JPS609174A - Semiconductor device - Google Patents
Semiconductor deviceInfo
- Publication number
- JPS609174A JPS609174A JP11730183A JP11730183A JPS609174A JP S609174 A JPS609174 A JP S609174A JP 11730183 A JP11730183 A JP 11730183A JP 11730183 A JP11730183 A JP 11730183A JP S609174 A JPS609174 A JP S609174A
- Authority
- JP
- Japan
- Prior art keywords
- layer
- schottky barrier
- schottky
- superlattice structure
- ingaas
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
- 239000004065 semiconductor Substances 0.000 title claims abstract description 26
- 150000001875 compounds Chemical class 0.000 claims description 14
- 229910000530 Gallium indium arsenide Inorganic materials 0.000 abstract description 11
- 230000004888 barrier function Effects 0.000 abstract description 11
- 229910001218 Gallium arsenide Inorganic materials 0.000 abstract description 7
- 239000000758 substrate Substances 0.000 abstract description 6
- 239000013078 crystal Substances 0.000 abstract description 3
- 239000002184 metal Substances 0.000 abstract description 2
- 239000010410 layer Substances 0.000 description 22
- 238000010586 diagram Methods 0.000 description 2
- 230000005669 field effect Effects 0.000 description 2
- 240000002329 Inga feuillei Species 0.000 description 1
- 238000010030 laminating Methods 0.000 description 1
- 238000004519 manufacturing process Methods 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 239000002356 single layer Substances 0.000 description 1
- 238000004347 surface barrier Methods 0.000 description 1
- 230000005641 tunneling Effects 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L29/00—Semiconductor devices adapted for rectifying, amplifying, oscillating or switching, or capacitors or resistors with at least one potential-jump barrier or surface barrier, e.g. PN junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof ; Multistep manufacturing processes therefor
- H01L29/66—Types of semiconductor device ; Multistep manufacturing processes therefor
- H01L29/68—Types of semiconductor device ; Multistep manufacturing processes therefor controllable by only the electric current supplied, or only the electric potential applied, to an electrode which does not carry the current to be rectified, amplified or switched
- H01L29/76—Unipolar devices, e.g. field effect transistors
- H01L29/772—Field effect transistors
- H01L29/80—Field effect transistors with field effect produced by a PN or other rectifying junction gate, i.e. potential-jump barrier
- H01L29/802—Field effect transistors with field effect produced by a PN or other rectifying junction gate, i.e. potential-jump barrier with heterojunction gate, e.g. transistors with semiconductor layer acting as gate insulating layer, MIS-like transistors
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L29/00—Semiconductor devices adapted for rectifying, amplifying, oscillating or switching, or capacitors or resistors with at least one potential-jump barrier or surface barrier, e.g. PN junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof ; Multistep manufacturing processes therefor
- H01L29/40—Electrodes ; Multistep manufacturing processes therefor
- H01L29/43—Electrodes ; Multistep manufacturing processes therefor characterised by the materials of which they are formed
- H01L29/47—Schottky barrier electrodes
- H01L29/475—Schottky barrier electrodes on AIII-BV compounds
Abstract
Description
【発明の詳細な説明】
(FI)発明の技術分野
本発明は半導体装置、特に高電子移動度の化合物半導体
層を能動層として用い、またショットキ電極を制御電極
として用いた電界効果型半導体装置に関する。Detailed Description of the Invention (FI) Technical Field of the Invention The present invention relates to a semiconductor device, and particularly to a field effect semiconductor device using a compound semiconductor layer with high electron mobility as an active layer and a Schottky electrode as a control electrode. .
(bl 技術の背景
高速動作可能な素子としてGaAsを用いた電界効果型
トランジスタ(FET)が実用化され、応用分野の拡大
が期待されているが、その動作高速性はGaAsの高電
子移動度に負うところが大きい。更に高い電子移動度を
有する化合物半導体として、InGaAsなどが有望視
されている。(bl Background of the technology) Field-effect transistors (FETs) using GaAs have been put into practical use as devices capable of high-speed operation, and are expected to expand their application fields. InGaAs and the like are seen as promising compound semiconductors with even higher electron mobility.
特にInGa’、AsはInP基板上に格子整合してエ
ピタキシャル成長させる技術が確立しつつあり、実用化
上のyW点は少ない。In particular, a technique for epitaxially growing InGa' and As on an InP substrate with lattice matching is being established, and there are few yW points for practical use.
fc) 従来技術と問題点
I n Q 2ΔSによりFETを製作するうえでの難
点の1つば制御電極(ゲート電極)、にある。Ga71
+、sの場合、特性良好なショットキ接合(バリア高さ
で0.7〜0.8eV)が比較的容易に形成できるのに
対し、I nGaAsでは特性良好なショットキ接合は
得られない。例えば、InP基板と格子整合するI n
o、、、G aOゆgAsの場合、表面準位によってそ
の表面バリアは0.3〜0.4 、e Vに固定され、
即ちピンニング効果を生じてショットキ電極金属の種類
にかかわりなく上記バリア高さのショソトキ接合しか形
成できない。fc) Prior Art and Problems One of the difficulties in manufacturing an FET using I n Q 2ΔS lies in the control electrode (gate electrode). Ga71
+, s, a Schottky junction with good characteristics (barrier height of 0.7 to 0.8 eV) can be formed relatively easily, whereas a Schottky junction with good characteristics cannot be obtained with InGaAs. For example, InP substrate and lattice matching In
In the case of GaO YugAs, its surface barrier is fixed at 0.3-0.4, e V due to the surface states,
That is, a pinning effect occurs, and only a Schottky junction with the above barrier height can be formed regardless of the type of Schottky electrode metal.
そこでInGaAsでEFTを構成するためにはMIS
型構造のゲートを採用することが一般に考えられている
。しかし、SiにおけるMO3型ゲートの如く界面準位
の少ない安定なゲート絶縁膜を得ることばできていす、
実現は難しいものと考えられる。Therefore, in order to configure EFT with InGaAs, MIS
It is generally considered to adopt a gate with a type structure. However, it is possible to obtain a stable gate insulating film with few interface states, such as the MO3 type gate in Si.
It is considered difficult to realize this.
(d) 発明の目的
本発明の目的は、InGaAsの如く、特性良好なショ
ットキ接合を形成するのが困難な化合物半導体を能動層
とする半導体装置において、特性良好なショットキ接合
部の制御電極を実現するための新規な構造を提供するこ
とにある。(d) Purpose of the Invention The purpose of the present invention is to realize a control electrode for a Schottky junction with good characteristics in a semiconductor device whose active layer is a compound semiconductor such as InGaAs, in which it is difficult to form a Schottky junction with good characteristics. The objective is to provide a new structure for
(d) 発明の構成
上記目的は達成するために本発明により提供される半導
体装置は、ショットキ電極から延びる空乏層を第1の化
合物半導体層中に拡げ得る構成を有し、該第1の化合物
半導体層上にば、前記ショットキ電極と接して該第1の
化合物半導体より大きなショットキバリアを形成する第
2の化合物半導体層と第1の化合物半導体層とを繰返し
積層して成る超格子構造が設けられ、前記ショットキ電
極ば該超格子構造におりる第2化合物半導体層表面に接
して設けられていることを特徴とするものである。(d) Structure of the Invention In order to achieve the above object, a semiconductor device provided by the present invention has a structure in which a depletion layer extending from a Schottky electrode can be expanded into a first compound semiconductor layer, A superlattice structure formed by repeatedly laminating a second compound semiconductor layer and a first compound semiconductor layer that is in contact with the Schottky electrode and forms a larger Schottky barrier than the first compound semiconductor is provided on the semiconductor layer. The Schottky electrode is provided in contact with the surface of the second compound semiconductor layer included in the superlattice structure.
([1発明の実施例
第1図は本発明実施例による半導体装置の構造断面を示
す。同図にて1は半絶縁性のInP基板。([1 Embodiment of the Invention] FIG. 1 shows a structural cross section of a semiconductor device according to an embodiment of the invention. In the figure, 1 is a semi-insulating InP substrate.
2はn型1nGaAsJm、3はInGaAstJiと
GaAs薄層とから成る超格子構造、4は制御電極(〕
、;−ト電極)、5.6はソース及びドレイン電極であ
る。半絶縁性InP基板1上のn型InGaAs団はF
ETの能動チャネルを構成する層であり、InPと格子
整合するIn’o嗅Ga〜、峙Asの単結晶のエビクキ
シャル成長層である。超格子構造3におけるInGaA
s層及びGaAs層は夫々単一層厚みは最大で約100
人位に制限し、超格子構造全体で電子力用−ンネリング
を生じない程度の厚さとなるよう、少なくとも各2層以
上の、望ましくは数十層程度の繰返し積層構造とする。2 is an n-type 1nGaAsJm, 3 is a superlattice structure consisting of InGaAstJi and a thin GaAs layer, and 4 is a control electrode ()
, ;-to electrode), and 5.6 are source and drain electrodes. The n-type InGaAs group on the semi-insulating InP substrate 1 is F
This layer constitutes the active channel of ET, and is an evixial growth layer of a single crystal of In'oGa and As, which is lattice-matched to InP. InGaA in superlattice structure 3
The maximum single layer thickness of the S layer and GaAs layer is approximately 100 mm.
The superlattice structure has a repeated laminated structure of at least two or more layers, preferably several tens of layers, so that the thickness is such that the entire superlattice structure does not cause electron tunneling.
InGaAsJFtの組成は能動層と同じでよいが、I
n o−LG a o、tr A sの組成に漸変さ
せてもよい。最上層1はGaAsFiとする。この超格
子構造はノンドープでよく、またn型にドープすること
により、その上に形成されるショットキ接合から内部へ
向う空乏層の拡がり幅を調整することもできる。ショッ
トキ接合を形成する制御電極4は例えばAIである。The composition of InGaAsJFt may be the same as that of the active layer, but I
The composition may be gradually changed to no-LG ao, tr As. The top layer 1 is made of GaAsFi. This superlattice structure may be undoped, and by doping it to n-type, the width of the depletion layer extending inward from the Schottky junction formed thereon can be adjusted. The control electrode 4 forming the Schottky junction is made of AI, for example.
本実施例の如くに形成されたショットキ接合のバンド図
を第2図に示す。同図にて第1図の各部と対応するfl
域には同一符号を付しである。InGaASI’ff1
l 2とGaAs1illは本質的には格子整合しない
が、ミスマツチによる転位発生は超格子構造で緩和され
、特にショットキ接合を形成すべき最−上表面結晶層に
対してはミスマツチの影響が緩和されている。最上表面
はGaAs薄層であり、その表面に(4’<AIF71
1の形成するショットキバリ゛1は0.7〜0.8 e
VというG a A ’s本来のバリアの高さを有す
る。かくして、GaAsに対する特性良好なショットキ
バリアを、InGaAsデバイスに導入することが可能
になる。FIG. 2 shows a band diagram of a Schottky junction formed as in this example. In the figure, fl corresponding to each part in Figure 1
Areas are given the same reference numerals. InGaASI'ff1
Although L2 and GaAs1ill are not essentially lattice matched, the occurrence of dislocations due to mismatch is alleviated by the superlattice structure, and the influence of mismatch is especially alleviated on the uppermost surface crystal layer where a Schottky junction is to be formed. There is. The top surface is a thin layer of GaAs with (4'<AIF71
Schottky burr 1 formed by 1 is 0.7 to 0.8 e
G a A 's original barrier height is V. In this way, it becomes possible to introduce a Schottky barrier with good characteristics against GaAs into an InGaAs device.
第1図実施例におけるオーミック電極5,6は周知の如
く例えばA 11 G eのようなオーミック金属の合
金化して設ければよく、これはシヨy )キ金屈付着前
に行なっておいてよい。As is well known, the ohmic electrodes 5 and 6 in the embodiment shown in FIG. .
(gl 発明の効果
本発明によれば、低ショソトキハリアしが作り得ない半
導体に対して、格子整合はしないが高ショットキバリア
を作り得る半導体を利用することにより、特性良好なシ
ョットキバリアを作成することができ、FET等へ応答
して特性改善効果を達成し得るものである。(gl) Effects of the Invention According to the present invention, a Schottky barrier with good characteristics can be created by using a semiconductor that does not lattice match but can create a high Schottky barrier for a semiconductor that cannot create a low Schottky barrier. It is possible to achieve the characteristic improvement effect in response to FET etc.
第1図は本発明実施例の装置の構造断面図、第2図はそ
のショットキ接合部のバンド図である。
1−・半絶縁性(nP基板
2−n型InGaAs能動層
3−・InGaAsの超格子構造FIG. 1 is a structural sectional view of the device according to the embodiment of the present invention, and FIG. 2 is a band diagram of the Schottky joint. 1- Semi-insulating (nP substrate 2- N-type InGaAs active layer 3- InGaAs superlattice structure
Claims (1)
中に拡げ得る構成を有し、該第1の化合物半導体層上に
は、前記ショットキ電極と接して該第1の化合物半導体
より大きなショソトキハリアを形成する第2の化合物半
導体層と第1の化合物半導体層とを繰返し稍層して成る
超格子構造が設けられ、前記ショットキ電極は該超格子
構造における第2化合物半導体層表面に接して設けられ
ていることを特徴とする半導体装置。It has a structure in which a depletion layer extending from a Schottky electrode can be expanded into a first compound semiconductor, and on the first compound semiconductor layer, in contact with the Schottky electrode, a Schossotchi halia larger than the first compound semiconductor is provided. A superlattice structure is provided in which a second compound semiconductor layer to be formed and a first compound semiconductor layer are repeatedly layered, and the Schottky electrode is provided in contact with a surface of the second compound semiconductor layer in the superlattice structure. A semiconductor device characterized by:
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP11730183A JPS609174A (en) | 1983-06-29 | 1983-06-29 | Semiconductor device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP11730183A JPS609174A (en) | 1983-06-29 | 1983-06-29 | Semiconductor device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS609174A true JPS609174A (en) | 1985-01-18 |
Family
ID=14708362
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP11730183A Pending JPS609174A (en) | 1983-06-29 | 1983-06-29 | Semiconductor device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS609174A (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS61290776A (en) * | 1985-06-14 | 1986-12-20 | アメリカン テレフオン アンド テレグラフ カムパニ− | Semiconductor device |
JPS63116471A (en) * | 1986-11-04 | 1988-05-20 | Sumitomo Electric Ind Ltd | Field effect transistor |
US4796068A (en) * | 1986-04-21 | 1989-01-03 | Hitachi, Ltd. | Semiconductor device having ultrahigh-mobility |
EP0514077A2 (en) * | 1991-05-13 | 1992-11-19 | AT&T Corp. | Article comprising an opto-electronic device |
-
1983
- 1983-06-29 JP JP11730183A patent/JPS609174A/en active Pending
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS61290776A (en) * | 1985-06-14 | 1986-12-20 | アメリカン テレフオン アンド テレグラフ カムパニ− | Semiconductor device |
US4796068A (en) * | 1986-04-21 | 1989-01-03 | Hitachi, Ltd. | Semiconductor device having ultrahigh-mobility |
JPS63116471A (en) * | 1986-11-04 | 1988-05-20 | Sumitomo Electric Ind Ltd | Field effect transistor |
EP0514077A2 (en) * | 1991-05-13 | 1992-11-19 | AT&T Corp. | Article comprising an opto-electronic device |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
JP2804041B2 (en) | Field-effect transistor | |
JPH0312769B2 (en) | ||
JPS609174A (en) | Semiconductor device | |
JP3447438B2 (en) | Field effect transistor | |
JPS61147577A (en) | Complementary semiconductor device | |
JP3094500B2 (en) | Field effect transistor | |
JPS6214105B2 (en) | ||
JPS61268069A (en) | Semiconductor device | |
JPH084140B2 (en) | Field effect transistor | |
JP2661557B2 (en) | Field effect type semiconductor device | |
JP2917719B2 (en) | Field effect transistor | |
JPH025438A (en) | Insulated-gate field-effect transistor | |
JPH0261149B2 (en) | ||
JP2655594B2 (en) | Integrated semiconductor device | |
JP3423812B2 (en) | HEMT device and manufacturing method thereof | |
JP2786208B2 (en) | Semiconductor device | |
JPS63281474A (en) | Semiconductor device | |
JPH03165576A (en) | Quantum fine line semiconductor device and manufacture thereof | |
JPH01225368A (en) | Semiconductor device | |
JPS63188972A (en) | Field-effect transistor | |
JPH02150038A (en) | Modulation-doping field effect transistor | |
JPH04324645A (en) | Semiconductor transistor | |
JPH02265251A (en) | Semiconductor device | |
JPH0485939A (en) | Field effect semiconductor device | |
JPH04142750A (en) | High electron mobility transistor |