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JPH0614534B2 - Semiconductor integrated circuit - Google Patents

Semiconductor integrated circuit

Info

Publication number
JPH0614534B2
JPH0614534B2 JP59153972A JP15397284A JPH0614534B2 JP H0614534 B2 JPH0614534 B2 JP H0614534B2 JP 59153972 A JP59153972 A JP 59153972A JP 15397284 A JP15397284 A JP 15397284A JP H0614534 B2 JPH0614534 B2 JP H0614534B2
Authority
JP
Japan
Prior art keywords
region
gate
channel
emission type
induction 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.)
Expired - Lifetime
Application number
JP59153972A
Other languages
Japanese (ja)
Other versions
JPS6134980A (en
Inventor
潤一 西澤
薫 本谷
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.)
SHINGIJUTSU JIGYODAN
Original Assignee
SHINGIJUTSU JIGYODAN
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 SHINGIJUTSU JIGYODAN filed Critical SHINGIJUTSU JIGYODAN
Priority to JP59153972A priority Critical patent/JPH0614534B2/en
Priority to US06/759,090 priority patent/US4712122A/en
Priority to GB8518841A priority patent/GB2162370B/en
Priority to DE19853526826 priority patent/DE3526826A1/en
Priority to FR8511514A priority patent/FR2568410B1/en
Publication of JPS6134980A publication Critical patent/JPS6134980A/en
Priority to US07/469,226 priority patent/US5117268A/en
Publication of JPH0614534B2 publication Critical patent/JPH0614534B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime 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]
    • H10D30/202FETs having static field-induced regions, e.g. static-induction transistors [SIT] or permeable base transistors [PBT]
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D62/00Semiconductor bodies, or regions thereof, of devices having potential barriers
    • H10D62/10Shapes, relative sizes or dispositions of the regions of the semiconductor bodies; Shapes of the semiconductor bodies
    • H10D62/17Semiconductor regions connected to electrodes not carrying current to be rectified, amplified or switched, e.g. channel regions
    • H10D62/213Channel regions of field-effect devices
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D62/00Semiconductor bodies, or regions thereof, of devices having potential barriers
    • H10D62/80Semiconductor bodies, or regions thereof, of devices having potential barriers characterised by the materials
    • H10D62/82Heterojunctions
    • H10D62/824Heterojunctions comprising only Group III-V materials heterojunctions, e.g. GaN/AlGaN heterojunctions
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D64/00Electrodes of devices having potential barriers
    • H10D64/60Electrodes characterised by their materials
    • H10D64/602Heterojunction gate electrodes for FETs
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D84/00Integrated devices formed in or on semiconductor substrates that comprise only semiconducting layers, e.g. on Si wafers or on GaAs-on-Si wafers
    • H10D84/01Manufacture or treatment
    • H10D84/02Manufacture or treatment characterised by using material-based technologies
    • H10D84/05Manufacture or treatment characterised by using material-based technologies using Group III-V technology

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  • Bipolar Integrated Circuits (AREA)
  • Junction Field-Effect Transistors (AREA)

Description

【発明の詳細な説明】 〔発明の技術分野〕 本発明は熱電子放射型静電誘導トランジスタを用いた半
導体集積回路に関する。
Description: TECHNICAL FIELD OF THE INVENTION The present invention relates to a semiconductor integrated circuit using a thermionic emission type static induction transistor.

〔先行技術とその問題点〕[Prior art and its problems]

静電誘導型トランジスタ(以下、SITと略す)は、ゲ
ート領域とゲート領域の間で空乏層がつながって生じて
いる電位障壁の高さを変化させてソース領域・ドレイン
領域間の電流を制御するトランジスタである。このと
き、電位の制御が空乏層の静電容量を通して行われるこ
とから、バイポーラトランジスタにおけるベース層の蓄
積容量がないものに相等しく、FETと比べてみても非
常に高速、低雑音で動作するという優れた特性を有して
いる。
An electrostatic induction transistor (hereinafter abbreviated as SIT) controls the current between the source region and the drain region by changing the height of a potential barrier generated by connecting a depletion layer between gate regions. It is a transistor. At this time, since the control of the potential is performed through the capacitance of the depletion layer, it is equivalent to that of the bipolar transistor which does not have the storage capacitance of the base layer, and it operates at a very high speed and low noise as compared with the FET. It has excellent characteristics.

しかし、従来のSITはソース領域・ドレイン領域間、
特にソース領域・ゲート領域間の寸法が割合と大きな構
造になっていたため、キャンリアが結晶格子の散乱を受
け、上限周波数が制限される問題点があった。
However, in the conventional SIT, between the source region and the drain region,
In particular, since the size between the source region and the gate region has a relatively large structure, there is a problem in that the canria is scattered by the crystal lattice and the upper limit frequency is limited.

〔発明の目的〕[Object of the Invention]

本発明は、上記従来の問題点を解消し、キャリアが結晶
格子の散乱を受けずに熱電子速度で動くことのできる新
規な熱電子放射型SITを用いた半導体集積回路を提供
することを目的とする。
It is an object of the present invention to solve the conventional problems described above and to provide a semiconductor integrated circuit using a novel thermionic emission type SIT in which carriers can move at a thermionic velocity without being scattered by a crystal lattice. And

〔発明の概要〕[Outline of Invention]

本発明は、真性或いは半絶縁性基板の一部に第1導電型
の高不純物密度領域よりなる第1ドレイン領域を設け、
その第1ドレイン領域上に第1チャンネル領域、第1導
電型の高不純物密度領域よりなる第1ソース領域を縦型
に、また、前記第1チャンネル領域周辺部には前記第1
チャンネル領域よりも禁制帯幅の大きい半導体で第1ゲ
ート領域を形成し、前記第1ソース領域と真の第1ゲー
ト領域間の寸法をキャリアの平均自由行程以下にしてノ
ーマリオフ型の駆動用熱電子放射型静電誘導トランジス
タを形成すると共に、この駆動用熱電子放射型静電誘導
トランジスタに隣接する領域には、前記第1ドレイン領
域を第2ソース領域とし、この第2ソース領域上に第2
チャンネル領域、第1導電型の高不純物密度領域よりな
る第2ドレイン領域を縦型に、また、前記第2チャンネ
ル領域周辺部には前記第2チャンネル領域よりも禁制帯
幅の大きい半導体を用い前記第1ゲート領域よりも薄型
の第2ゲート領域を形成してノーマリオン型とした負荷
用静電誘導トランジスタを形成し、前記駆動用熱電子放
射型静電誘導トランジスタの第1ゲート領域に接して形
成される電極に信号入力端子、第1ソース領域に接して
形成される電極に接地端子、第1ドレイン領域に接して
形成される電極に出力端子、更に前記負荷用静電誘導ト
ランジスタの第2ドレイン領域に接して形成される電極
に電源端子をそれぞれ設けて集積回路を構成したことを
特徴とする。
The present invention provides a first drain region formed of a high-concentration impurity region of the first conductivity type in a part of an intrinsic or semi-insulating substrate,
A first channel region, a first source region formed of a first-conductivity-type high-impurity-density region are formed vertically on the first drain region, and the first channel region is provided with a first source region in the peripheral portion.
The first gate region is formed of a semiconductor having a forbidden band width larger than that of the channel region, and the dimension between the first source region and the true first gate region is set to be equal to or smaller than the mean free path of carriers, and a normally-off type driving thermoelectron. A radiation type electrostatic induction transistor is formed, and the first drain region is used as a second source region in a region adjacent to the driving thermoelectron radiation type static induction transistor, and a second source region is formed on the second source region.
A channel region and a second drain region composed of a first-conductivity-type high-impurity-density region are formed vertically, and a semiconductor having a forbidden band width larger than that of the second channel region is used in the peripheral portion of the second channel region. A normally-on type load static induction transistor is formed by forming a second gate region thinner than the first gate region, and is in contact with the first gate region of the driving thermionic emission type static induction transistor. The formed electrode has a signal input terminal, the electrode formed in contact with the first source region has a ground terminal, the electrode formed in contact with the first drain region has an output terminal, and the second electrode of the load static induction transistor. It is characterized in that an integrated circuit is configured by providing power supply terminals to electrodes formed in contact with the drain region.

〔発明の実施例〕Example of Invention

静電誘導トランジスタの高速化を図るために寸法を小さ
していくと、ソース領域に接し形成される電極前面の電
位の山(障壁)を越えたものは全てドレイン側に走ると
考えたときに、この障壁の幅がキャリアの平均自由行程
に近くなると、キャリアは殆んど格子散乱によらず、非
常に高速で走行するようになる。
When the size is reduced in order to increase the speed of the electrostatic induction transistor, all that exceeds the potential peak (barrier) on the front surface of the electrode formed in contact with the source region runs to the drain side, When the width of this barrier becomes close to the mean free path of the carriers, the carriers will be traveling at a very high speed almost without relying on the lattice scattering.

このときの電流密度Jは下記(1)式で与えられる。The current density J at this time is given by the following equation (1).

ここで、qは単位電荷、kはボルツマン定数、Tは絶対
温度、mはキャリアの有効質量、nsはソース領域の不
純物密度、φGSはゲート領域とソース領域の拡散電位、
Gはゲート領域に加えた電位である。
Here, q is a unit charge, k is a Boltzmann constant, T is an absolute temperature, m * is an effective mass of carriers, ns is an impurity density of a source region, φ GS is a diffusion potential of a gate region and a source region,
V G is the potential applied to the gate region.

キャリアの注入状態が熱電子放射状態になったときのS
ITのしゃ断周波数fcは、電位障壁の幅をWgのしたとき
に、SITを従属接続して2段目の入力容量を考慮した
ときには下記(2)式で与えられる。
S when the carrier injection state becomes the thermionic emission state
The cut-off frequency fc of IT is given by the following equation (2) when the width of the potential barrier is set to Wg and the input capacitance of the second stage is considered by connecting SIT in cascade.

従って、GaAsを用いた場合で電位障壁の幅Wgを0.
1μmとしたときに、しゃ断周波数fcはほぼ780GH
z程度となる。
Therefore, when GaAs is used, the width Wg of the potential barrier is 0.
The cutoff frequency fc is approximately 780 GH when 1 μm is set.
It is about z.

以上のことからソース領域と真のゲート領域間の寸法を
キャリアの平均自由行程以下にして SITを熱電子放射構造とすれば、スイッチング時間が
短かくなり、しかもキャリアが散乱を受けずに真のゲー
ト領域を越えて走行するためにgm(相互コンダクタン
ス)を大きくし易く電流駆動能力が高いという集積回路
用の優れたトランジスタが得られる。
From the above, if the size between the source region and the true gate region is made equal to or smaller than the mean free path of the carriers and the SIT has a thermionic emission structure, the switching time becomes short, and the carriers are not scattered and the true An excellent transistor for an integrated circuit can be obtained in which gm (transconductance) is easily increased to travel over the gate region and the current driving capability is high.

ここで、真のゲート領域とは、トンネル注入型SIT動
作時にチャンネル中のソース領域近傍に生じる電位障壁
の最も高い点のことである。この真のゲート領域の生じ
る位置は、チャンネル幅(チャンネル領域中のソース領
域とドレイン領域間の寸法)が短い場合は殆んどドレイ
ン電圧には影響されることなく、ほぼソース領域近傍に
できる。
Here, the true gate region is the highest point of the potential barrier generated in the vicinity of the source region in the channel during the tunnel injection type SIT operation. When the channel width (the size between the source region and the drain region in the channel region) is short, the position where the true gate region is generated can be almost near the source region without being affected by the drain voltage.

以下、この熱電子放射型SITを用いた集積回路につい
て説明する。
Hereinafter, an integrated circuit using this thermionic emission type SIT will be described.

第1図は本発明の一実施例に係る半導体集積回路の断面
図を示したものである。図において、1は真性半導体な
いしは半絶縁性のGaGs基板、2は駆動用熱電子放射
型SITのドレイン領域、3はチャンネル領域、4はチ
ャンネル領域3を形成するGaAsよりも禁制帯幅の大
きいGa1 -xAlxAsまたはGa1-xAlxAs1 -yPy等の材料を用いて形成されるヘテロ接合ゲート領
域、5は駆動用熱電子放射型SITのソース領域、8は
ゲート電極、9はソース電極、 10は出力電極である。
FIG. 1 is a sectional view of a semiconductor integrated circuit according to an embodiment of the present invention. In the figure, 1 is an intrinsic semiconductor or semi-insulating GaGs substrate, 2 is a drain region of a driving thermoelectron emission type SIT, 3 is a channel region, and 4 is a Ga having a larger forbidden band than GaAs forming the channel region 3. A heterojunction gate region formed using a material such as 1 -xAlxAs or Ga 1 -xAlxAs 1 -yPy, 5 is a source region of a driving thermoelectron emission SIT, 8 is a gate electrode, 9 is a source electrode, and 10 is It is an output electrode.

この第1図の左側に形成される駆動用熱電子放射型SI
Tに接続する領域に、前記ドレイン領域2をソース領域
とする負荷用熱電子放射型SITが形成される。40は
ゲート領域4と同じ材料で形成されたゲート領域である
が、ゲート領域4よりも薄く形成することによりノーマ
リオン動作型のSITを形成させ負荷抵抗として機能さ
せてる。45は負荷用熱電子放射型SITのドレイン領
域、91はドレイン電極である。
Driving thermionic emission type SI formed on the left side of FIG.
A thermionic emission type SIT for load having the drain region 2 as a source region is formed in a region connected to T. Reference numeral 40 denotes a gate region formed of the same material as the gate region 4, but by forming the gate region 4 thinner than the gate region 4, a normally-on operation type SIT is formed to function as a load resistance. Reference numeral 45 is a drain region of the thermionic emission type SIT for load, and 91 is a drain electrode.

12はSi3N4、SiO2、ポリイミド樹脂等の絶縁物、20
は入力端子、21はソース電極に設けられた接地単式、
22は出力端子、23は電源端子である。
12 is an insulator such as Si 3 N 4 , SiO 2 , and polyimide resin, 20
Is an input terminal, 21 is a ground single type provided on the source electrode,
22 is an output terminal and 23 is a power supply terminal.

駆動用及び負荷用熱電子放射型SITの各チャンネル領
域3の不純物密度は101218cm-3、チャンネルの長さ
は0.1〜1μmとして動作時には空乏層となるように
し、また、寸法は平均自由行程以下とする。また、ソー
ス領域およびドレイン領域の不純物密度は101820cm
-3、ゲート領域のヘテロ接合の組成はx=0.3、y=
0. 01程度とし、ソース電極、出力および電源端子の電極
9,10,91はAu−Ge、Au−Ge−Ni等の合
金、ゲート電極8はAl、Au、W、Pt等の重金属を
用いて構成する。
The impurity density of each channel region 3 of the driving and loading thermionic emission type SIT is 10 12 to 18 cm −3 , and the length of the channel is 0.1 to 1 μm so as to form a depletion layer during operation. Is less than the mean free path. The impurity density of the source region and the drain region is 10 18 to 20 cm.
-3 , the composition of the heterojunction in the gate region is x = 0.3, y =
0. The electrode electrodes 9, 10 and 91 for the source electrode, the output and the power supply terminal are made of an alloy such as Au-Ge, Au-Ge-Ni, etc., and the gate electrode 8 is made of a heavy metal such as Al, Au, W, Pt, etc. To do.

第2図は第1図の等価回路を示したものである。FIG. 2 shows an equivalent circuit of FIG.

30は第1図に示した半導体集積回路の断面図の左側に
形成された熱電子放射型SITでノーマリオフ特性を有
するもの、32は第1図の右側に形成され負荷抵抗とし
て用いるノーマリオン特性を有するSITの等価回路を
示している。20,21,22,23はそれぞれ入力端
子、接地端子、出力端子、電源端子である。入力端子2
0に印加される入力信号が「ロー」のときは熱電子放射
型SIT30がオフで出力端子22へは「ハイ」レベル
が生じ、入力信号が「ハイ」になると、熱電子放射型S
IT30はオンして出力端子22へは「ロー」レベルが
生じ、いわゆるインバータ動作をする。ここで、SIT
32はノーマリオン動作とするとにより等価的に抵抗と
して機能させている。
Reference numeral 30 denotes a thermionic emission type SIT formed on the left side of the sectional view of the semiconductor integrated circuit shown in FIG. 1, which has a normally-off characteristic, and 32 indicates a normally-on characteristic used as a load resistance formed on the right side of FIG. The equivalent circuit of SIT which it has is shown. Reference numerals 20, 21, 22, and 23 are an input terminal, a ground terminal, an output terminal, and a power supply terminal, respectively. Input terminal 2
When the input signal applied to 0 is “low”, the thermionic emission type SIT 30 is off and a “high” level is generated at the output terminal 22, and when the input signal becomes “high”, the thermionic emission type SIT 30 is
The IT 30 is turned on, a "low" level is generated at the output terminal 22, and the so-called inverter operation is performed. Where SIT
32 is made to function as a resistance equivalently by the normally-on operation.

このように、本実施例の集積回路は、熱電子放射型SI
Tが縦型構造であるので、チャンネル長を1000Å以
下にすることは容易で、スイッチング速度が従来とFE
TないしはHEMTよりも高速、かつ、低消費電力の集
積回路が実現できる。更に、上部に形成されるソース領
域とゲート領域の配線が容易であることによって、ソー
ス電極、ゲート電極、ドレイン電極の微細配線を要する
FETないしはHEMTによる集積回路に比べて製造が
容易となる。そのために配線部分に要する面積をおおよ
そ2/3に減らせる結果、高集積化が実現できるように
なる。
As described above, the integrated circuit of this embodiment has the thermionic emission SI
Since T has a vertical structure, it is easy to set the channel length to 1000 Å or less, and the switching speed is the same as that of the conventional FE.
It is possible to realize an integrated circuit which is faster than T or HEMT and has lower power consumption. Further, since the wiring of the source region and the gate region formed on the upper portion is easy, the manufacturing becomes easier as compared with the integrated circuit by FET or HEMT which requires fine wiring of the source electrode, the gate electrode, and the drain electrode. Therefore, as a result of reducing the area required for the wiring portion to about 2/3, high integration can be realized.

〔発明の効果〕〔The invention's effect〕

以上のように本発明によれば、ノーマリオフ特性の駆動
用熱電子放射型SITにノーマリオン特性の負荷用熱電
子放射型SITを直列接続した集積回路を形成するよう
にしたので、わざわざ別に抵抗を作ること無く同じ工程
で効率よく集積回路が形成できる上、高速、低電力にし
て高集積化可能な半導体集積回路が得られる。
As described above, according to the present invention, the driving thermionic emission type SIT having the normally-off characteristic and the thermistor emitting type SIT for the load having the normally-on characteristic are connected in series to form an integrated circuit, so that the resistors are purposely separated. It is possible to efficiently form an integrated circuit in the same process without making it, and obtain a semiconductor integrated circuit that can be highly integrated at high speed with low power consumption.

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

第1図は本発明の一実施例に係る半導体集積回路の断面
図、第2図はその等価回路図である。 1……基板、2……ドレイン領域、3……チャンネル領
域、4……ゲート領域、5……ソース領域、20……入
力端子、21……接地端子、22……出力端子、23…
…電源端子。
FIG. 1 is a sectional view of a semiconductor integrated circuit according to an embodiment of the present invention, and FIG. 2 is an equivalent circuit diagram thereof. 1 ... Substrate, 2 ... Drain region, 3 ... Channel region, 4 ... Gate region, 5 ... Source region, 20 ... Input terminal, 21 ... Ground terminal, 22 ... Output terminal, 23 ...
… Power supply terminal.

───────────────────────────────────────────────────── フロントページの続き (72)発明者 本谷 薫 宮城県仙台市米ヶ袋2丁目1番9号406 (56)参考文献 特開 昭57−186374(JP,A) 昭和50年電気四学会連合大会講演論文集 第537〜540頁 ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Inventor Kaoru Motoya 2-9-9 Yonegabukuro, Sendai-shi, Miyagi 406 (56) Reference JP-A-57-186374 (JP, A) Proceedings of the Federation Conference, pp. 537-540

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】真性或いは半絶縁性基板の一部に第1導電
型の高不純物密度領域よりなる第1ドレイン領域を設
け、その第1ドレイン領域上に第1チャンネル領域、第
1導電型の高不純物密度領域よりなる第1ソース領域を
縦型に、また、前記第1チャンネル領域周辺部には前記
第1チャンネル領域よりも禁制帯幅の大きい半導体で第
1ゲート領域を形成し、前記第1ソース領域と真の第1
ゲート領域間の寸法をキャリアの平均自由行程以下にし
てノーマリオフ型の駆動用熱電子放射型静電誘導トラン
ジスタを形成すると共に、この駆動用熱電子放射型静電
誘導トランジスタに隣接する領域には、前記第1ドレイ
ン領域を第2ソース領域とし、この第2ソース領域上に
第2チャンネル領域、第1導電型の高不純物密度領域よ
りなる第2ドレイン領域を縦型に、また、前記第2チャ
ンネル領域周辺部には前記第2チャンネル領域よりも禁
制帯幅の大きい半導体を用い前記第1ゲート領域よりも
薄型の第2ゲート領域を形成してノーマリオン型とした
負荷用熱電子放射型静電誘導トランジスタを形成し、前
記駆動用熱電子放射型静電誘導トランジスタの第1ゲー
ト領域に接して形成される電極に信号入力端子、第1ソ
ース領域に接して形成される電極に接地端子、第1ドレ
イン領域に接して形成される電極に出力端子、更に前記
負荷用熱電子放射型静電誘導トランジスタの第2ドレイ
ン領域に接して形成される電極に電源端子をそれぞれ設
けて集積回路を構成したことを特徴とする半導体集積回
路。
1. A first drain region formed of a high impurity density region of the first conductivity type is provided in a part of an intrinsic or semi-insulating substrate, and a first channel region and a first conductivity type are provided on the first drain region. A first source region formed of a high impurity density region is vertically formed, and a first gate region is formed in the peripheral portion of the first channel region with a semiconductor having a forbidden band width larger than that of the first channel region. 1 source region and true 1st
A dimension between the gate regions is equal to or less than the mean free path of carriers to form a normally-off type driving thermoelectron emission type electrostatic induction transistor, and in a region adjacent to the driving thermoelectron emission type electrostatic induction transistor, The first drain region is used as a second source region, a second channel region is formed on the second source region, a second drain region including a first-conductivity-type high impurity density region is formed vertically, and the second channel is formed. A thermionic emission type electrostatic load for electrostatic charging which is a normally-on type in which a second gate region thinner than the first gate region is formed using a semiconductor having a forbidden band width larger than that of the second channel region in the peripheral portion of the region. An induction transistor is formed, and an electrode formed in contact with the first gate region of the driving thermoelectron emission type electrostatic induction transistor is in contact with the signal input terminal and the first source region. The formed electrode is a ground terminal, the electrode formed in contact with the first drain region is an output terminal, and the electrode formed in contact with the second drain region of the thermionic emission type static induction transistor for load is a power supply terminal. A semiconductor integrated circuit characterized in that an integrated circuit is configured by providing each of them.
【請求項2】特許請求の範囲第1項記載において、チャ
ンネル領域がCaAs、ゲート領域がGa1-xAlxAs
ないしGa1-xAlxAs1-yyで形成されてなる半導体
集積回路。
2. The method according to claim 1, wherein the channel region is CaAs and the gate region is Ga 1 -x Al x As.
To Ga 1-x Al x As 1-y P y .
JP59153972A 1984-07-26 1984-07-26 Semiconductor integrated circuit Expired - Lifetime JPH0614534B2 (en)

Priority Applications (6)

Application Number Priority Date Filing Date Title
JP59153972A JPH0614534B2 (en) 1984-07-26 1984-07-26 Semiconductor integrated circuit
US06/759,090 US4712122A (en) 1984-07-26 1985-07-25 Heterojunction gate ballistic JFET with channel thinner than Debye length
GB8518841A GB2162370B (en) 1984-07-26 1985-07-25 Static induction transistor and integrated circuit comprising such a transistor
DE19853526826 DE3526826A1 (en) 1984-07-26 1985-07-26 STATIC INDUCTION TRANSISTOR AND SAME INTEGRATED CIRCUIT
FR8511514A FR2568410B1 (en) 1984-07-26 1985-07-26 STATIC INDUCTION TRANSISTOR AND ITS INTEGRATED CIRCUIT
US07/469,226 US5117268A (en) 1984-07-26 1990-01-24 Thermionic emission type static induction transistor and its integrated circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59153972A JPH0614534B2 (en) 1984-07-26 1984-07-26 Semiconductor integrated circuit

Publications (2)

Publication Number Publication Date
JPS6134980A JPS6134980A (en) 1986-02-19
JPH0614534B2 true JPH0614534B2 (en) 1994-02-23

Family

ID=15574099

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59153972A Expired - Lifetime JPH0614534B2 (en) 1984-07-26 1984-07-26 Semiconductor integrated circuit

Country Status (1)

Country Link
JP (1) JPH0614534B2 (en)

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS57186374A (en) * 1981-05-12 1982-11-16 Semiconductor Res Found Tunnel injection type travelling time effect semiconductor device

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
昭和50年電気四学会連合大会講演論文集第537〜540頁

Also Published As

Publication number Publication date
JPS6134980A (en) 1986-02-19

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