JPH0328060B2 - - Google Patents

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Publication number
JPH0328060B2
JPH0328060B2 JP60152861A JP15286185A JPH0328060B2 JP H0328060 B2 JPH0328060 B2 JP H0328060B2 JP 60152861 A JP60152861 A JP 60152861A JP 15286185 A JP15286185 A JP 15286185A JP H0328060 B2 JPH0328060 B2 JP H0328060B2
Authority
JP
Japan
Prior art keywords
gate
plane
fet
directions
mes
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.)
Expired - Lifetime
Application number
JP60152861A
Other languages
Japanese (ja)
Other versions
JPS6213079A (en
Inventor
Tsukasa Onodera
Haruo Kawada
Toshiro Futaki
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.)
Fujitsu Ltd
Original Assignee
Fujitsu Ltd
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 Fujitsu Ltd filed Critical Fujitsu Ltd
Priority to JP60152861A priority Critical patent/JPS6213079A/en
Priority to KR1019850007310A priority patent/KR900000584B1/en
Priority to EP85307129A priority patent/EP0178133B1/en
Priority to DE8585307129T priority patent/DE3581159D1/en
Publication of JPS6213079A publication Critical patent/JPS6213079A/en
Priority to US07/158,043 priority patent/US4791471A/en
Publication of JPH0328060B2 publication Critical patent/JPH0328060B2/ja
Granted legal-status Critical Current

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  • Junction Field-Effect Transistors (AREA)

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、特に−族化合物半導
体ウエハー上に複数の電界効果トランジスタ素子
が形成された半導体集積回路装置の改造に関す
る。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a semiconductor device, particularly to modification of a semiconductor integrated circuit device in which a plurality of field effect transistor elements are formed on a - group compound semiconductor wafer.

マイクロエレクトロニクスは現代産業進展の基
盤となり、また社会生活に大きい影響を与えてい
る。現在このマイクロエレクトロニクスの主役は
シリコン(Si)半導体装置であつて、トランジス
タ素子の微細化によつて高速化と集積度の増大に
大きい効果をあげている。
Microelectronics has become the foundation of modern industrial progress and has had a major impact on social life. Silicon (Si) semiconductor devices are currently the mainstay of microelectronics, and the miniaturization of transistor elements has had a great effect on speeding up and increasing the degree of integration.

更にシリコンの物性に基づく限界を超える動作
速度の向上などを実現するために、キヤリアの移
動度がシリコンより遥かに大きい砒化ガリウム
(GaAs)などの化合物半導体を用いる半導体装
置が開発されている。
Furthermore, in order to achieve improvements in operating speed that exceed the limits based on the physical properties of silicon, semiconductor devices using compound semiconductors such as gallium arsenide (GaAs), whose carrier mobility is much higher than that of silicon, have been developed.

化合物半導体を用いるトランジスタとしては、
その製造工程が簡単であるなどの理由によつて電
界効果トランジスタ、特にシヨツトキバリア形電
界効果トランジスタの開発が先行しているが、そ
の特徴を十分に発揮した集積回路装置の実用化へ
の努力が重ねられている。
As a transistor using a compound semiconductor,
Although field effect transistors, especially shot-barrier field effect transistors, have been developed earlier due to their simple manufacturing process, efforts have been made to commercialize integrated circuit devices that take full advantage of their characteristics. It is being

〔従来の技術〕[Conventional technology]

シヨツトキバリア形電界効果トランジスタ(以
下MES FETと略称する)は現在化合物半導体、
特にGaAsを半導体材料とする例が多いが、その
構造の一例を第1図の模式側断面図に示す。
Schottky barrier field effect transistors (hereinafter abbreviated as MES FETs) are currently made of compound semiconductors.
In particular, there are many examples in which GaAs is used as the semiconductor material, and an example of its structure is shown in the schematic side sectional view of FIG.

図に示す従来例においては、半絶縁性GaAs基
板1の(100)面に、例えばイオン注入法によつ
てn形チヤネル層2が形成され、このn形チヤネ
ル層2上にシヨツトキ接触するゲート電極3が配
設される。
In the conventional example shown in the figure, an n-type channel layer 2 is formed on the (100) plane of a semi-insulating GaAs substrate 1 by, for example, ion implantation, and a gate electrode is in contact with the n-type channel layer 2. 3 is arranged.

このゲート電極3がマスクとするイオン注入法
によつて不純物が導入されて、n形チヤネル層2
より高不純物濃度のn+形ソース及びドレイン領
域4が形成され、絶縁膜5が被着されて、n+
ソース及びドレイン領域4にオーミツク接触する
ソース及びドレイン電極6が配設される。
Impurities are introduced into the n-type channel layer 2 by an ion implantation method using the gate electrode 3 as a mask.
N + -type source and drain regions 4 with higher impurity concentration are formed, an insulating film 5 is deposited, and source and drain electrodes 6 are provided in ohmic contact with the n + -type source and drain regions 4 .

上述の如きMES FETを素子として集積回路装
置が構成され、その高速化、高集積化のために
MES FET素子の微細化が進められそのゲート長
が短縮されるに伴つて、ゲート閾値電圧Vth等の
特性の期待される値からの変動幅が次第に大きく
なり、かつ基体面上の晶帯軸方向によりこのゲー
ト閾値電圧Vthの変動方向が異なる。
Integrated circuit devices are constructed using MES FETs as described above, and in order to increase their speed and integration,
As the miniaturization of MES FET elements progresses and their gate lengths are shortened, the range of variation in characteristics such as gate threshold voltage Vth from the expected value gradually increases, and Therefore, the direction of variation of this gate threshold voltage Vth differs.

第2図は、ゲート幅方向がGaAs(100)単結晶
面上で直交する晶帯軸〔011〕方向であるMES
FETと〔011〕方向であるMES FETとの、ゲ
ート閾値電圧Vth変動の例を示し、ゲート長2μm
程度以下において〔011〕方向ではプラス側に変
動する傾向があるのに対して、〔011〕方向ではマ
イナス側に大きく変動している。
Figure 2 shows an MES in which the gate width direction is in the [011] direction of the crystal zone axis, which is perpendicular to the GaAs (100) single crystal plane.
An example of gate threshold voltage Vth variation between FET and MES FET in the [011] direction is shown, and the gate length is 2 μm.
Below this level, there is a tendency for the [011] direction to fluctuate in the positive direction, while in the [011] direction it fluctuates significantly in the negative direction.

従つてMES FET素子をこの様に2方向に配置
した集積回路装置では、例えば製造プロセス中の
ばらつき等によりゲート長が設計値からずれた場
合に、ゲート閾値電圧Vthの変動量は相対的に大
きくなり、 目的とする回路動作が得られないために、従来
は通常ゲート方向を一方向に限つている。
Therefore, in an integrated circuit device in which MES FET elements are arranged in two directions in this way, if the gate length deviates from the design value due to variations during the manufacturing process, for example, the amount of variation in the gate threshold voltage Vth will be relatively large. Conventionally, the gate direction is usually limited to one direction because the desired circuit operation cannot be obtained.

第3図はゲート幅が同一方向のMES FET素子
で記憶装置のX及びYアドレスデコーダ回路を構
成した例を示す。
FIG. 3 shows an example in which the X and Y address decoder circuits of a storage device are constructed using MES FET elements whose gate widths are in the same direction.

同図aの如く、Xデコーダ11の出力線14と
Yデコーダ12の出力線15とは直角方向でメモ
リセルマトリクス13に接続される。Xデコーダ
11については同図bの如く、その出力線14と
MES FET素子のゲート電極Gの幅方向とを、例
えば〔011〕方向に揃えて無駄のないパターンと
することが出来る。
As shown in FIG. 3A, the output line 14 of the X decoder 11 and the output line 15 of the Y decoder 12 are connected to the memory cell matrix 13 in a perpendicular direction. As for the X decoder 11, its output line 14 and
By aligning the width direction of the gate electrode G of the MES FET element with, for example, the [011] direction, it is possible to form an efficient pattern.

これに対してYデコーダ12では、MES FET
素子のゲート電極Gの幅方向をXデコーダ11と
同一の〔011〕方向に揃える場合に、これは出力
線15に直角方向となる。このために同図cの如
く、ゲート電極Gを櫛形に分岐させ、多数のソー
スS及びドレインDを配設してXデコーダ11と
同等のゲート幅を得ている。このパターンは図b
のパターンより複雑であり、設計、製造プロセス
両面で微細化、高集積化が困難な部分となつてい
る。
On the other hand, in the Y decoder 12, the MES FET
When the width direction of the gate electrode G of the element is aligned in the same [011] direction as the X decoder 11, this becomes a direction perpendicular to the output line 15. For this purpose, the gate electrode G is branched into a comb shape, and a large number of sources S and drains D are arranged to obtain a gate width equivalent to that of the X decoder 11, as shown in FIG. This pattern is shown in Figure b
The pattern is more complex than that of the previous one, making miniaturization and high integration difficult in both the design and manufacturing process.

先に述べた所謂シヨートチヤネル効果の原因と
して、ソース及びドレイン領域4に導入された高
濃度の不純物のチヤネル層2への侵入と、主とし
て絶縁膜5によつて半導体基体に生ずる圧電分極
の効果が注目されている。
As the causes of the so-called short channel effect mentioned above, attention is focused on the penetration of high concentration impurities introduced into the source and drain regions 4 into the channel layer 2 and the effect of piezoelectric polarization generated in the semiconductor substrate mainly by the insulating film 5. has been done.

この圧電分極による特性の変動は、MES FET
素子の半導体基体に接して設けられる絶縁膜5、
ゲート電極3などが半導体基体に及ぼす応力によ
つて化合物半導体基体に圧電分極を生じ、チヤネ
ル層2におけるキラリアの分布が変化してシヨツ
トキ空乏層が伸縮するためにゲート閾値電圧Vth
が変動するものであり、応力方向と晶帯軸方向と
によつて定まる圧電分極の極性により、その変動
方向がプラス側又はマイナス側となるのである。
Changes in characteristics due to this piezoelectric polarization are caused by MES FET
an insulating film 5 provided in contact with the semiconductor substrate of the element;
The stress exerted on the semiconductor substrate by the gate electrode 3 causes piezoelectric polarization in the compound semiconductor substrate, and the chiral distribution in the channel layer 2 changes and the shot depletion layer expands and contracts, so that the gate threshold voltage Vth increases.
varies, and the direction of the variation is either positive or negative depending on the polarity of the piezoelectric polarization determined by the stress direction and the crystal zone axis direction.

(例えば、P.M.Asbeck et al.;IEEE
Transac−tions on Electron Devices、Vol.ED
−31、No.10、Oct.1984pp.1377−1380参照) これは特に−族の化合物半導体の場合、化
合物故その結晶性が非対称であることから生じる
ものと思われる。
(e.g. PMAsbeck et al.; IEEE
Transactions on Electron Devices, Vol.ED
(Refer to -31, No. 10, Oct. 1984 pp. 1377-1380) This seems to occur because, especially in the case of - group compound semiconductors, their crystallinity is asymmetric because they are compounds.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

以上の説明の如く従来の構造では、化合物半導
体電界効果トランジスタの特性の変動がゲート長
の短縮とともに極めて大きくなり、特に直交配置
は甚だ困難である。
As explained above, in the conventional structure, variations in the characteristics of the compound semiconductor field effect transistor become extremely large as the gate length is shortened, and in particular, orthogonal arrangement is extremely difficult.

この様な現状をこえて、微細化されたFET素
子を相互に直交するなど異なる方向に配置しても
特性が安定して、集積度の増大が可能である半導
体装置が強く要望されている。
In order to overcome this current situation, there is a strong demand for a semiconductor device whose characteristics are stable even when miniaturized FET elements are arranged in different directions, such as perpendicular to each other, and which allows for an increase in the degree of integration.

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

前記問題点は、主面が(110)面である−
族化合物半導体基板の該主面上に複数のゲート電
極が形成され、該複数のゲート電極上及び該主面
上に絶縁膜が形成され、該化合物半導体基板と該
複数のゲート電極とで複数の電界効果型トランジ
スタ素子が形成され、該複数のゲート電極が、異
なるゲート方向を有することを特徴とする本発明
による半導体装置より解決される。
The above problem is that the principal plane is the (110) plane.
A plurality of gate electrodes are formed on the main surface of the group compound semiconductor substrate, an insulating film is formed on the plurality of gate electrodes and the main surface, and a plurality of gate electrodes are formed on the compound semiconductor substrate and the plurality of gate electrodes. A semiconductor device according to the invention is characterized in that a field effect transistor element is formed and the plurality of gate electrodes have different gate directions.

〔作用〕[Effect]

本発明者等は例えばGaAs等の−族化合物
半導体基体に生ずる応力と絶縁膜の材料及び厚
さ、半導体基体の結晶面、晶帯軸とこの応力によ
る圧電分極の状態、電界効果トランジスタのゲー
ト閾値電圧及びK値と圧電分極の状態などの相関
関係を研究し、例えば絶縁膜が二酸化シリコン
(SiO2)である場合に、GaAs単結晶基体の結晶
面、nチヤネル形のMESFETのゲート軸方向と
ゲート閾値電圧Vthの変動方向との関係について
以下の結果を得ている。
The present inventors have studied, for example, the stress generated in a − group compound semiconductor substrate such as GaAs, the material and thickness of an insulating film, the crystal plane of the semiconductor substrate, the crystal zone axis and the state of piezoelectric polarization caused by this stress, the gate threshold of a field effect transistor. We study the correlation between voltage and K value and the state of piezoelectric polarization, and for example, when the insulating film is silicon dioxide (SiO 2 ), we investigate the relationship between the crystal plane of a GaAs single crystal substrate, the gate axis direction of an n-channel MESFET, etc. The following results were obtained regarding the relationship between the gate threshold voltage Vth and the direction of variation.

まず、第4図aにGaAs(100)面上でゲート幅
方向を〔110〕及び〔110〕方向とした場合、
同図bにGaAs(110)面上でゲート幅方向を
〔001〕及び〔110〕方向に向けて形成した場合
について、種々のSiO2膜厚に対するゲート閾値
電圧のゲート長依存性を示す。
First, when the gate width direction is set to [110] and [110] directions on the GaAs (100) plane as shown in Fig. 4a,
Figure b shows the dependence of the gate threshold voltage on the gate length for various SiO 2 film thicknesses when the gates are formed on the GaAs (110) plane with the gate width directed in the [001] and [110] directions.

これにより、(100)面上の直交する〔011〕方
向と〔011〕方向とでは、上述の如くVthの変動
方向が反対方向であるのに対して、(100)面上の
直交する〔001〕方向と〔110〕方向とはVth
の変動方向が同一方向であり、Vthの値それ自体
も、非常に近い値となつており、SiO2膜厚依存
性も極めて小さい。
As a result, the direction of Vth variation is opposite in the [011] direction and the [011] direction, which are perpendicular to each other on the (100) plane, as described above, whereas the [001] direction which is orthogonal to each other on the (100) plane ] direction and [110] direction are Vth
The fluctuation direction of Vth is the same direction, the value of Vth itself is also a very close value, and the dependence on the SiO 2 film thickness is also extremely small.

更に詳細に、GaAs半導体基体の(110)面上
に、ゲート幅方向が〔110〕方向のゲート電極
を例えばタングステンシリサイド(WSi)で形成
し、SiO2膜を被着したときの圧電分極電荷の分
布を第5図に示す。同図において、Aは1×1016
cm-3以上、Bは5×1015cm-3以上、Cは1×1015
cm-3以上、Dは5×1014cm-3以上の濃度を、また
−はマイナス、無符号はプラスの電荷を表す。
More specifically, when a gate electrode with the gate width direction in the [110] direction is formed, for example, from tungsten silicide (WSi) on the (110) plane of a GaAs semiconductor substrate, and a SiO 2 film is deposited, the piezoelectric polarization charge is The distribution is shown in Figure 5. In the same figure, A is 1×10 16
cm -3 or more, B is 5 × 10 15 cm -3 or more, C is 1 × 10 15
cm -3 or higher, D represents a concentration of 5 x 10 14 cm -3 or higher, - represents a negative charge, and no sign represents a positive charge.

同図から明らかなように、圧電分極電荷の符号
はゲート電極の中央を境に左右で反転しており、
絶対値は各々等しくなつている。このため、
FETチヤネルの空乏層への影響はプラスとマイ
ナスで打ち消し合うように作用する。従つて圧電
効果による〔110〕FETのVthの変動は小さ
い。また、圧電分極電荷の符号がFETの左右で
反転しているため、チヤネル内のキヤリアの移動
を加速する効果がある。このため、通常のFET
よりも伝達コンダクタンスgmが大きくなり、集
積回路中で電流を駆動する目的に使用すれば、動
作速度の改良に利用できる。
As is clear from the figure, the sign of the piezoelectric polarization charge is reversed on the left and right sides with the center of the gate electrode as the border.
The absolute values are equal. For this reason,
The positive and negative influences on the depletion layer of the FET channel act to cancel each other out. Therefore, the variation in Vth of the [110] FET due to the piezoelectric effect is small. Furthermore, since the sign of the piezoelectric polarization charge is reversed on the left and right sides of the FET, it has the effect of accelerating the movement of carriers within the channel. For this reason, a normal FET
The transconductance gm is larger than that of the current, and if used for the purpose of driving current in an integrated circuit, it can be used to improve the operating speed.

また、これを直交する〔001〕方向のFETでは
圧電分極電荷は全く誘起されない。このため第4
図bに示されたように、〔001〕FETのVthの
SiO2膜厚依存性は無い。
Further, in the FET in the [001] direction perpendicular to this, no piezoelectric polarization charge is induced at all. For this reason, the fourth
As shown in Figure b, the Vth of [001] FET is
There is no dependence on SiO 2 film thickness.

更に(110)面上では、任意の方向について、
圧電効果によるFET特性の変動は極めて小さく、
ゲート閾値電圧Vthの制御は非常に容易となる この(110)面の特性により、この面に形成さ
れたゲート方向が相互に直交するFETの間には
圧電分極効果の差が現れず、チヤネル長を短縮し
ても方向の異なるFET間にゲート閾値電圧等の
特性の差を生じない。またゲート方向が斜交する
FETの間でも特性の差異は僅少となる。このこ
とは集積回路の設計の容易性をもたらすのであ
る。
Furthermore, on the (110) plane, for any direction,
Fluctuations in FET characteristics due to piezoelectric effects are extremely small.
Controlling the gate threshold voltage Vth is very easy.Due to the characteristics of this (110) plane, there is no difference in piezoelectric polarization effect between FETs formed on this plane whose gate directions are perpendicular to each other, and the channel length is Even if the length is shortened, there will be no difference in characteristics such as gate threshold voltage between FETs with different directions. Also, the gate direction is oblique.
Differences in characteristics between FETs are minimal. This provides ease of integrated circuit design.

〔実施例〕〔Example〕

以下本発明を実施例により具体的に説明する。 The present invention will be specifically explained below using examples.

第6図はGaAs MES FETを基本素子とする
E/D構成の集積回路装置にかかる本発明の実施
例を示す工程順模式平面図である。
FIG. 6 is a schematic plan view showing the process order of an embodiment of the present invention relating to an integrated circuit device having an E/D configuration using GaAs MES FET as a basic element.

本実施例では、(110)面を主面とする半絶縁性
GaAs基板上に、E(エンハンスメント)モード
(以下添字Eで表す)とD(デイプリーシヨン)モ
ード(以下添字Dで表す)のMES FET素子から
なるインバータを、それぞれのゲート幅方向を
〔001〕方向(以下添字1で表す)及び〔110〕
方向(以下添字2で表す〕として形成する。
In this example, a semi-insulating film with (110) plane as the main surface is used.
An inverter consisting of an E (enhancement) mode (hereinafter referred to as subscript E) and a D (depletion) mode (hereinafter referred to as subscript D) MES FET elements is mounted on a GaAs substrate, with the gate width direction of each [001] Direction (hereinafter represented by subscript 1) and [110]
direction (hereinafter represented by subscript 2).

第6図a参照 半絶縁性GaAs基板21の(110)面に、例え
ば下記の如くシリコン(Si)をイオン注入して各
素子のn形チヤネル領域2を形成する。
Refer to FIG. 6a. For example, silicon (Si) is ion-implanted into the (110) plane of the semi-insulating GaAs substrate 21 as described below to form the n-type channel region 2 of each element.

Dモードのチヤネル領域22D1及び22D2、 エネルギー59kev、 ドーズ量1.7×1012cm-2 Eモードのチヤネル領域22E1及び22E2、 エネルギー59kev、 ドーズ量0.9×1012cm-2 イオン注入後、基板1面上に窒化アルミニウム
(AIN)等の保護膜(図示されない)を設けて、
例えば温度850℃、時間15分間程度の活性化熱処
理を行う。
D mode channel regions 22 D1 and 22 D2 , energy 59kev, dose 1.7×10 12 cm -2 E mode channel regions 22 E1 and 22 E2 , energy 59kev, dose 0.9×10 12 cm -2 After ion implantation, A protective film (not shown) such as aluminum nitride (AIN) is provided on one surface of the substrate,
For example, activation heat treatment is performed at a temperature of 850° C. for about 15 minutes.

第6図b参照 基板1面上に、例えばW5Si3を厚さ400mm程度
にスパツタ法等により被着し、これをパターニン
グして各ゲート電極23を形成する。本実施例で
はゲート長を約1μmとしている。
Refer to FIG. 6b. For example, W 5 Si 3 is deposited to a thickness of about 400 mm by sputtering or the like on the surface of the substrate 1, and this is patterned to form each gate electrode 23. In this embodiment, the gate length is approximately 1 μm.

第6図c参照 ゲート電極23をマスクとして、基板に例えば
Siをエネルギー175kevで、ドーズ量1.7×1013cm
-2程度にイオン注入し、例えば温度750℃、時間
10分間程度の活性化熱処理を行つて、n+形ソー
ス、ドレイン領域24を形成する。
Refer to FIG. 6c. Using the gate electrode 23 as a mask, for example,
Si at energy 175kev, dose 1.7×10 13 cm
Ion implantation is performed at a temperature of about -2 , for example at a temperature of 750°C for a period of time.
Activation heat treatment is performed for about 10 minutes to form n + type source and drain regions 24.

第6図d参照 例えばプラズマ化学気相成長方法法(P−
CVD法)により、窒化シリコン(SiNx)膜(図
示されない)を厚さ例えば500mm程度に、ゲート
電極を含む基板1全面上に被着する。
See Figure 6d. For example, plasma chemical vapor deposition method (P-
A silicon nitride (SiNx) film (not shown) is deposited to a thickness of, for example, about 500 mm over the entire surface of the substrate 1 including the gate electrode by CVD (CVD method).

n+形ソース、ドレイン領域24上でSiNxに開
口を設け、例えば蒸着法により金ゲルマニウム/
金(AuGe/Au)などを用いて、ソース、ドレ
イン電極25等を厚さ250mm程度に形成する。
Openings are formed in SiNx above the n + type source and drain regions 24, and gold/germanium/gold/germanium/
The source and drain electrodes 25 and the like are formed to a thickness of about 250 mm using gold (AuGe/Au) or the like.

本実施例のゲート方向が直交する2種類の
MES FET素子は、D、Eそれぞれのモードにつ
いて、ゲート閾値電圧Vthの差がゲート長1μmに
おいて数10mVに止まり、全く同等に使用するこ
とが可能である。
In this example, two types of gates with orthogonal gate directions are used.
In the MES FET element, the difference in gate threshold voltage Vth for each of the D and E modes is only a few tens of mV at a gate length of 1 μm, and it is possible to use them completely equally.

先の従来例のデコーダについても、同一のパタ
ーンのMES FET素子で良好なX、Y両デコーダ
が得られており、任意の集積回路を形成すること
が可能である。
Regarding the conventional decoder described above, both X and Y decoders can be obtained using MES FET elements having the same pattern, and it is possible to form an arbitrary integrated circuit.

また以上の説明はGaAs MES FETを対象と
しているが、他の化合物半導体材料を用い、或い
は接合形、MIS形の電界効果トランジスタについ
ても、本発明の方法により同様の効果が得られ
る。
Further, although the above description is directed to GaAs MES FETs, similar effects can be obtained by the method of the present invention using other compound semiconductor materials, or with junction type or MIS type field effect transistors.

〔発明の効果〕〔Effect of the invention〕

以上説明した如く本発明によれば、化合物半導
体電界効果トランジスタのゲート方向を任意の相
互に直交する方向に配置し、チヤネル長を短縮し
ても、ゲート閾値電圧等の特性を均一にすること
が可能となり、斜交する場合においても特性の差
異が減少して、化合物半導体集積回路装置の実用
化に大きい効果が得られる。
As explained above, according to the present invention, even if the gate directions of compound semiconductor field effect transistors are arranged in arbitrary mutually orthogonal directions and the channel length is shortened, characteristics such as gate threshold voltage can be made uniform. This makes it possible to reduce the difference in characteristics even in the case of diagonal crossing, resulting in a great effect on the practical application of compound semiconductor integrated circuit devices.

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

第1図はMES FETの従来例を示す模式側断面
図、第2図はMES FETの特性の従来例を示す
図、第3図aはデコーダの例を示す模式平面図、
第3図b及びcはデコーダのMES FET素子の従
来例を示す模式平面図、第4図aはMES FETの
特性の従来例を示す図、第4図bはMES FETの
特性の本発明の効果を示す図、第5図はGaAs
(110)面上、ゲート幅が〔110〕方向で、SiO2
を被着したときの圧電分極電荷の分布図、第6図
a乃至dは本発明の実施例を示す工程順模式平面
図である。 図において、21は半絶縁性GaAs基板、22
はn形チヤネル領域、23はゲート電極、24は
n+形ソース、ドレイン領域、25はソース、ド
レイン電極、添字Dはデイプリーシヨンモード、
添字Eはエンハンスメントモード、添字1はゲー
ト幅方向〔001〕、添字2はゲート幅方向〔11
0〕を示す。
FIG. 1 is a schematic side sectional view showing a conventional example of MES FET, FIG. 2 is a diagram showing a conventional example of MES FET characteristics, and FIG. 3a is a schematic plan view showing an example of a decoder.
Figures 3b and 3c are schematic plan views showing conventional examples of MES FET elements in decoders, Figure 4a is a diagram showing conventional examples of MES FET characteristics, and Figure 4b is a diagram showing the characteristics of MES FETs according to the present invention. A diagram showing the effect, Figure 5 is GaAs
A piezoelectric polarization charge distribution diagram when a SiO 2 film is deposited on the (110) plane with a gate width in the [110] direction. Figures 6a to 6d are schematic plan views in the order of steps showing embodiments of the present invention. It is. In the figure, 21 is a semi-insulating GaAs substrate, 22
is an n-type channel region, 23 is a gate electrode, and 24 is an n-type channel region.
n + type source and drain regions, 25 is source and drain electrode, subscript D is depletion mode,
Subscript E is enhancement mode, subscript 1 is gate width direction [001], subscript 2 is gate width direction [11]
0].

Claims (1)

【特許請求の範囲】 1 主面が(110)面である−族化合物半導
体基板の該主面上に複数のゲート電極が形成さ
れ、 該複数のゲート電極上及び該主面上に絶縁膜が
形成され、 該化合物半導体基板と該複数のゲート電極とで
複数の電界効果型トランジスタ素子が形成され、 該複数のゲート電極が、異なるゲート方向を有
することを特徴とする半導体集積回路装置。 2 前記異なるゲート方向が、相互に直交する方
向であることを特徴とする特許請求の範囲第1項
記載の半導体装置。
[Claims] 1. A plurality of gate electrodes are formed on the main surface of a - group compound semiconductor substrate whose main surface is a (110) plane, and an insulating film is formed on the plurality of gate electrodes and on the main surface. A semiconductor integrated circuit device, wherein a plurality of field effect transistor elements are formed by the compound semiconductor substrate and the plurality of gate electrodes, and the plurality of gate electrodes have different gate directions. 2. The semiconductor device according to claim 1, wherein the different gate directions are directions perpendicular to each other.
JP60152861A 1984-07-11 1985-07-11 Semiconductor integrated circuit device Granted JPS6213079A (en)

Priority Applications (5)

Application Number Priority Date Filing Date Title
JP60152861A JPS6213079A (en) 1985-07-11 1985-07-11 Semiconductor integrated circuit device
KR1019850007310A KR900000584B1 (en) 1984-07-11 1985-10-04 Semiconductor integrated circuit device
EP85307129A EP0178133B1 (en) 1984-10-08 1985-10-04 Semiconductor integrated circuit device
DE8585307129T DE3581159D1 (en) 1984-10-08 1985-10-04 SEMICONDUCTOR ARRANGEMENT WITH INTEGRATED CIRCUIT.
US07/158,043 US4791471A (en) 1984-10-08 1988-02-16 Semiconductor integrated circuit device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60152861A JPS6213079A (en) 1985-07-11 1985-07-11 Semiconductor integrated circuit device

Publications (2)

Publication Number Publication Date
JPS6213079A JPS6213079A (en) 1987-01-21
JPH0328060B2 true JPH0328060B2 (en) 1991-04-17

Family

ID=15549723

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60152861A Granted JPS6213079A (en) 1984-07-11 1985-07-11 Semiconductor integrated circuit device

Country Status (1)

Country Link
JP (1) JPS6213079A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01273359A (en) * 1988-04-26 1989-11-01 Nec Corp Semiconductor integrated circuit

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58145168A (en) * 1982-02-24 1983-08-29 Fujitsu Ltd Semiconductor device

Also Published As

Publication number Publication date
JPS6213079A (en) 1987-01-21

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