JPH01101671A - semiconductor equipment - Google Patents
semiconductor equipmentInfo
- Publication number
- JPH01101671A JPH01101671A JP62258438A JP25843887A JPH01101671A JP H01101671 A JPH01101671 A JP H01101671A JP 62258438 A JP62258438 A JP 62258438A JP 25843887 A JP25843887 A JP 25843887A JP H01101671 A JPH01101671 A JP H01101671A
- Authority
- JP
- Japan
- Prior art keywords
- gate electrode
- semiconductor layer
- layer
- source
- gate
- 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.)
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Links
Classifications
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- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D64/00—Electrodes of devices having potential barriers
- H10D64/20—Electrodes characterised by their shapes, relative sizes or dispositions
- H10D64/27—Electrodes not carrying the current to be rectified, amplified, oscillated or switched, e.g. gates
- H10D64/311—Gate electrodes for field-effect devices
- H10D64/411—Gate electrodes for field-effect devices for FETs
Landscapes
- Junction Field-Effect Transistors (AREA)
Abstract
Description
【発明の詳細な説明】
[産業上の利用分野]
本発明は半導体装置に関し、特にA I GaAS/
GaA3選択ドープ構造を有する電界効果トランジスタ
で代表されるヘテロ接合デバイス、すなわちHEMT(
高移動度トランジスタ)等の2次元電子ガス層を動作層
とする半導体装置に関する。[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a semiconductor device, and particularly to an A I GaAS/
A heterojunction device, typified by a field effect transistor with a GaA3 selectively doped structure, i.e., a HEMT (
The present invention relates to a semiconductor device having a two-dimensional electron gas layer as an active layer, such as a high-mobility transistor.
[従来の技術]
従来、HEMT等の半導体装置においては、不純物無添
加のGaAS半導体層と不純物添加のA I GaAS
混晶半導体層とのヘテロ界面に形成される2次元電子ガ
ス層を動作層として利用するために、基板上に前記Ga
As半導体層と前記A I GaAs半導体層を交互に
成長させることにより1層あるいは多層の前記2次元電
子ガス層を形成し、前記A I GaAs半導体層各層
中に埋め込まれた単一の、あるいは多数のゲート電極に
より前記各2次元電子ガス層における走行キャリアを制
御する構造がとられていた。[Prior Art] Conventionally, in semiconductor devices such as HEMT, an undoped GaAS semiconductor layer and an impurity-doped AI GaAS semiconductor layer are used.
In order to utilize the two-dimensional electron gas layer formed at the hetero interface with the mixed crystal semiconductor layer as an active layer, the Ga
The two-dimensional electron gas layer of one layer or multiple layers is formed by growing the As semiconductor layer and the A I GaAs semiconductor layer alternately, and the single or multiple electron gas layers are embedded in each layer of the A I GaAs semiconductor layer. A structure was adopted in which traveling carriers in each of the two-dimensional electron gas layers were controlled by a gate electrode.
従来のHEMTにおいてゲート電極が半導体層に埋め込
まれている構造の一例を第3図に示す。FIG. 3 shows an example of a structure in which a gate electrode is buried in a semiconductor layer in a conventional HEMT.
ゲート電極35を不純物無添加のGaAs層32・、3
4あるいは不純物添加のAlGaAs層33に埋め込む
ことによる効用は、第1にはソース抵抗の改善であり、
第2には前記GaAs層32.34と前記A I Ga
As層33を交互に基板31上で成長させることで多層
の2次元電子ガス層40を形成させている場合、該2次
元電子ガス層40をチャネルとして動作させる際には、
単一あるいは多数のゲート電極を埋め込む方法が有効で
あると考えられる点である。The gate electrode 35 is made of impurity-free GaAs layers 32, 3.
4 or the effect of embedding in the impurity-added AlGaAs layer 33 is, first, improvement of source resistance;
Second, the GaAs layer 32, 34 and the A I Ga
When a multilayer two-dimensional electron gas layer 40 is formed by growing As layers 33 alternately on the substrate 31, when operating the two-dimensional electron gas layer 40 as a channel,
A method of burying a single or multiple gate electrodes is considered to be effective.
[発明が解決しようとする問題点]
しかし、上記従来の構造のトランジスタは、ゲート電極
35の各2次元電子ガス層40側に生じる空乏層の幅を
変化させることによって、該2次元電子ガス層40にお
ける走行キャリアを制御するものでおるから、かかるゲ
ート電極35のドレイン側あるいはソース側の半導体は
本来不要であるばかりか、ソースとゲートとの間あるい
はドレインとゲートとの間の奇生容量として作用し、高
周波特性あるいは高速スイッチング特性に大きな欠点と
なる。[Problems to be Solved by the Invention] However, in the transistor of the conventional structure described above, by changing the width of the depletion layer generated on the side of each two-dimensional electron gas layer 40 of the gate electrode 35, the two-dimensional electron gas layer 40, the semiconductor on the drain side or the source side of the gate electrode 35 is essentially unnecessary, and it also acts as a parasitic capacitance between the source and the gate or between the drain and the gate. This causes a major drawback in high frequency characteristics or high speed switching characteristics.
本発明は、上記問題点に鑑みて創案されたちので、ゲー
トとソースまたはドレインとの間の奇生容量を減少させ
ることかでき、電界効果トランジスタの高周波特性ある
いは高速スイッチング特性を改善した半導体装置を提供
することを目的とする。The present invention was devised in view of the above-mentioned problems, and therefore provides a semiconductor device that can reduce the parasitic capacitance between the gate and the source or drain, and improves the high frequency characteristics or high speed switching characteristics of a field effect transistor. The purpose is to provide.
[問題点を解決づるための手段]
本発明は、電子親和力に差のおる相異なる半導体層間の
、電子親和力が大なる半導体層側に、前記半導体層間の
ヘテロ界面沿いに形成された2次元電子ガス層を1層ま
たは2層以上と、この2次元電子ガス層を流れる電流を
取出す合金電極とを有し、かつ前記半導体層に埋設され
た1個または2個以上のゲート電極を備えてなる半導体
装置において、ゲート電極のソース側側面およびドレイ
ン側側面に前記半導体層よりも比誘電率の小なる絶縁物
で形成された側壁を備えてなることを特徴とする半導体
装置である。[Means for Solving the Problems] The present invention provides two-dimensional electrons formed along the hetero-interface between the semiconductor layers on the side of the semiconductor layer with the larger electron affinity between different semiconductor layers having different electron affinities. It has one or more gas layers, an alloy electrode for extracting the current flowing through the two-dimensional electron gas layer, and one or more gate electrodes embedded in the semiconductor layer. A semiconductor device characterized in that a side wall on a source side and a drain side of a gate electrode is formed of an insulator having a dielectric constant lower than that of the semiconductor layer.
本発明において、半導体層よりも比誘電率の小なる絶縁
物としては、たとえば二酸化シリコンがあげられる。In the present invention, an example of the insulator having a dielectric constant lower than that of the semiconductor layer is silicon dioxide.
[作用]
本発明は、2次元電子ガス層を動作層とする埋め込みゲ
ート電極を備えた電界効果1トランジスタにおいて、前
記ソースとゲートとの間あるいはドレインとゲートとの
間の寄生容量を減少させるためにゲート電極のソース側
の側面と、ゲート電極のドレイン側の側面に比誘電率の
小さな絶縁物で形成された側壁を設けることによって動
作の高周波化を図ったものでおる。[Function] The present invention provides a method for reducing the parasitic capacitance between the source and the gate or between the drain and the gate in a field effect transistor having a buried gate electrode with a two-dimensional electron gas layer as an operating layer. The high-frequency operation is achieved by providing side walls made of an insulator with a low relative dielectric constant on the side surface of the gate electrode on the source side and the side surface of the gate electrode on the drain side.
従来は、埋め込まれたゲート電極のソース側およびドレ
イン側の両側面における奇生容量がゲート電極と接して
いるGaAs層あるいはAIGaAS層の生み出すもの
として無視できぬ大きざであったが、本発明による電界
効果トランジスタにおいてはゲート電極におけるソース
側およびトレイン側の側面に比誘電率の小さな絶縁物、
たとえばシリコン酸化膜が配置されているため、従来に
比へ前記奇生容量が大幅に改善される。GaASおよび
A I GaAsの比誘電率は12.5〜13.0であ
るが5i02の比誘電率は3.5〜4.0とGaAsお
よびA I GaAsのそれと比べてほぼ173以下の
値を示しており、電界効果トランジスタとしての高周波
特性の改善に大きく寄与する。Conventionally, the parasitic capacitance on both the source and drain sides of the buried gate electrode was caused by the GaAs layer or AIGaAS layer in contact with the gate electrode and was a non-negligible problem, but the present invention In a field effect transistor, an insulator with a low dielectric constant is used on the source side and train side sides of the gate electrode.
For example, since a silicon oxide film is disposed, the parasitic capacitance is significantly improved compared to the conventional case. The relative permittivity of GaAS and A I GaAs is 12.5 to 13.0, but the relative permittivity of 5i02 is 3.5 to 4.0, which is approximately 173 or less compared to that of GaAs and A I GaAs. This greatly contributes to improving the high-frequency characteristics of field-effect transistors.
[実施例]
以下、図面を参照して、本発明の実施例を詳細に説明す
る。[Example] Hereinafter, an example of the present invention will be described in detail with reference to the drawings.
第1図は本発明による電界効果トランジスタの一実施例
を示す縦断面図である。第1図において、1は半絶縁性
GaAs基板、2および4は不純物無添加GaAs半導
体層、3は不純物添加A I GaAs半導体層、5は
ゲート電極、6はソース電極、7はソース領域、8はド
レイン電極、9はトレイン領域、10は2次元電子ガス
層、11は5i02側壁でおる。本実施例に示す電界効
果トランジスタは基本的には2層の不純物無添加のGa
As半導体層2,4の間に不純物をドープしたAIGa
AS半導体層3を挟み、該A I GaAS半導体層3
中にゲート電極5を埋設した構造をしている。この構造
においては2層のGaAS半導体層2,4とA I G
aAS半導体層3との界面に2次元電子ガス層10が形
成される。該A I GaAs半導体層3に埋め込まれ
たゲート電極5の周囲の空乏層は動作電圧により上下方
向に広がり、2層の前記2次元電子ガス層10のキャリ
ア蓄積状態を同時に制御する。従って、この埋め込みゲ
ート電極構造は、従来のHEMTに比べて制御可能な電
流量を向上させ得ると共に、高い相互コンダクタンスを
得ることが可能となる。第1図中で示すゲート電極5の
ソース側およびドレイン側の側面に設けられたシリコン
酸化膜の側壁11が本発明の絶縁体側壁で、この側壁1
1の存在によりゲート・ソース間の寄生容Nおよびゲー
ト・トレイン間の奇生容量の削減が行われ、電界効果ト
ランジスタとしての高周波特性および高速スイッチング
特性が改善される。FIG. 1 is a longitudinal sectional view showing an embodiment of a field effect transistor according to the present invention. In FIG. 1, 1 is a semi-insulating GaAs substrate, 2 and 4 are undoped GaAs semiconductor layers, 3 is an impurity-doped AI GaAs semiconductor layer, 5 is a gate electrode, 6 is a source electrode, 7 is a source region, 8 9 is a drain electrode, 9 is a train region, 10 is a two-dimensional electron gas layer, and 11 is a 5i02 side wall. The field effect transistor shown in this example basically consists of two layers of undoped Ga.
AIGa doped with impurities between As semiconductor layers 2 and 4
The A I GaAS semiconductor layer 3 sandwiching the AS semiconductor layer 3
It has a structure in which a gate electrode 5 is embedded. In this structure, two GaAS semiconductor layers 2 and 4 and an A I G
A two-dimensional electron gas layer 10 is formed at the interface with the aAS semiconductor layer 3. The depletion layer around the gate electrode 5 embedded in the A I GaAs semiconductor layer 3 expands in the vertical direction due to the operating voltage, and simultaneously controls the carrier accumulation state of the two two-dimensional electron gas layer 10 . Therefore, this buried gate electrode structure can improve the amount of current that can be controlled compared to conventional HEMTs, and can also obtain high mutual conductance. The side walls 11 of the silicon oxide film provided on the source and drain sides of the gate electrode 5 shown in FIG. 1 are the insulator side walls of the present invention.
1 reduces the parasitic capacitance N between the gate and source and the parasitic capacitance between the gate and train, improving the high frequency characteristics and high speed switching characteristics of the field effect transistor.
次に、上記側壁を備えた埋め込みゲート電極の製造工程
の一例を第2図(a)〜(d)の各図により説明する。Next, an example of the manufacturing process of the buried gate electrode having the sidewalls will be explained with reference to FIGS. 2(a) to 2(d).
各図は、半絶縁性GaAs基板21上に、例えば有機金
属化学堆積法により成長させた不純物無添加のGaAs
半導体層あるいは不純物添加のA I GaAs半導体
層22にゲート電極23を埋め込む場合を説明するもの
でおる。ゲート電極23の材料としてはタングステンシ
リサイド等の金属おるいは金属化合物を用い、スパッタ
あるいは電子ビーム蒸着またはCVD法によって第2図
(a)に示す如く、厚さ400人で付着させ、例えばプ
ラズマエツチング法あるいはリフトオフ法によって金属
幅が5000八以下となるようにゲート電極23を形成
する。Each figure shows impurity-free GaAs grown on a semi-insulating GaAs substrate 21 by, for example, an organometallic chemical deposition method.
A case will be described in which a gate electrode 23 is buried in a semiconductor layer or an impurity-doped AI GaAs semiconductor layer 22. A metal or metal compound such as tungsten silicide is used as the material for the gate electrode 23, and is deposited to a thickness of 400 mm by sputtering, electron beam evaporation, or CVD as shown in FIG. The gate electrode 23 is formed by a method or a lift-off method so that the metal width is 5,000 mm or less.
この金属幅がすなわちゲート長に相当する。This metal width corresponds to the gate length.
ゲート電極23を形成した後、CVD法により、第2図
(b)に示す如く、全面にシリコン酸化膜24を400
人程度付着させ、CF4およびSF6の混合ガスによる
M I E (Magnetron Ion Etch
ina >法によりゲート電極23の上面およびGaA
s半導体層あるいはA I GaAs半導体層22表面
が現れる直前までシリコン酸化膜24のエツチングを行
う。その後、完全に表面が現れるまで過酸化水素と弗酸
の混合液によりシリコン酸化膜24のエツチングを行う
。After forming the gate electrode 23, as shown in FIG.
Attach the body to about the same level as a person, and perform MIE (Magnetron Ion Etch) using a mixed gas of CF4 and SF6.
The upper surface of the gate electrode 23 and the GaA
The silicon oxide film 24 is etched until just before the surface of the s semiconductor layer or the A I GaAs semiconductor layer 22 appears. Thereafter, the silicon oxide film 24 is etched using a mixture of hydrogen peroxide and hydrofluoric acid until the surface is completely exposed.
その結果第2図(C)に示されるようにゲート電極23
の両側にシリコン酸化膜24の側壁25が形成される。As a result, as shown in FIG. 2(C), the gate electrode 23
Side walls 25 of silicon oxide film 24 are formed on both sides of the silicon oxide film 24 .
その後はゲート電極形成前と同様に、有機金属化学堆積
法によりGaAs半導体層あるいはAlGaAs半導体
層22の成長を再度打つ。n 選択成長に関しての有機
金属化学堆積法の有効性および再現性は′、例えば19
84年第45回応用物理学会14a−J−7で中村他に
より報告されており、また、金属ゲート電極の埋め込み
成長に関しては、特表昭56−500991 @公報に
おいてPBTの製造工程の中でCarl、0. Boz
ler他によって詳しく報告されている。ゲート電極2
3の材料としてはGaAsおよびエピタキシャル成長過
程中用いられる他の製品に対して充分不活性であること
からタングステンの有効性が指摘されている。しかしゲ
ート電極23としては金属おるいはその化合物の代りに
p型の不純物を高濃度に添加した低抵抗のGaAsを用
いても良い。Thereafter, the GaAs semiconductor layer or the AlGaAs semiconductor layer 22 is grown again by the organometallic chemical deposition method in the same manner as before forming the gate electrode. The effectiveness and reproducibility of metal-organic chemical deposition methods for selective growth is ', e.g. 19
It was reported by Nakamura et al. at the 45th Annual Meeting of Japan Society of Applied Physics 14a-J-7 in 1984, and regarding buried growth of metal gate electrodes, Carl ,0. Boz
It has been reported in detail by ler et al. Gate electrode 2
As material No. 3, tungsten has been shown to be effective as it is sufficiently inert to GaAs and other products used during the epitaxial growth process. However, for the gate electrode 23, low-resistance GaAs doped with p-type impurities at a high concentration may be used instead of metal or its compound.
以上の工程によりGaAs半導体層あるいはAIGaA
S半導体層22中にシリコン酸化膜24に挟まれた形で
ゲート電極23を埋め込む操作が第2図(d)に示す−
ような形状で完了する。Through the above steps, GaAs semiconductor layer or AIGaA
The operation of embedding the gate electrode 23 in the S semiconductor layer 22 sandwiched between the silicon oxide films 24 is shown in FIG. 2(d).
Complete with a shape like this.
なお、結晶系としてはGaAs/ A I GaAs系
を用いた事例を示したが、この他にInAlAs系 I
nAlAs系、InP/ InGaAS系等についても
本発明を実施することは可能でおる。また、本発明の実
施例は特定の値を用いて説明したが、これは理解を容易
にするためであり、例えばゲート電極の蒸着量が増加す
れば、シリコン酸化膜側壁の量も比例して増加させるこ
とは言うまでもなく、ゲート・ソース間およびゲート・
ドレイン間の奇生容量を十分に削減するだけの量であれ
ば良い。また、側壁として用いる材料も用いられるそれ
ぞれの半導体よりも比誘電率の小さい絶縁物ならばシリ
コン酸化物に限らない。Although we have shown an example using the GaAs/A I GaAs crystal system, there are also cases where the InAlAs I
The present invention can also be practiced with nAlAs systems, InP/InGaAS systems, and the like. Furthermore, although the embodiments of the present invention have been explained using specific values, this is for ease of understanding; for example, if the amount of deposited gate electrode increases, the amount of silicon oxide film sidewalls also increases proportionally. Needless to say, the gate-to-source and gate-to-source
The amount may be sufficient as long as it sufficiently reduces the parasitic capacitance between the drains. Furthermore, the material used for the sidewalls is not limited to silicon oxide as long as it is an insulator with a dielectric constant lower than that of the respective semiconductors used.
[発明の効果]
以上、説明したとおり、本発明によれば、2次元電子ガ
ス層をチャネルとして用い、かつその制御を半導体層中
に埋め込まれたゲート電極により行う電界効果トランジ
スタにおいて、ゲート電極のソース側の側面およびドレ
イン側の側面に比誘電率の小さな絶縁物で形成された側
壁を設けることにより、ゲートとソースとの間の容量お
よびゲ−トとドレインとの間の奇生容量を減少させるこ
とができ、電界効果トランジスタの高周波特性おるいは
高速スイッチング特性を改善した半導体装置を提供する
ことができる。[Effects of the Invention] As described above, according to the present invention, in a field effect transistor that uses a two-dimensional electron gas layer as a channel and controls it by a gate electrode embedded in a semiconductor layer, By providing sidewalls made of an insulator with a low dielectric constant on the source side and drain side, the capacitance between the gate and source and the parasitic capacitance between the gate and drain are reduced. Therefore, it is possible to provide a semiconductor device with improved high frequency characteristics or high speed switching characteristics of a field effect transistor.
第1図は本発明の一実施例を示す縦断面図、第2図(a
)〜(d)は本発明の一実施例の製造工程の説明図、第
3図は従来例の縦断面図である。
1 、21.31 ・・・半絶縁性GaAs基板2、4
.32.34・・・不純物無添加GaAs半導体層3.
33・・・不純物添加AIGaAS半導体層5、23,
35.・・・ゲート電極
6.36・・・ソース電極 7,37・・・ソース領
域8.38・・・ドレイン電極 9,39・・・ドレイ
ン領域10、40・・・2次元電子ガス層FIG. 1 is a vertical sectional view showing one embodiment of the present invention, and FIG.
) to (d) are explanatory diagrams of the manufacturing process of an embodiment of the present invention, and FIG. 3 is a longitudinal sectional view of a conventional example. 1, 21.31 ... Semi-insulating GaAs substrate 2, 4
.. 32.34... Impurity-free GaAs semiconductor layer 3.
33... Impurity-doped AIGaAS semiconductor layer 5, 23,
35. ...Gate electrode 6.36...Source electrode 7,37...Source region 8.38...Drain electrode 9,39...Drain region 10, 40...Two-dimensional electron gas layer
Claims (2)
子親和力が大なる半導体層側に、前記半導体層間のヘテ
ロ界面沿いに形成された2次元電子ガス層を1層または
2層以上と、この2次元電子ガス層を流れる電流を取出
す合金電極とを有し、かつ前記半導体層に埋設された1
個または2個以上のゲート電極を備えてなる半導体装置
において、ゲート電極のソース側側面およびドレイン側
側面に前記半導体層よりも比誘電率の小なる絶縁物で形
成された側壁を備えてなることを特徴とする半導体装置
。(1) between different semiconductor layers having different electron affinities, one or more two-dimensional electron gas layers formed along the hetero interface between the semiconductor layers on the side of the semiconductor layer having a large electron affinity; an alloy electrode for extracting a current flowing through the two-dimensional electron gas layer, and a semiconductor layer embedded in the semiconductor layer.
In a semiconductor device comprising one or more gate electrodes, a side wall formed of an insulator having a dielectric constant lower than that of the semiconductor layer is provided on a side surface on the source side and a side surface on the drain side of the gate electrode. A semiconductor device characterized by:
シリコンである特許請求の範囲第1項記載の半導体装置
。(2) The semiconductor device according to claim 1, wherein the insulator having a dielectric constant lower than that of the semiconductor layer is silicon dioxide.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62258438A JP2541240B2 (en) | 1987-10-15 | 1987-10-15 | Semiconductor device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62258438A JP2541240B2 (en) | 1987-10-15 | 1987-10-15 | Semiconductor device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH01101671A true JPH01101671A (en) | 1989-04-19 |
| JP2541240B2 JP2541240B2 (en) | 1996-10-09 |
Family
ID=17320205
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP62258438A Expired - Lifetime JP2541240B2 (en) | 1987-10-15 | 1987-10-15 | Semiconductor device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2541240B2 (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6893961B2 (en) | 1999-09-01 | 2005-05-17 | Micron Technology, Inc. | Methods for making metallization structures for semiconductor device interconnects |
-
1987
- 1987-10-15 JP JP62258438A patent/JP2541240B2/en not_active Expired - Lifetime
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6893961B2 (en) | 1999-09-01 | 2005-05-17 | Micron Technology, Inc. | Methods for making metallization structures for semiconductor device interconnects |
| US6955979B2 (en) * | 1999-09-01 | 2005-10-18 | Micron Technology, Inc. | Methods for making metallization structures for semiconductor device interconnects |
| US7071557B2 (en) | 1999-09-01 | 2006-07-04 | Micron Technology, Inc. | Metallization structures for semiconductor device interconnects, methods for making same, and semiconductor devices including same |
Also Published As
| Publication number | Publication date |
|---|---|
| JP2541240B2 (en) | 1996-10-09 |
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