JPS62274675A - Manufacture of field-effect transistor - Google Patents

Manufacture of field-effect transistor

Info

Publication number
JPS62274675A
JPS62274675A JP61118336A JP11833686A JPS62274675A JP S62274675 A JPS62274675 A JP S62274675A JP 61118336 A JP61118336 A JP 61118336A JP 11833686 A JP11833686 A JP 11833686A JP S62274675 A JPS62274675 A JP S62274675A
Authority
JP
Japan
Prior art keywords
layer
groove
type
algaas
gaas layer
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
Application number
JP61118336A
Other languages
Japanese (ja)
Inventor
Ryoichi Hirano
良一 平野
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP61118336A priority Critical patent/JPS62274675A/en
Publication of JPS62274675A publication Critical patent/JPS62274675A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D30/00Field-effect transistors [FET]
    • H10D30/40FETs having zero-dimensional [0D], one-dimensional [1D] or two-dimensional [2D] charge carrier gas channels
    • H10D30/47FETs having zero-dimensional [0D], one-dimensional [1D] or two-dimensional [2D] charge carrier gas channels having two-dimensional [2D] charge carrier gas channels, e.g. nanoribbon FETs or high electron mobility transistors [HEMT]
    • H10D30/471High electron mobility transistors [HEMT] or high hole mobility transistors [HHMT]
    • H10D30/475High electron mobility transistors [HEMT] or high hole mobility transistors [HHMT] having wider bandgap layer formed on top of lower bandgap active layer, e.g. undoped barrier HEMTs such as i-AlGaN/GaN HEMTs
    • H10D30/4755High electron mobility transistors [HEMT] or high hole mobility transistors [HHMT] having wider bandgap layer formed on top of lower bandgap active layer, e.g. undoped barrier HEMTs such as i-AlGaN/GaN HEMTs having wide bandgap charge-carrier supplying layers, e.g. modulation doped HEMTs such as n-AlGaAs/GaAs HEMTs
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D64/00Electrodes of devices having potential barriers
    • H10D64/20Electrodes characterised by their shapes, relative sizes or dispositions 
    • H10D64/27Electrodes not carrying the current to be rectified, amplified, oscillated or switched, e.g. gates
    • H10D64/311Gate electrodes for field-effect devices
    • H10D64/411Gate electrodes for field-effect devices for FETs

Landscapes

  • Electrodes Of Semiconductors (AREA)
  • Junction Field-Effect Transistors (AREA)

Abstract

PURPOSE:To specify the gate length not exceeding 0.5mum with excellent evenness and reproducibility by a method wherein a groove with normal mesa type section reaching the N type GaAs layer thereunder is formed on the second AlGaAs layer as the top layer to form a gate metal in the groove and then the second AlGaAs layer is removed. CONSTITUTION:A high purity GaAs layer 2, an N type AlGaAs layer 3, an N type GaAs layer 4 are epitaxially grown on a GaAs substrate to generate 2DEG5 and then the second AlGaAs layer 16 is formed on the N type GaAs layer 4. Next, a mesaetching part 17 is formed and both ends of the second AAlGaAs layer 16 are etched to form ohmic metallic electrodes 6, 7 as well as ohmic metallic diffused layers 8, 9 by heat treatment. Later, a photoresist 18 for masking groove with an opening is formed on the central part of the second AlGaAs layer 16 which is selectively etched to form a groove 19 with so-called normal mesa type section expanding upward.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は、GaAl1IとAj?GaAsとの界面に
形成される2次電子ガス(2DEO’)を利用した電界
効果トランジスタ(FET)の製造方法に関するもので
ある。
[Detailed Description of the Invention] [Industrial Field of Application] The present invention is directed to GaAl1I and Aj? The present invention relates to a method for manufacturing a field effect transistor (FET) using secondary electron gas (2DEO') formed at the interface with GaAs.

〔従来の技術〕[Conventional technology]

第4図(a)〜(e)はそれぞれ従来の2DEC)F’
ETの例を示す断面図で、この2 DEGFETには大
別してプラナ−構造〔第4図(a) 、 (す〕と溝構
造〔第4図(c)〜(e)〕との2種類がある。
Figures 4(a) to (e) are respectively conventional 2DEC)F'
This is a cross-sectional view showing an example of an ET. This 2 DEGFET can be roughly divided into two types: a planar structure [Fig. 4(a), (S)] and a groove structure [Fig. 4(c) to (e)]. be.

第4図(a) K示したものは、図示していない()a
A s基板上に高純度GaA8ftj t、!l l 
n形AlciaAs層!31 + n形GaAs層(4
)を順次エピタキシャル成長させ、2DEG(5)を発
生させ、n形GaAs層(4)の上にオーミック電極(
6) 、 (7)を形成して、オーミック金属拡散層(
8)。
Figure 4 (a) KWhat is shown is not shown ()a
High purity GaA8ftj t on As substrate! l l
N-type AlciaAs layer! 31 + n-type GaAs layer (4
) are sequentially epitaxially grown to generate 2DEG (5), and an ohmic electrode (
6) and (7) to form an ohmic metal diffusion layer (
8).

(9)をそれぞれ形成させ、両オーミック電極+61 
、 (7)の間にゲート電極(11を形成した構造であ
る。
(9) are formed respectively, and both ohmic electrodes +61
, (7) in which a gate electrode (11) is formed.

IE4図(1)) K示すものは、その改良形として、
ゲート電極(10)の下にp形GaAs層u1)を設け
た構造である0 第4図(e)に示すものは、n形GaAs層(4)に設
けた溝(2)内にゲート′社極flolを形成したもの
であるが、溝(功の底はn形GaAs層(4)内に留っ
ている。第4図(d)K示すものは、溝α埠の底がn形
GaAs層(4)とn形AlGaAs層(3)との界面
または更にn形AlGaAs層(3)の中にまで入った
ものである0また、第4図(e)に示すものは、基本構
造であるn形AlGaAs層(3)及びn形GaAs層
(4)の上に、更に、AIGaAa層αぐ及びn形Ga
As N(至)を形成し、n形GaAs層(至)だけを
溝形成構造としている。
IE4 Figure (1)) The one shown in K is an improved version of
The structure shown in FIG. 4(e) has a p-type GaAs layer u1) provided below the gate electrode (10). However, the bottom of the groove (gong) remains within the n-type GaAs layer (4). The interface between the GaAs layer (4) and the n-type AlGaAs layer (3) or even the inside of the n-type AlGaAs layer (3) is shown in FIG. 4(e). Further, on the n-type AlGaAs layer (3) and the n-type GaAs layer (4), an AIGaAa layer α and an n-type GaAs layer
An As N layer is formed, and only the n-type GaAs layer has a groove-forming structure.

2DEGFETの構造としては、このように大別して2
種類存在するが、第4図(a) 、 (1))のプラナ
−構造のものはトランジスタ特性のウェーノー面内での
均一性向上が期待できる反面、エピタキシャル成長層の
層厚と不純物ドーピング量の正確な制御が必要であるこ
とや、トランジスタ特性向上のためにオーミック電極(
6) 、 (7)の間隔を、第4図(0)〜(e)の溝
形成構造のFETに比して狭くしなければならないとい
う製作上の困難性がある。そこで、現在では、第4図(
0)〜(e)に示した溝形成構造のものが比較的多く製
作されている0 次に、最も一般的な第4図(c)の構造のものについて
、その動作を説明する0オーミツク電極(6)。
The structure of 2DEGFET can be roughly divided into 2 types as shown below.
Although there are several types, the planar structure shown in Figures 4(a) and (1) can be expected to improve the uniformity of transistor characteristics within the Wanow plane. Ohmic electrodes (
6) There is a manufacturing difficulty in that the intervals between (7) and (7) must be narrower than in the FETs having the grooved structure shown in FIGS. 4(0) to (e). Therefore, at present, Figure 4 (
Relatively many ohmic electrodes with the groove forming structures shown in 0) to (e) are manufactured.Next, we will explain the operation of the most common structure shown in Fig. 4(c). (6).

(7)に電圧を印加すると、2DEG (5)を通して
電流が流れるが、その際、ゲート電極(11に電圧を印
加すると、ゲート下の2DEG (5)の濃度が変化し
、トランジスタ動作をする0従って、ゲート電柵aOを
形成する溝(2)の深さを調整することKよって、トラ
ンジスタとしての初期電流値を調整し、所望の特性をも
つ2DEGFETを製作することができるものである0
〔発明が解決しようとする問題点〕 従来から2DEGFETとしては前述した理由によりプ
ラナ−形に比べて溝形成構造のものが一般的に製作され
ているが、この構造では、ゲート長Lgをいかに短縮す
るかが最大のポイントとなる0第4図(C)に示した構
造ではゲート長Lgを短縮するため光学露光方式でも最
も狭い線幅(約0.5μm)をねらってパターニングを
行うことが通常行なわれているが、それ以下の線幅を光
学露光方式で得ることはウェーハ面内の均一性、再現性
の上で問題が多い。
When a voltage is applied to (7), a current flows through the 2DEG (5), but at that time, when a voltage is applied to the gate electrode (11), the concentration of the 2DEG (5) under the gate changes, causing a transistor operation. Therefore, by adjusting the depth of the groove (2) forming the gate electric fence aO, the initial current value of the transistor can be adjusted and a 2DEGFET with desired characteristics can be manufactured.
[Problem to be solved by the invention] Conventionally, 2DEGFETs have generally been manufactured with a grooved structure compared to a planar type for the reasons mentioned above. In the structure shown in Figure 4 (C), the most important point is whether the line width is the narrowest (approximately 0.5 μm) even with the optical exposure method in order to shorten the gate length Lg. However, obtaining a line width smaller than this using an optical exposure method has many problems in terms of uniformity and reproducibility within the wafer surface.

又、これ以下の線幅のパターニングを行うためには、電
子ビーム露光(EB)法、集束イオンと−ム(FIB)
法などの方法が現在、研究されているが、装置が大がか
りになること、量童性、などの点で、まだ問題が多いと
いうのが現状である。
In addition, in order to perform patterning with a line width smaller than this, electron beam exposure (EB) method, focused ion beam (FIB) method, etc.
Methods such as the method are currently being researched, but the current situation is that there are still many problems, such as the large scale of the equipment and the complexity.

ゲート長Lgの短縮は、ゲート会ソース間容量Cgsの
減少、遮断周波数f!の上昇、トランスコンダクタンス
g。等の諸特性の改善につながシ、低雑音化および高周
波特性の向上にはゲート長Lgの短縮は重要な技術的ポ
イントである。
A reduction in the gate length Lg results in a reduction in the gate-to-source capacitance Cgs and a reduction in the cutoff frequency f! rise in transconductance g. Shortening the gate length Lg is an important technical point for reducing noise and improving high frequency characteristics.

この発明は上記のような問題点を解消するためになされ
たもので、従来の光学露光方式によっても0.5μm以
下のゲート長を達成できる2DEGFETの製造方法を
提供することを目的とする。
The present invention has been made to solve the above-mentioned problems, and an object of the present invention is to provide a method for manufacturing a 2DEGFET that can achieve a gate length of 0.5 μm or less even by a conventional optical exposure method.

〔問題点を解決するための手段〕[Means for solving problems]

この発明に係る2DEGFETの製造方法では、通常用
いられるn形AlGaAs層とへテロ接合を形成するn
形GaA s層の上にさらに第2のAlGaAs層を形
成し、第2のAJGaAe層((反応律速形エッチャン
トを利用して、下層のn形()aAa層に到達する深さ
まで頭メサ形の溝を形成し、その後、この溝上にゲート
金属を形成し、然る後に、第2のAlGaAs層ツfン
グ除去するものである。
In the method for manufacturing a 2DEGFET according to the present invention, an n
A second AlGaAs layer is further formed on the GaAs layer, and a second AJGaAe layer is formed using a reaction-controlled etchant to a depth that reaches the underlying n-type ()aAa layer. A trench is formed, then a gate metal is formed on the trench, and then the second AlGaAs layer is removed.

〔作用〕[Effect]

この発明においては、上記のような手順〈よって、2D
EGFETを製作することにょシ、ゲート長が最上層の
第2のAIGaAa層上でパターニングを行った線幅よ
シ狭いゲートを再現性よく形成することができ、均一性
のよい2DEGFETを容易に得ることができる。
In this invention, the above procedure (therefore, 2D
When manufacturing an EGFET, a gate whose gate length is narrower than the line width patterned on the topmost second AIGaAa layer can be formed with good reproducibility, and a 2DEGFET with good uniformity can be easily obtained. be able to.

〔実施例〕〔Example〕

第1図はこの発明の一実施例の方法によって製造された
2DE()PETを示す断面図である。以下、従来例と
同一符号は同等部分を示し、その説明は重複を避ける。
FIG. 1 is a sectional view showing 2DE()PET manufactured by the method of one embodiment of the present invention. Hereinafter, the same reference numerals as those in the conventional example indicate equivalent parts, and the description thereof will be avoided from duplication.

この実施例では、n形AIGILAe層(3)上のn形
GaAs層(4)の上に第2のAA’GaAsAlGa
As層α0第2のA#GaAs層αfeK選択エツチン
グによって、その下のn形GaAs層(4)に達する順
メサ形断面形状の溝を形成し、その溝内にゲート金属電
極a〔が形成されている。
In this example, a second AA'GaAsAlGa layer is formed on the n-type GaAs layer (4) on the n-type AIGILAe layer (3).
By selectively etching the As layer α0 and the second A#GaAs layer αfeK, a groove with a normal mesa-shaped cross section reaching the n-type GaAs layer (4) below is formed, and a gate metal electrode a is formed in the groove. ing.

以下、第2図についてこの実施例の製造方法を略述する
。図示を省略したGaAs基板上に高純度()aAe 
FJ t2) * n形A7GaAs層(3) 、 n
形GaAs層(4)を1順次エピタキシャル成長させて
2DEC) (5)を発生させ、n形GaAs M (
4)の上に第2のAIGaAe層σりを形成する〔第2
図(a) 〕o続いて、アイソレーションのためのメサ
エッチング部分αηを形成し〔第2図(b)〕、第2の
AlGaAs層aQの両端部をフッ酸(HF)系、塩酸
(HR)系のエツチング液で選択エツチングして、そこ
ヘオーミツク金属電極[6) 、 (7)を形成し〔第
2ホトレジスト(至)を形成し〔第2図(e) ) 、
これをマスクとして、例えば、ヨウ化カリ(K工):ヨ
ウ素(工2):水(H2O) =226 : 130 
: 200 (重量比)のような反応律速形のエッチャ
ントによる選択エツチングを第2のAlc)aAs層α
呻に施して上方に拡開するいわゆる順メサ形断面形状の
溝α傷を形成する〔第2図(f)〕。
The manufacturing method of this embodiment will be briefly described below with reference to FIG. High purity ()aAe on a GaAs substrate (not shown)
FJ t2) * n-type A7GaAs layer (3), n
The n-type GaAs layer (4) is epitaxially grown one after another to generate 2DEC) (5), and the n-type GaAs M (
4) Form a second AIGaAe layer σ on top of [Second
[Fig. 2 (a)] o Next, a mesa etching portion αη for isolation is formed [Fig. 2 (b)], and both ends of the second AlGaAs layer aQ are etched with hydrofluoric acid (HF) and hydrochloric acid (HR). ) selective etching with an etching solution to form micrometal electrodes [6) and (7) thereon, and then form a second photoresist (Fig. 2(e)).
Using this as a mask, for example, potassium iodide (K): iodine (2): water (H2O) = 226: 130
: 200 (weight ratio) by selectively etching the second Alc)aAs layer α with a reaction rate-limiting etchant such as
A groove α wound with a so-called mesa-shaped cross section that expands upward is formed by applying it to the groove [FIG. 2(f)].

このエッチャントは、室温(25°C)において、Ga
Asに対し、3×10μm/分、AII o 、 3G
a o 、7A8に対し1μm/分のエツチング速度を
有し、GaAsとAIo、30a。、7Asとのエツチ
ング速度の比は1:30となっている。従ってAlGa
AsをGaAsに対して選択的にエツチングすることが
できる。又、(100)表面のC)aA8基板上の<o
i l>方向のストライプ溝のエツチング断面形状は表
面と54.7°の角度をもつ、いわゆる順メサ形となる
。従って、このエツチング液は選択エツチング液でじか
も、順メサ形断面を有しているという点から、AIG&
Aθ層αQのメサエッチングに好適でろる0 この方法によれば、順メサ形の溝断面の傾斜を利用する
ことによって、表面におけるマスク幅が0.5μmであ
っても、Al()aAe層σQを経てn形GaAe層(
4)に接する溝底の幅を0.5μm以下に絞ることがで
き、しかも、この溝底の幅の再現性は良好であるという
特長をもつ。また、n形GaA s層(4)をエツチン
グ溝のストッパーとして使用しているので、溝形成時に
電流調整を行って溝の深さを制御する必要はなく、かつ
、高度ドライエツチング技術を使用しなくても容易に再
現性及びウエーノ・内の均一性に優れたエツチング溝が
形成できる。
This etchant is a Ga
For As, 3 × 10 μm/min, AII o, 3G
ao, with an etching rate of 1 μm/min for 7A8, GaAs and AIo, 30a. , 7As, the etching rate ratio is 1:30. Therefore, AlGa
As can be selectively etched relative to GaAs. Also, <o on C) aA8 substrate with (100) surface
The etched cross-sectional shape of the stripe groove in the i l direction is a so-called forward mesa shape having an angle of 54.7° with the surface. Therefore, since this etching solution is a selective etching solution and has a normal mesa-shaped cross section,
This method is suitable for mesa etching of the Aθ layer αQ. By utilizing the slope of the mesa-shaped groove cross section, even if the mask width at the surface is 0.5 μm, the Al()aAe layer σQ through the n-type GaAe layer (
4) The width of the groove bottom in contact with the groove bottom can be narrowed down to 0.5 μm or less, and the reproducibility of the width of the groove bottom is good. Furthermore, since the n-type GaAs layer (4) is used as a stopper for the etching groove, there is no need to adjust the current to control the depth of the groove when forming the groove, and advanced dry etching technology is used. Etching grooves with excellent reproducibility and uniformity within the wafer can be easily formed even without the use of etching grooves.

次に、溝形成用ホトレジスト(ト)を除去して〔第2図
(ω〕、改めて中央開孔の大きいゲート電極形成用ホト
レジスト(1)を形成し〔第2図(h)〕、このホトレ
ジスト(1)をマスクとして、上記mαα上上ショット
キーゲート金属α1を形成し〔第2図(i)〕、その後
に、ゲート電極形成用ホトレジストwを除去し〔第2図
(j)〕、更に、第2のAlGaAs層αQを除去して
、この実施例の2DEGFETが完成する〔第2図(k
)〕。
Next, the groove forming photoresist (g) is removed [Fig. 2 (ω)], and a gate electrode forming photoresist (1) with a large central opening is formed again [Fig. 2 (h)]. Using (1) as a mask, an upper Schottky gate metal α1 is formed on the mαα [FIG. 2(i)], and then the photoresist w for gate electrode formation is removed [FIG. 2(j)], and then , the second AlGaAs layer αQ is removed to complete the 2DEGFET of this example [Fig.
)].

以上のように、この実施例方法による2DEGFETで
はn形GaA s層(4)に接するゲート金属α■の@
(ゲート長)は、最上層の第2のA/GaAs層αQの
膜厚と溝形成用ホトレジスト(至)のストライプ状開口
幅とで決っており、サイドエツチング量は少なく、上記
ホトレジスト(至)のストライプ状開口幅より小さい0
.5μm以下の寸法を再現性よく実現できる0なお、上
記実施例では、オーミック抵抗低減のために、オーミッ
ク金属+6) 、 (7)の下第2のAlGaAs層α
Gを除去する場合を示したが、オーミック抵抗を特に低
下させる必要のない場合には、第3図に断面図で示す他
の例のように、オーミック金属(6)。
As described above, in the 2DEGFET according to this embodiment method, the gate metal α■ in contact with the n-type GaAs layer (4) is
The (gate length) is determined by the film thickness of the second A/GaAs layer αQ on the top layer and the striped opening width of the trench-forming photoresist. 0 smaller than the striped opening width of
.. In the above example, in order to reduce ohmic resistance, the lower second AlGaAs layer α of ohmic metal +6), (7)
Although the case where G is removed is shown, if there is no need to particularly reduce the ohmic resistance, use the ohmic metal (6) as in another example shown in the cross-sectional view in FIG.

(7)の下に第2のAIGaAe層0Qを残しておいて
もよい。
The second AIGaAe layer 0Q may be left under (7).

〔発明の効果〕〔Effect of the invention〕

以上のように、この発明に係る2DEOFETの製造方
法では最上層の第2のAl()aAe層に順メサ形断面
の溝をその下のn形GaAs層に達するように形成しこ
の溝内にゲート金属を形成し、その後に第2のAgGa
As層を除去するようにしたので、通常の光学的写真天
版法で上記溝形成のためのレジストパターンを0.5μ
m程度の幅に形成しても、当該溝底の幅で決定されるゲ
ート長は均一性、再現性よく0・5能である。
As described above, in the method for manufacturing a 2DEOFET according to the present invention, a groove with a normal mesa-shaped cross section is formed in the second Al()aAe layer as the uppermost layer so as to reach the n-type GaAs layer below. Form gate metal followed by second AgGa
Since the As layer was removed, the resist pattern for forming the grooves was formed with a thickness of 0.5 μm using a normal optical photolithography method.
Even when formed to a width of about m, the gate length determined by the width of the groove bottom has good uniformity and reproducibility of 0.5.

【図面の簡単な説明】[Brief explanation of drawings]

第1図はこの発明の一実施例方法によって製作された2
DEC)PETの構成を示す断面図、第2図はこの実施
例の製造方法の各過程における状態を示す断面図、第3
図はこの発明の方法で製作された2I)EGFE’I’
の他の例の構成を示す断面図、第4図は従来の2DEG
FETの構成例を示す断面図である。 図において、(2)は高純度GaAs層、(3)はn形
の第1のAlGaAs層、(4)はn形GaAe層、(
5)は2次元電子ガス、顛はゲート金属、(lは第2の
AlGaAs層、α偵は順メサ形溝である。 なお、図中同一符号は同一または相当部分を示す0
FIG. 1 shows a 2
Figure 2 is a cross-sectional view showing the structure of DEC) PET; Figure 2 is a cross-sectional view showing the states at each step of the manufacturing method of this example;
The figure shows 2I) EGFE'I' manufactured by the method of this invention.
A sectional view showing the configuration of another example, FIG. 4 is a conventional 2DEG
FIG. 2 is a cross-sectional view showing a configuration example of an FET. In the figure, (2) is a high-purity GaAs layer, (3) is an n-type first AlGaAs layer, (4) is an n-type GaAe layer, (
5) is a two-dimensional electron gas, the back is a gate metal, (l is a second AlGaAs layer, and α is a forward mesa-shaped groove. In addition, the same reference numerals in the figure indicate the same or corresponding parts.

Claims (1)

【特許請求の範囲】[Claims] (1)高純度GaAs層の上にこれとの間にヘテロ接合
を構成するn形の第1のAlGaAs層を形成し、この
n形の第1のAlGaAs層の上にn形GaAs層を形
成し、 このn形GaAs層の上に第2のAlGaAs層を形成
し、 この第2のAlGaAs層に上方に拡開する順メサ形の
断面形状を有し上記n形GaAs層に達する溝を形成し
、 この溝を介して上記n形GaAs層にショットキー接合
するゲート金属を形成した後に、上記第2のAlGaA
s層を除去する工程を備えた電界効果トランジスタの製
造方法。
(1) Form a first n-type AlGaAs layer forming a heterojunction between the high-purity GaAs layer and form an n-type GaAs layer on the first n-type AlGaAs layer. Then, a second AlGaAs layer is formed on this n-type GaAs layer, and a groove is formed in this second AlGaAs layer, which has a mesa-shaped cross-sectional shape that expands upward and reaches the n-type GaAs layer. After forming a gate metal that makes a Schottky junction to the n-type GaAs layer through this groove, the second AlGaAs
A method for manufacturing a field effect transistor, comprising a step of removing an s-layer.
JP61118336A 1986-05-22 1986-05-22 Manufacture of field-effect transistor Pending JPS62274675A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61118336A JPS62274675A (en) 1986-05-22 1986-05-22 Manufacture of field-effect transistor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61118336A JPS62274675A (en) 1986-05-22 1986-05-22 Manufacture of field-effect transistor

Publications (1)

Publication Number Publication Date
JPS62274675A true JPS62274675A (en) 1987-11-28

Family

ID=14734145

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61118336A Pending JPS62274675A (en) 1986-05-22 1986-05-22 Manufacture of field-effect transistor

Country Status (1)

Country Link
JP (1) JPS62274675A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01168069A (en) * 1987-12-24 1989-07-03 New Japan Radio Co Ltd Manufacture of semiconductor device
JPH0319243A (en) * 1989-06-15 1991-01-28 Matsushita Electron Corp Manufacture of field-effect transistor
JPH05136175A (en) * 1991-11-14 1993-06-01 Nec Corp Manufacture of field-effect transistor

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01168069A (en) * 1987-12-24 1989-07-03 New Japan Radio Co Ltd Manufacture of semiconductor device
JPH0319243A (en) * 1989-06-15 1991-01-28 Matsushita Electron Corp Manufacture of field-effect transistor
JPH05136175A (en) * 1991-11-14 1993-06-01 Nec Corp Manufacture of field-effect transistor

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