the dopant gas for each layer. 105, a GaAlN electron supply layer 110 and an n-type GaN layer 111 are sequentially epitaxially grown. Thereafter, part of the n-type GaN layer 111 is partially removed by photolithography or the like, and the gate electrode 108 is formed on the exposed GaAlN electron supply layer 110, and the drain electrode 106 and the source electrode are formed on the remaining n-type GaN layer 111. 107 is formed. Thereafter, dicing is performed with the substrate 101 to form a chip, and resin molding is performed together with a lead frame that is electrically connected to each electrode, thereby forming the final HEMT 200.
[0024]
HEMT200 obtained by the above process, the semiconductor element layer 103, the lattice constant difference between GaN is composed of In x Ga y Al 1-x -y N within 1% ±. Then, the buffer layer 102, the semiconductor element layer 103 and the contact unit layer 2-n (FIG. 2) is, InN mixed crystal ratio a is from 0.1 to 0.25 of Al 1-a In a N. The unit layer 2-n has a lattice constant substantially equal to that of the semiconductor element layer 103, and can effectively prevent generation of crystal defects near a boundary between the buffer layer 102 and the semiconductor element layer 103. Also, the unit layer 2-1 (FIG. 2) of the buffer layer 102 which is in contact with the SiC single crystal substrate 101 is made of Al 1-a In a N having an InN mixed crystal ratio a of 0, that is, an AlN layer. The difference in lattice constant from the crystal substrate 101 is reduced, and the generation of crystal defects near the boundary with the SiC single crystal substrate 101 can be effectively suppressed.
[0025]
Hereinafter, various modifications of the present invention will be described.
As shown in FIG. 4, the InN mixed crystal ratio a of the buffer layer 102 may change continuously in the layer thickness direction. In order to form such a buffer layer 102, the flow ratio of the organometallic gas serving as an In source and an Al source during growth by MOVPE may be controlled by a mass flow controller or the like so as to be continuously changed.
[0026]
As shown in FIG. 5, the buffer layer 102 has an InN mixed crystal ratio near the boundary with the substrate (single crystal substrate) a1 and an InN mixed crystal ratio near the boundary with the semiconductor element layer an (where As an> a1), the distribution of the InN mixed crystal ratio a in the layer thickness direction increases and decreases from the single crystal substrate side toward the semiconductor element layer side while repeatedly increasing and decreasing with a fluctuation width smaller than an-a1. It can also be formed so as to show a tendency. When a layer having a higher InN mixed crystal ratio is formed on the preceding layer toward the semiconductor element layer side, the lattice constant is increased by the increment of the InN mixed crystal ratio. Stress acts. If the tensile stress level is high, crystal defects such as cracks and peeling are likely to occur between adjacent layers. Therefore, after a layer having a high InN mixed crystal ratio is formed, a layer having a reduced lattice constant and a low InN mixed crystal ratio is grown on the layer. The tensile stress due to the layers is offset, and the generation of crystal defects between the layers can be made more difficult. Specifically, the buffer layer in FIG. 5 has a structure in which a plurality of unit layers each having a constant InN mixed crystal ratio are stacked in such a manner that the InN mixed crystal ratio alternately increases and decreases toward the semiconductor element layer side. It has become.
[0027]
In the above embodiment, almost all of the buffer layer 2 is configured as an AlInN layer except that the vicinity of the boundary with the substrate 101 is AlN, and the buffer layer 2 is in contact with the semiconductor element layer. Although arranged, as shown in FIG. 6, the buffer layer should be formed as having an auxiliary layer in which a GaN layer and an InGaAlN layer are alternately stacked between an AlInN layer and a semiconductor element layer. You can also. Thereby, it is possible to more effectively prevent a defect that a crystal defect due to lattice mismatch with the substrate occurs in the semiconductor element layer.
[0028]
In the embodiment described above, the compound semiconductor element is configured as a HEMT. However, the present invention can be applied to other ultra-high-speed transistors, such as a MESFET (Metal-Semiconductor Field Effect Transistor) and an HBT (Hetero Bipolar Transistor). You can also. Further, the compound semiconductor element can be configured as a light emitting element as shown in FIG. The light emitting element 1 (shown in schematic cross-section of a main portion) of a sapphire substrate as a single crystal substrate (hereinafter, simply referred to as a substrate) via a buffer layer 2 on the 1, In x Ga y Al 1 -x- A semiconductor element layer 50 of yN (where 0 ≦ x <1, 0 ≦ y ≦ 1, 0 <x + y ≦ 1) is formed. This buffer layer 2 has the same configuration as the buffer layer 102 shown in FIG. 2, FIG. 3, FIG. 4 or FIG. The forms the main part of the semiconductor element layer 50, In a Ga b Al 1- a-b N active layer (non-doped) 5, p-type In x Ga y Al 1-x -y N cladding layer (p-type dopant for example Mg: hereinafter also referred to as p-type cladding layer) 6 and n-type in x Ga y Al 1-x -y n layer (n-type dopant, for example Si: hereinafter also referred to as n-type cladding layer) sandwich at 4 The light emitting layer portion 24 has a double hetero structure. The p-type cladding layer 6 and the n-type cladding layer 4 are assumed to contain AlN in the present embodiment, and form a potential barrier for the GaN active layer 5 that advantageously acts to confine carriers in the active layer 5. ing.
[0029]
In the present embodiment, light is extracted from the p-type cladding layer 6 side. On the p-type cladding layer 6, a current diffusion layer having a higher p-type dopant concentration than the p-type cladding layer 6 is formed. For example, it is made of GaN: it is regarded as forming a part of the semiconductor element layer 50), and an electrode 9 for driving light emission is provided on the current diffusion layer. On the other hand, between the buffer layer 2 and the n-type cladding layer 4, a backside low-resistance layer having a higher n-type dopant concentration than the n-type cladding layer 4 (for example, made of GaN: a part of the semiconductor element layer 50) 3) are arranged. The back surface low resistance layer 3 extends outward in the in-plane direction of the light emitting layer portion 24 on the main surface of the substrate 1, and a light emitting drive electrode 15 is provided in the extended region.
[0030]
Further, in the light emitting element 100 of FIG. 7, the sapphire substrate 1 is taken in as a part of the element structure. However, the insulating sapphire substrate 1 is peeled off, and an electrode is provided on the peeling surface side of the light emitting layer portion. The formed element structure can also be used.
[0031]
Further, instead of the sapphire substrate 1, a SiC substrate may be used. Since the SiC substrate has high conductivity, the backside low-resistance layer 3 is omitted, while the electrode 15 is provided on the backside of the SiC substrate, and the conduction for light emission drive is performed in such a manner that a conduction path is formed in the thickness direction of the SiC substrate. It is possible to do.
[Brief description of the drawings]
FIG. 1 is a cross-sectional view schematically showing a HEMT which is an example of a compound semiconductor device of the present invention.
FIG. 2 is a schematic cross-sectional view showing details of a buffer layer of the HEMT of FIG. 1;
FIG. 3 is a schematic diagram showing the distribution of the InN mixed crystal ratio in the thickness direction of the buffer layer of FIG. 2;
FIG. 4 is a schematic diagram showing a first modification of the distribution of the InN mixed crystal ratio of the buffer layer in the layer thickness direction.
FIG. 5 is a schematic diagram showing a second modification of the distribution of the InN mixed crystal ratio in the buffer layer in the thickness direction of the buffer layer.
FIG. 6 is a schematic view showing still another modified example of the buffer layer.
FIG. 7 is a cross-sectional view schematically showing a light-emitting element which is another example of the compound semiconductor element of the present invention.
[Explanation of symbols]
1 Sapphire substrate (single crystal substrate)
2 Buffer layers 50 and 103 Semiconductor element layer 100 Light emitting element (compound semiconductor element)
101 SiC single crystal substrate 200 HEMT (compound semiconductor device)

Claims (6)

InGaAl1−x−yN(ただし、0≦x<1、0≦y≦1、0<x+y≦1)よりなる半導体素子層が、層厚方向の少なくとも一部区間がAl1−aInN(aはInN混晶比、0<a<1)よりなるAlInN層とされたバッファ層を介して、単結晶基板上にエピタキシャル成長されてなることを特徴とする化合物半導体素子。 In x Ga y Al 1-x -y N ( However, 0 ≦ x <1,0 ≦ y ≦ 1,0 <x + y ≦ 1) semiconductor element layer of the at least some sections of the layer thickness direction Al 1 -A In a N (a is an InN mixed crystal ratio, 0 <a <1) A compound semiconductor element which is epitaxially grown on a single crystal substrate via a buffer layer which is an AlInN layer. 前記バッファ層中の前記AlInN層は、前記半導体素子層との境界側にて前記単結晶基板との境界側よりもInN混晶比aが大となるように形成され、該バッファ層を介して前記半導体素子層が、SiC、サファイア及びシリコンのいずれかよりなる前記単結晶基板上にエピタキシャル成長されてなることを特徴とする請求項1記載の化合物半導体素子。The AlInN layer in the buffer layer is formed such that the InN mixed crystal ratio a is larger on the boundary side with the semiconductor element layer than on the boundary side with the single crystal substrate, and through the buffer layer. 2. The compound semiconductor device according to claim 1, wherein said semiconductor device layer is epitaxially grown on said single crystal substrate made of one of SiC, sapphire and silicon. 前記半導体素子層は、GaNとの格子定数差が±1%以内となるように、InN混晶比x、GaN混晶比y及びAlN混晶比1−x−yが調整されたものであり、
バッファ層中の前記AlInN層は、前記半導体素子層との境界を含む部分が、前記InN混晶比aが0.1以上0.25以下に調整されたAl1−aInNよりなることを特徴とする請求項2記載の化合物半導体素子。
The semiconductor element layer has an InN mixed crystal ratio x, a GaN mixed crystal ratio y, and an AlN mixed crystal ratio 1-xy adjusted so that a lattice constant difference from GaN is within ± 1%. ,
In the AlInN layer in the buffer layer, a portion including a boundary with the semiconductor element layer is made of Al 1-a In a N in which the InN mixed crystal ratio a is adjusted to 0.1 or more and 0.25 or less. The compound semiconductor device according to claim 2, wherein:
バッファ層中の前記AlInN層は、前記単結晶基板側の境界から前記半導体素子層側の境界に向けて、InN混晶比aが段階的又は連続的に増加することを特徴とする請求項2または3に記載の化合物半導体素子。3. The AlInN layer in the buffer layer, wherein the InN mixed crystal ratio a increases stepwise or continuously from the boundary on the single crystal substrate side to the boundary on the semiconductor element layer side. Or the compound semiconductor device according to 3. バッファ層中の前記AlInN層は、前記単結晶基板側の境界近傍におけるInN混晶比をanとし、前記半導体素子層側の境界近傍におけるInN混晶比をa1(ただし、an>a1)として、層厚方向のInN混晶比aの分布が、an−a1よりも小さい変動幅にて増加と減少とを繰り返しながら、前記単結晶基板側から前記半導体素子層側に向けて増加傾向を示すものとなっていることを特徴とする請求項2ないし4のいずれか1項に記載の化合物半導体素子。The AlInN layer in the buffer layer has an InN mixed crystal ratio near the boundary on the single crystal substrate side as an, and an InN mixed crystal ratio near the boundary on the semiconductor element layer side as a1 (where an> a1). The distribution of the InN mixed crystal ratio a in the layer thickness direction shows an increasing tendency from the single crystal substrate side to the semiconductor element layer side while repeatedly increasing and decreasing with a fluctuation width smaller than an-a1. The compound semiconductor device according to any one of claims 2 to 4, wherein 単結晶基板上に、層厚方向の少なくとも一部区間がAl1−aInN(aはInN混晶比、0<a<1)よりなるAlInN層とされたバッファ層をエピタキシャル成長する工程と、
InGaAl1−x−yN(ただし、0≦x<1、0≦y≦1、0<x+y≦1)よりなる半導体素子層を、前記バッファ層上にエピタキシャル成長する工程と、
を含むことを特徴とする化合物半導体素子の製造方法。
Epitaxially growing a buffer layer on the single crystal substrate, wherein at least a part of the layer in the layer thickness direction is an AlInN layer in which Al 1-a In a N (a is an InN mixed crystal ratio, 0 <a <1). ,
In x Ga y Al 1-x -y N ( However, 0 ≦ x <1,0 ≦ y ≦ 1,0 <x + y ≦ 1) and the step of the semiconductor element layer made of epitaxially grown on the buffer layer,
A method for manufacturing a compound semiconductor device, comprising:
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