JPS5856471A - Compound semiconductor device - Google Patents
Compound semiconductor deviceInfo
- Publication number
- JPS5856471A JPS5856471A JP56155283A JP15528381A JPS5856471A JP S5856471 A JPS5856471 A JP S5856471A JP 56155283 A JP56155283 A JP 56155283A JP 15528381 A JP15528381 A JP 15528381A JP S5856471 A JPS5856471 A JP S5856471A
- Authority
- JP
- Japan
- Prior art keywords
- wiring
- type
- layer
- field effect
- effect transistor
- 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.)
- Granted
Links
Classifications
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D30/00—Field-effect transistors [FET]
- H10D30/80—FETs having rectifying junction gate electrodes
Landscapes
- Bipolar Transistors (AREA)
- Internal Circuitry In Semiconductor Integrated Circuit Devices (AREA)
- Junction Field-Effect Transistors (AREA)
Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】
本発明は、複数のゲート電極とそれらのゲート電極のそ
れぞれを挾んでソース電極とドレイン電極とが交互に設
けられている、いわ、ゆる、櫛型構造を有し、砒化ガリ
エウム(GtAs)基板に形成された電界効果トランジ
スタの′di極・配線の改良に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention has a so-called comb-shaped structure in which a plurality of gate electrodes and source electrodes and drain electrodes are provided alternately between each of the gate electrodes. This invention relates to improvement of the 'di pole and wiring of a field effect transistor formed on a gallium arsenide (GtAs) substrate.
化合物半導体特に砒化ガリエウム(GaAs)を使用し
た半導体装置は、その電子移動度が大きいこと、微細パ
ターンの形成が可能であること等種々な理由により、高
周波特性がすぐ力、ており、高出力化が容易であるため
、マイクロ波用電力トランジスタとして多く使用されて
おシ、又、その集積度を更に向上するための努力がなさ
れている。Semiconductor devices using compound semiconductors, especially gallium arsenide (GaAs), have excellent high-frequency characteristics and are suitable for high output due to various reasons such as their high electron mobility and the ability to form fine patterns. Because it is easy to implement, it is widely used as a power transistor for microwaves, and efforts are being made to further improve its degree of integration.
従来技術における砒化ガリエウム(GaAa)ペースの
電界効果トランジスタにおいては、クローム(Or)等
のP−プされた牛絶縁性砒化ガリエウム(GaAs)基
板上にn型砒化ガリエウム(GaAs)層をエピタキシ
ャル成長させ、この層をチャンネルとして利用すること
とし、この層上にゲート電極、ソース電極、ドレイン電
極を配設し、かくして形成された素子を囲む領域からは
n型エピタキシャル層をメサエッチする手法が多く使用
されているが、メサエッチされた段差を有するものは集
積化に不適切−’Q6す、又、エピタキシャル成長を使
用するよりイオン注入法を使用することが工程的にも有
利であるため、イオン注入法を活用したプレーナ型の砒
化ガリュウム(Ga As )ペースの電界効果トラン
ジスタの開発が望まれている。In prior art gallium arsenide (GaAa) based field effect transistors, an n-type gallium arsenide (GaAs) layer is epitaxially grown on a p-type insulating gallium arsenide (GaAs) substrate such as chrome (Or). This layer is used as a channel, and a method is often used in which a gate electrode, a source electrode, and a drain electrode are arranged on this layer, and the n-type epitaxial layer is mesa-etched from the region surrounding the thus formed device. However, those with mesa-etched steps are unsuitable for integration. Also, since it is more advantageous in terms of process than using epitaxial growth, ion implantation is used. It is desired to develop a planar type gallium arsenide (GaAs) based field effect transistor.
一方、その高出力化のためには、ゲート電極を複数とし
、各々のゲート電極を挾ん1ソース電極とドレイン電極
とを交互に配置した、いわゆる櫛型構造が有利−t’あ
る。かかる構造にあっては、ゲート電極幅を極力小さく
する必要がある。一方、各配線特にソース・ドレイン用
配線はある程度の電流容量を必要とするから各配線特に
ソース・ドレイン用配線の幅はある程度大きくしなけれ
ばならない。したがつて、各配線間隔を極めて狭くする
必要のある場合が存在する。On the other hand, in order to increase the output power, a so-called comb-shaped structure in which a plurality of gate electrodes are provided and one source electrode and one drain electrode are arranged alternately between each gate electrode is advantageous. In such a structure, it is necessary to make the gate electrode width as small as possible. On the other hand, since each wiring, especially the source/drain wiring, requires a certain amount of current capacity, the width of each wiring, especially the source/drain wiring, must be increased to some extent. Therefore, there are cases where it is necessary to make the intervals between each wiring extremely narrow.
クローム(Or)等をP−プした半絶縁性の砒化ガリュ
ウム(GaAs)には本来p型の不純物もn型の不純物
もかなりな量残留していることが一般1あるから、電界
条件、温度条件等によってはこれらの導電性不純物が絶
縁破壊の原因となりうる筈〒あり、配線間絶縁耐力の信
頼性に疑問のあることが砒化ガリエウム(GaAs)を
使用する牛導体装電の本来的欠点の一つt%あるが、特
に上記の櫛形構造においては、この欠点が顕在化し、致
命的欠点となり、この欠点の解消された櫛型構造を有す
る砒化ガリエウム(GaAa)ペースの電界効果ト、ラ
ンジスタの開発が望まれていた。Semi-insulating gallium arsenide (GaAs), which is P-type with chromium (Or), etc., generally has a considerable amount of p-type and n-type impurities remaining1, so electric field conditions and temperature Depending on the conditions, these conductive impurities can cause dielectric breakdown, and the fact that the reliability of the dielectric strength between wires is questionable is an inherent drawback of conductor installation using gallium arsenide (GaAs). However, especially in the above-mentioned comb-shaped structure, this defect becomes obvious and becomes a fatal defect, and this defect has been solved in gallium arsenide (GaAa)-based field effect transistors having a comb-shaped structure. development was desired.
、本発明の目的は、半絶縁性の砒化ガリュウム(GaA
a)基板表層に埋設されたn型領域(以下活性層という
。)を使用して形成するプレーナ型1あり、かつ、櫛型
構造の電界効果トランジスタにおいて、その各配線と基
板との絶縁耐圧の改善さねた電界効果トランジスタを提
供することにある0その要旨は、上記の電界効果トラン
ジスタにおいて、ゲート電極、ソース電極、ドレイン電
極に接続される配線の少なくとも一つは上記の砒化ガリ
ュウム(GaAa)基板の表層に埋設されたn型領域(
以下配線用n型層という0)上に配設することとし、こ
の配線の幅は配線用n型層の幅より狭いことにある。次
に、配線用n型層のn型不純物#度は、砒化ガリュウム
(GaAs)基板に残留しているn型不純物濃度の10
倍程度以上あることが効果を顕著に向上させる要件〒あ
り、基板に残留するn型不純物濃Vは通常1014/α
3程度fあるから、配線用p型層のn型不純物濃度は1
0 ” ’ /l:nr”以上あることが望ましい。第
2に、配線用n型層の効果が確実に発揮されるにはその
n型層の厚さが一定の値以上であることが必要マあるが
、この許容最小厚さは基板に形成しfCn型層の不純物
濃度が増加するにしたがって小さくなる傾向が認められ
、一方、基板に形成すべきn型層の含有不純物の濃度が
101s/an、”程度の場合その許容最小厚さは10
00Xrある。又、基板に形成するn型層の不純物濃度
が1017/cy−”程度と高い場合は許容最小厚さも
小さくなり、100 g程度となる。第3に、配線用n
型層の幅とこれ七対応する配線の幅との差は大きいこと
が安全″11%あるが、その必要最小限の値はその配線
に印加される電圧に応じて大きくなり、通常使用される
IOV程度フはパターニングの限界である1JIIn(
片@0.5μm)?十分!あるが、100v#&に対し
て1j2aun(片側1μm)程度が必要である。, the object of the present invention is to use semi-insulating gallium arsenide (GaA
a) In a planar type 1 field effect transistor formed using an n-type region (hereinafter referred to as an active layer) buried in the surface layer of the substrate and having a comb-type structure, the dielectric breakdown voltage between each wiring and the substrate is determined. The purpose is to provide an improved field effect transistor.In the above field effect transistor, at least one of the wirings connected to the gate electrode, the source electrode, and the drain electrode is made of the above gallium arsenide (GaAa). An n-type region (
Hereinafter, it is arranged on an n-type wiring layer (0), and the width of this wiring is narrower than the width of the n-type wiring layer. Next, the n-type impurity concentration of the n-type wiring layer is 10% of the n-type impurity concentration remaining in the gallium arsenide (GaAs) substrate.
The n-type impurity concentration V remaining in the substrate is usually 1014/α.
Since there is about 3 f, the n-type impurity concentration of the p-type layer for wiring is 1
It is desirable that the value is 0 ''/l:nr'' or more. Second, in order for the n-type layer for wiring to be effective, it is necessary that the thickness of the n-type layer be at least a certain value, but this minimum allowable thickness is the minimum thickness that can be formed on the substrate. It is recognized that fC tends to decrease as the impurity concentration of the n-type layer increases.On the other hand, when the impurity concentration of the n-type layer to be formed on the substrate is about 101s/an, the minimum allowable thickness is 10s/an.
There is 00Xr. Furthermore, if the impurity concentration of the n-type layer formed on the substrate is as high as about 1017/cy-'', the allowable minimum thickness will also be small, about 100 g.Thirdly, the n-type layer for wiring
It is safe to say that the difference between the width of the mold layer and the width of the corresponding wire is as large as 11%, but its minimum value increases depending on the voltage applied to that wire and is normally used. The IOV level is 1JIIn(
piece @0.5μm)? sufficient! However, approximately 1j2aun (1 μm on one side) is required for 100V#&.
以下、本発明の着想から発明への具体化に至る過程につ
いて説明する。まず、本発明の発明者は、牛絶縁性砒化
ガリエウム(GaAs)基板の一部領域にシリコン(s
l)をイオン注入して活性層を形成し、この活性層を利
用してプレーナ型電界効果トランジスタを形成した。こ
こで、ソース電極、rレインiil!極に接続される配
線は半絶縁性砒化ガリュウム(GaAa)基板上に配設
した。この試作品に対し、ゲート電圧を調整してチャン
ネルの抵抗を大きくしておき、ソース電極・Pレイン電
債間の電圧を増大しても活性層の温度が過度に上昇しな
り条件の下においてソース電極・rレイン’l ’IN
間の電圧を次第に上昇させて絶縁破壊に至る試験を実
施した。この破壊試験で観察されたことは絶縁破壊の発
住した箇PJrは活性層上ではなく半絶縁性基板上にお
いてであることであった。Hereinafter, the process from the idea of the present invention to its embodiment will be explained. First, the inventors of the present invention have discovered that a silicon (silicon)
1) was ion-implanted to form an active layer, and this active layer was used to form a planar field effect transistor. Here, the source electrode, r rain iil! Wiring connected to the poles was arranged on a semi-insulating gallium arsenide (GaAa) substrate. For this prototype, the gate voltage was adjusted to increase the channel resistance, and even if the voltage between the source electrode and the P-rain bond was increased, the temperature of the active layer would not rise excessively. Source electrode/r-rain 'l'IN
A test was conducted in which the voltage between the two was gradually increased until dielectric breakdown occurred. What was observed in this breakdown test was that the point PJr where dielectric breakdown occurred was not on the active layer but on the semi-insulating substrate.
そこフ、この現象を再確認する試験を下記のとおり実施
した。すなわち、まず、第1図に示すように、牛絶縁性
砒化ガリエウム(GaAa)基板l上に間隔x1を離し
て1対の金属層2を形成し、この間隔X1を0.5μm
乃至加μmの量変化させ、これら金属層2間を絶縁破壊
させて、間隔X1と絶縁破壊電圧Vmとの関係を測定し
て、第2図に示す結果を得た。図は間隔長x1の対数と
絶縁破壊電圧VBの対数とを示す。次に、第3図に示す
ように、牛絶縁性砒化ガリュウム(GaJks)基板1
の表層の一部領域に選択的にn型不純物が、イオン注入
された領域3を間隔X、を喘して形成し、その上に一対
の金属層2をオーミック接触させて形成し、この間隔x
2を0.5μm乃至(資)μmの量変化させ、金属層2
間を絶縁破壊させて、間隔長x2と絶縁破壊電圧Vnと
の関係を測定して第4図に示す結果を得た。図は間隔長
x2の対数とP!縁破壊電圧VBの対数とを示す。Therefore, we conducted the following test to reconfirm this phenomenon. That is, as shown in FIG. 1, first, a pair of metal layers 2 are formed on an insulating gallium arsenide (GaAa) substrate l with a distance x1 apart, and this distance X1 is set to 0.5 μm.
The relationship between the distance X1 and the dielectric breakdown voltage Vm was measured by changing the amount by .mu.m to .mu.m to cause dielectric breakdown between these metal layers 2, and the results shown in FIG. 2 were obtained. The figure shows the logarithm of the interval length x1 and the logarithm of the dielectric breakdown voltage VB. Next, as shown in FIG. 3, an insulating gallium arsenide (GaJks) substrate 1
A region 3 in which n-type impurities are selectively implanted into a partial region of the surface layer is formed at a distance of X, and a pair of metal layers 2 are formed thereon in ohmic contact. x
2 by varying the amount of 0.5 μm to (capital) μm, the metal layer 2
The relationship between the interval length x2 and the dielectric breakdown voltage Vn was measured by causing dielectric breakdown between the two, and the results shown in FIG. 4 were obtained. The figure shows the logarithm of interval length x2 and P! The logarithm of the edge breakdown voltage VB is shown.
第2図、第4図を比較すれば明らかなように、生絶縁性
砒化ガリュウム(GaAs)基板は意外に絶縁耐力に乏
しいことが発見され、従来かたく信じられていたクロー
ム(Or)ドープ等のなされた半絶縁性の砒化ガリエウ
ム(Ga Aθ)等の化合物半導体の絶縁耐力に対する
信頼性は誤であったことが確認された。As is clear from a comparison of Figures 2 and 4, it has been discovered that bioinsulating gallium arsenide (GaAs) substrates have unexpectedly poor dielectric strength. It has been confirmed that the reliability of the dielectric strength of semi-insulating compound semiconductors such as gallium arsenide (GaAθ) was incorrect.
上記の実験結果にもとづき、半絶縁性の砒化ガリュウム
(GaAs)を基板として櫛型構造の電界効果トランジ
スタを製造する場合、各電極と接続される配線、特に、
隣接する配線間の距離が接近しているものや、基板上に
配設される第1層配線(誘電体を介して配設される第二
、第三層は除く。)等は、直接基板上に配設するのでは
なく、半絶縁性の砒化ガリュウム(GaAs)基板の表
層にn型領域(配線用n型層)を形成し、その上に配線
を配設すれば、上記の目的を実現しうるものと結論した
。Based on the above experimental results, when manufacturing a comb-type field effect transistor using semi-insulating gallium arsenide (GaAs) as a substrate, the wiring connected to each electrode, in particular,
If the distance between adjacent wirings is close or the first layer wiring arranged on the board (excluding the second and third layers arranged through a dielectric), etc. The above purpose can be achieved by forming an n-type region (an n-type layer for wiring) on the surface layer of a semi-insulating gallium arsenide (GaAs) substrate and placing wiring on top of the substrate. I concluded that it is possible.
この結論にもとづき、この効果の確認をなす実験を繰り
返し、下記の事実を確認した。まず、配線用n型層のn
型不純物濃度と1?縁耐方向上効果との相関関係につい
ては、配線用n型層の不純物#度が基板に残留している
n型不純物濃度の10倍の不純物濃度の点で効果が顕著
に向上し、それ以下の1111度差では効果が必ずしも
顕著でないことが明らかになった。基板の残留n型不純
物#度はIQ + 4 /crnll程度が一般である
から、配線用n型層の不純物濃度は1015 /α3程
度以上が望ましい。第2に、配線用n型層の厚さと絶縁
耐力向上効果との相関関係については、この厚さが大き
い根絶縁耐力の向上に有効〒はあるが、配線用n型層の
不純物濃度と大きな相関関係が認められ、配線用n型層
の不純物濃度が大きいときは配線用n型層の厚さも薄く
てさしつかえない事実が明らかになった。Based on this conclusion, we repeated experiments to confirm this effect and confirmed the following facts. First, the n-type layer for wiring
Type impurity concentration and 1? Regarding the correlation with the effect on the edge resistance direction, the effect is significantly improved when the impurity concentration of the n-type wiring layer is 10 times the n-type impurity concentration remaining in the substrate, and when it is lower than that, the effect is significantly improved. It became clear that the effect was not necessarily significant with a difference of 1111 degrees. Since the residual n-type impurity concentration of the substrate is generally about IQ + 4 /crnll, the impurity concentration of the n-type wiring layer is preferably about 1015 /α3 or more. Second, regarding the correlation between the thickness of the n-type layer for wiring and the effect of improving dielectric strength, although this thickness is effective in improving the root dielectric strength, the impurity concentration of the n-type layer for wiring and the A correlation was observed, and it became clear that when the impurity concentration of the n-type wiring layer is high, the thickness of the n-type wiring layer can be thin.
その有効最小厚さは基板の残−留n型不純物濃度が10
17/cIIL3以上〒ある場合too X程度フあり
、基板の残留n型不純物濃度が101″/cIL3程度
マある場合1.00OA’t%ある。第3に、配線用n
型層−の幅とこれに対応する配線の幅との差と絶縁耐力
の向上効果との相関関係については、配線に印加される
電圧との相関関係が認められ、10v程度あれば、幅に
差があることが確認1きる程度(片側0.5μm程度)
あわば十分本発明の効果は認められた截100V程度!
ある場合は幅の差は2μm (片側1μm)程度必条で
ある事実が認められた。Its effective minimum thickness is determined by the residual n-type impurity concentration of the substrate being 10
If the residual n-type impurity concentration of the substrate is about 101''/cIL3 or more, it is 1.00OA't%.Thirdly, the wiring n
Regarding the correlation between the difference between the width of the mold layer and the width of the corresponding wiring and the effect of improving dielectric strength, there is a correlation with the voltage applied to the wiring. It can be confirmed that there is a difference (approximately 0.5 μm on one side)
The effect of the present invention is approximately 100V!
In some cases, it was recognized that the difference in width must be about 2 μm (1 μm on each side).
以上の構成を有する櫛型構造の電界効果トランジスタす
なわち、本発明の一実施例に係る砒化ガリニウム(Ga
As)ペースの電界効果トランジスタの断面図と平面図
とを、それぞれ、第5図と第6図とに示す。図において
、lは半絶縁性砒化ガリエウム(05LA!+)基板〒
アリ、4はシリコン(Sl)等n型の不純物をイオン注
入の上熱処理を施して形成した活性層である。5はシリ
コン(Sl)等n型の不純物を更にイオン注入の上熱処
理を施して形成したソース・ドレイン領域である。この
ソース・ドレイン領域は、平面図に示すように、そのま
ま延長して本発明の要旨である配線用n型層51となる
。6.7は、それぞれ、ソース・ドレイン電極−r!ア
リ、金・ゲルマニニウム(ムu−Go)等を蒸着の上ノ
ターニングし、熱処理を施してオーミックコンタクトと
なしである0このソース・ドレイン電極は、平面図に示
すように、そのまま配線用n型層51上にも延長してソ
ース・ドレイン配線61・71となる。8はショットキ
ノ々リヤゲート電極フありアルミニニウム(AI)等を
蒸着の上ノターニングして形成される。このゲート電極
も、平面図に示すように、延長してゲート配線81とな
る。A comb-type field effect transistor having the above configuration, that is, a gallium arsenide (Ga
A cross-sectional view and a plan view of a field-effect transistor of As) pace are shown in FIG. 5 and FIG. 6, respectively. In the figure, l is a semi-insulating gallium arsenide (05LA!+) substrate.
Reference numeral 4 indicates an active layer formed by ion-implanting n-type impurities such as silicon (Sl), followed by heat treatment. Reference numeral 5 denotes a source/drain region formed by further ion-implanting an n-type impurity such as silicon (Sl) and subjecting it to heat treatment. As shown in the plan view, this source/drain region is extended as it is to become the n-type wiring layer 51 which is the gist of the present invention. 6.7 are the source and drain electrodes -r! After depositing ants, gold/germanium (Mu-Go), etc., the source/drain electrodes are turned and heat treated to form ohmic contacts. It also extends onto the mold layer 51 to become source/drain wirings 61 and 71. Reference numeral 8 is formed by evaporating aluminum (AI) or the like with a Schottky rear gate electrode and then turning it. This gate electrode also extends to become a gate wiring 81, as shown in the plan view.
以上説明せるとおり、本発明によれば、半絶縁性の砒化
ガリュウム(GaAe)基板表層に即設されたn型領域
すなわち活性層を使用して形成するゾレーナ型であり、
かつ、櫛型構造の電界効果トランジスタにおいて、その
配線と基板との間の絶縁−耐力の改善された電界効果ト
ランジスタを提供することが1きる。As explained above, according to the present invention, the solena type is formed using an n-type region, that is, an active layer, immediately provided on the surface layer of a semi-insulating gallium arsenide (GaAe) substrate.
In addition, it is possible to provide a field effect transistor having a comb-shaped structure in which the insulation strength between the wiring and the substrate is improved.
第1図及び第3図は本発明の着想を確Vするためになし
た実験に使用した基板の断面図であり、第2図及び第4
図は上記実験の結果を示すグラフッある。第5.6図は
、それぞれ、本発明の一実施例に係る電界効果トランジ
スタの断面図と平面図とfある。
1・・・基板、2・・・金属層、3・・・n型不純物が
イオン注入された領域、”1・・・1対の金属層2の間
隔、x2・・・2箇のN型領域の縁間の間隔、4・・・
活性層、5・・・ソース・ドレイン領域、51・・・ソ
ース・ ドレイン配線用n型層、6・・・ソース電体、
61・・・ソース配線、7・・・ドレイン電極、フト・
・ドレイン配線、8・・・ダート電極、81・・・ゲー
ト配線0
第2図
LJ)g Xl f’Trr1 and 3 are cross-sectional views of the substrate used in experiments conducted to confirm the idea of the present invention, and FIGS.
The figure is a graph showing the results of the above experiment. FIG. 5.6 shows a cross-sectional view and a plan view, respectively, of a field effect transistor according to an embodiment of the present invention. DESCRIPTION OF SYMBOLS 1...Substrate, 2...Metal layer, 3...Region into which n-type impurity is ion-implanted, "1...Distance between a pair of metal layers 2, x2...2 N-type Spacing between edges of regions, 4...
Active layer, 5... Source/drain region, 51... N-type layer for source/drain wiring, 6... Source electric body,
61... Source wiring, 7... Drain electrode, foot...
・Drain wiring, 8... Dirt electrode, 81... Gate wiring 0 Figure 2 LJ)g Xl f'Trr
Claims (1)
されたn型領域(活性層)上に複数のゲート電極が設け
られており、該複数のゲート電極のそれぞれを挾んでソ
ース電極とドレイン電極とが交互に設けられてなる電界
効果トランジスタにおいて、ダート電極、ソース電極、
ドレイン電極に接続される配線の少なくとも一つは前記
半絶縁性の砒化ガリュウム基板の表層に埋設されたn型
領#(配線用n型層)上に設けられており、該少なくと
も一つめ配線の幅は核配線用n型層の幅より狭いことを
特徴とする電界効果トランジスタ。 (2)前記配線用n型層のn型不純物濃度は前記生絶縁
性砒化ガリエウム基板に残留しているn型不純物の濃度
の10倍以上であることを特徴とする特許請求の範囲第
1項記載の電界効果トランジスタ0(3)前記配線用n
型層の許容最小厚さは前記半絶縁性砒化ガリエウム基板
に形成さtた配線用n型不純物の濃度が増加するにした
がって小さくなり、n型不純物の濃度が10” 10R
3程度フある場合の許容最小厚さは1ooo Xであり
、n型不純物の濃度が1017/crn3以上〒ある場
合の許容最小厚さは100X〒あることを特徴とする特
許請求の範囲第1項又は第2項記載の電界効果トランジ
スタ。 (4)前記配線用n型層の幅と対応する配線の幅との差
は対応する配線に印加される最大電圧の増大にしたがっ
て大きくなり、該最大電圧の値がIOVの場合1μm程
度〒、、メリ、前記最大電圧の値が100Vの場合2μ
m程変であることを特徴とする特許請求の範囲第1項、
第2項又は第3項記載の電界効果トランジスタ。[Claims] (1) A plurality of gate electrodes are provided on an n-type region (active layer) buried in the surface layer of a semi-insulating arsenide diode IJJL substrate, and each of the plurality of gate electrodes is In a field effect transistor in which a source electrode and a drain electrode are provided alternately between the dirt electrode, the source electrode,
At least one of the wirings connected to the drain electrode is provided on an n-type region # (an n-type layer for wiring) buried in the surface layer of the semi-insulating gallium arsenide substrate, and the at least one wiring is connected to the drain electrode. A field effect transistor characterized in that its width is narrower than the width of an n-type layer for nuclear wiring. (2) The n-type impurity concentration of the wiring n-type layer is 10 times or more the n-type impurity concentration remaining in the bioinsulating gallium arsenide substrate. The field effect transistor described in 0(3) for the wiring n
The minimum allowable thickness of the mold layer decreases as the concentration of the n-type impurity for wiring formed on the semi-insulating gallium arsenide substrate increases, and when the concentration of the n-type impurity is 10" 10R.
Claim 1, characterized in that when the concentration of n-type impurities is 1017/crn3 or more, the minimum allowable thickness is 100X. Or the field effect transistor according to item 2. (4) The difference between the width of the n-type wiring layer and the width of the corresponding wiring increases as the maximum voltage applied to the corresponding wiring increases, and when the value of the maximum voltage is IOV, the difference is about 1 μm, , Meri, if the maximum voltage value is 100V, 2μ
Claim 1, characterized in that it varies by m.
The field effect transistor according to item 2 or 3.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56155283A JPS5856471A (en) | 1981-09-30 | 1981-09-30 | Compound semiconductor device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56155283A JPS5856471A (en) | 1981-09-30 | 1981-09-30 | Compound semiconductor device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5856471A true JPS5856471A (en) | 1983-04-04 |
| JPS632155B2 JPS632155B2 (en) | 1988-01-18 |
Family
ID=15602508
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP56155283A Granted JPS5856471A (en) | 1981-09-30 | 1981-09-30 | Compound semiconductor device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5856471A (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| EP0812020A2 (en) | 1996-06-04 | 1997-12-10 | Fujitsu Limited | Field effect transisor with reduced delay variation |
| US6200838B1 (en) | 1998-11-13 | 2001-03-13 | Fujitsu Quantum Devices Limited | Compound semiconductor device and method of manufacturing the same |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH03261859A (en) * | 1990-03-13 | 1991-11-21 | Nkk Corp | Tire-shaped ultrasonic probe |
| JPH0650944A (en) * | 1992-07-31 | 1994-02-25 | Nkk Corp | Inspecting apparatus for lap-joint welding part |
-
1981
- 1981-09-30 JP JP56155283A patent/JPS5856471A/en active Granted
Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| EP0812020A2 (en) | 1996-06-04 | 1997-12-10 | Fujitsu Limited | Field effect transisor with reduced delay variation |
| EP0812020A3 (en) * | 1996-06-04 | 1998-03-18 | Fujitsu Limited | Field effect transisor with reduced delay variation |
| US5942773A (en) * | 1996-06-04 | 1999-08-24 | Fujitsu Limited | Field effect transistor with reduced delay variation |
| US6200838B1 (en) | 1998-11-13 | 2001-03-13 | Fujitsu Quantum Devices Limited | Compound semiconductor device and method of manufacturing the same |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS632155B2 (en) | 1988-01-18 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| CN107996003B (en) | Insulated gate switching device and method of manufacturing the same | |
| US20230307529A1 (en) | Support shield structures for trenched semiconductor devices | |
| JPH0330310B2 (en) | ||
| US4662058A (en) | Self-aligned gate process for ICS based on modulation doped (Al,Ga) As/GaAs FETs | |
| KR920003799B1 (en) | Semiconductor device | |
| JPH0578949B2 (en) | ||
| JPH0548117A (en) | Static induction semiconductor device | |
| JPS632155B2 (en) | ||
| JP2688678B2 (en) | Field effect transistor and method of manufacturing the same | |
| JPS60180173A (en) | Field effect transistor capable of regulating threshold voltage and integrated circut having transistor of this type | |
| JPS59222966A (en) | Semiconductor device | |
| JPH0493038A (en) | Field-effect transistor | |
| JPS594083A (en) | Manufacture of semiconductor device | |
| JPS6034073A (en) | Method for manufacturing Schottky gate field effect transistor | |
| JPH04357844A (en) | Field-effect transistor | |
| JPS59210672A (en) | Semiconductor device | |
| JP2728427B2 (en) | Field effect transistor and its manufacturing method | |
| JPH0644605B2 (en) | Method of manufacturing high breakdown voltage MOS field effect semiconductor device | |
| JPS6332273B2 (en) | ||
| JP3338914B2 (en) | Semiconductor device and method of manufacturing semiconductor device | |
| KR930009811B1 (en) | Mes fet transistor and manufacturing method thereof | |
| JPS58145166A (en) | Semiconductor device | |
| GB2258344A (en) | Lt-gaas semiconductor device | |
| JPS6143443A (en) | Manufacture of semiconductor device | |
| JPS61222271A (en) | Field effect transistor and manufacture thereof |