JPS5896766A - Semiconductor device - Google Patents

Semiconductor device

Info

Publication number
JPS5896766A
JPS5896766A JP56194992A JP19499281A JPS5896766A JP S5896766 A JPS5896766 A JP S5896766A JP 56194992 A JP56194992 A JP 56194992A JP 19499281 A JP19499281 A JP 19499281A JP S5896766 A JPS5896766 A JP S5896766A
Authority
JP
Japan
Prior art keywords
substrate
drain
type
layer
voltage
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
Application number
JP56194992A
Other languages
Japanese (ja)
Other versions
JPH0612821B2 (en
Inventor
Toshio Baba
寿夫 馬場
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.)
NEC Corp
Original Assignee
NEC Corp
Nippon Electric Co 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 NEC Corp, Nippon Electric Co Ltd filed Critical NEC Corp
Priority to JP56194992A priority Critical patent/JPH0612821B2/en
Publication of JPS5896766A publication Critical patent/JPS5896766A/en
Publication of JPH0612821B2 publication Critical patent/JPH0612821B2/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]
    • H10D30/60Insulated-gate field-effect transistors [IGFET]
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D12/00Bipolar devices controlled by the field effect, e.g. insulated-gate bipolar transistors [IGBT]
    • H10D12/211Gated diodes

Landscapes

  • Insulated Gate Type Field-Effect Transistor (AREA)
  • Bipolar Transistors (AREA)

Abstract

PURPOSE:To obtain the semiconductor device enable to perform high speed action and enabled to form in high density by a method wherein a P<+> type layer and an N<+> type layer are provided at a part of a P type Si substrate, and a gate electrode is provided between both interposing an SiO2 film between them. CONSTITUTION:The P<+> type source 12 is held at zero potential, and the N<+> type drain 13 is made to have positive potential. Potential of the P type substrate is decided nearly by potential of the source. When the absolute value of the voltage of the gate electrode 5 is small, and no high concentration carrier region exists in the surface of the substrate, a thick depletion layer is generated at the junction of the substrate and the drain to make no drain current to flow. When a sufficiently negative voltage is applied to the gate electrode 5, and holes are stored in high concentration in the surface of the substrate, the drain current begins to flow. Moreover when a voltage higher than the threshold is applied to the electrode 5 to form an inversion layer of electrons in the surface of the substrate, the depletion layer is not extended, and the drain current can be controlled. The device thereof is not conducted completely up to generation of an avalanche or the tunnel effect of carriers, and indicates an ideal characteristic (a dotted line) without generating an weak inversion region as usual. However because the device is provided with no current limiting structure, it is necessary to insert a resistor in series.

Description

【発明の詳細な説明】 本発明は高速度動作の可能な新規半導体装置の構造に関
するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a novel semiconductor device structure capable of high-speed operation.

能蛎半導体装置の1つとしてM OS (MetalO
xide  Sem1conductor )トランジ
スタがあるが、その構造の単純性及び製造フロセスが比
較的簡単なことにより、集積回路の構成素子として広く
用(1) いられており、集積回路を高集積化すべく素子寸法の縮
小が創られ、また動作の高速化が計られている。
MOS (MetalO
Due to its simple structure and relatively easy manufacturing process, it is widely used as a component of integrated circuits(1). A reduction has been created and an attempt has been made to speed up the operation.

第1図に従来構造のMOS)>ンジスタの概略構造及び
動作を説明する模式図を示す。第1図において1は一導
電型を有する半導体基板、2は該基板1と異る第2の導
電型を有する不純物含有領域、3は該不純物含有領域2
と同じ導電型を有する不純物含有領域、4は基板1の上
に形成された絶縁膜、5はゲート電極である。なお、電
気回路における表現では不純物含有領域2はソース、不
純物含有領域3はドレイン電極、5はゲート電極と呼ば
れている。
FIG. 1 shows a schematic diagram illustrating the general structure and operation of a conventional MOS transistor. In FIG. 1, 1 is a semiconductor substrate having one conductivity type, 2 is an impurity-containing region having a second conductivity type different from the substrate 1, and 3 is the impurity-containing region 2.
4 is an insulating film formed on the substrate 1, and 5 is a gate electrode. In addition, in terms of an electric circuit, the impurity-containing region 2 is called a source, the impurity-containing region 3 is called a drain electrode, and 5 is called a gate electrode.

半導体基板1にP型を用いてこのMOS トランジスタ
の動作を説明すると次のようになる。基板1とソース2
を零電位とし、ドレイン3には正電圧が印加されている
。いま、ゲート5に負の電圧を加え基板表面に反転層が
形成されないようにすると、ソース2とドレイン3との
間の半導体基板1の表面にはソース及びドレインにおけ
る多数キヤ(2) リアである電子がほとんど存在しないため、ソース2と
ドレイン3との間には電流は流れない。さて、ケート5
にしきい値以上の正電圧を加え基板表面1こ反転層を形
成すると、反転層内には電子が多数存在するためソース
2とトレインとの間は電子の移動による電流が流れるよ
うになる。しかし、この2つの状態はステップ状に変イ
〕るのではなくケート電圧がしきい値近傍である場合に
は基板表面には弱い反転層が形成され、ソース2とドレ
イン3との間には該反転層内の電子の数に制限された電
流(ドレイン電流)が流れる。このように、ドレイン電
流がゲート電圧の変化と共に変化する弱反転領域が存在
する。
The operation of this MOS transistor using a P-type semiconductor substrate 1 will be explained as follows. Substrate 1 and source 2
is set to zero potential, and a positive voltage is applied to the drain 3. Now, if a negative voltage is applied to the gate 5 to prevent the formation of an inversion layer on the substrate surface, the surface of the semiconductor substrate 1 between the source 2 and the drain 3 will have a majority carrier (2) in the source and drain. Since there are almost no electrons, no current flows between the source 2 and the drain 3. Now, Kate 5
When a positive voltage higher than a threshold value is applied to the substrate surface 1 to form an inversion layer, a large number of electrons exist in the inversion layer, so a current flows between the source 2 and the train due to the movement of electrons. However, these two states do not change stepwise; instead, when the gate voltage is near the threshold, a weak inversion layer is formed on the substrate surface, and between the source 2 and drain 3. A current (drain current) that is limited to the number of electrons in the inversion layer flows. Thus, there is a weak inversion region where the drain current changes with changes in gate voltage.

第2図は従来構造MOSトランジスタのゲート電圧(■
G)に対するドレインX流(log Ib)の弱反転特
性である。第2図において実線は従来構造MOSトラン
ジスタの特性、点線は理想的なスイッチングトランジス
タの特性、aはソース2およびドレイン3の接合におけ
るリーク電流が流れる領域、bは弱反転領域、■Tはし
きい値電圧、Cは大(3) きなドレイン電MLか流れ得る反転層が形成されている
強反転領域である。スイッチング動作としてはaとCの
三領域を用いるたりでbは本質的には不要である。しか
し、実際上これを除去することは困難であるO MOS
 )ランジスタが微細化され、動作電圧が低くなると、
遷移領域すは狭くならないためにaとCの各領域の動作
マージンが狭くなる。したがって遷移領域の存在しない
特性(点線)が実現できれは極めて有効である。
Figure 2 shows the gate voltage (■
G) is a weak inversion characteristic of the drain X flow (log Ib). In Figure 2, the solid line is the characteristic of a conventionally structured MOS transistor, the dotted line is the characteristic of an ideal switching transistor, a is the region where leakage current flows at the junction of source 2 and drain 3, b is the weak inversion region, and ■T is the threshold. The value voltage C is a strong inversion region in which an inversion layer is formed in which a large drain current ML can flow. For the switching operation, three regions a and C are used, and b is essentially unnecessary. However, it is difficult to remove this in practice from OMOS
) As transistors become smaller and their operating voltage becomes lower,
Since the transition region S is not narrowed, the operating margins of each region a and C are narrowed. Therefore, it would be extremely effective to realize a characteristic (dotted line) in which no transition region exists.

本発明は、かかる従来のM 08 )ランジスタの持つ
欠点を除去し、高速動作及び高密度化が可能な新しい動
作原理に基づく新規半導体装置を提供するものである。
The present invention eliminates the drawbacks of the conventional M 08 ) transistor and provides a new semiconductor device based on a new operating principle that enables high-speed operation and high density.

その要旨は、半導体基板と、該半導体基板表面の一部1
こ設けられた当該基板と同型の第一の高濃度不純物含有
領域と、前記半導体基板表面の他の一部に設けられた当
該基板と異る第2の導電型を有する第2の高濃度不純物
含有領域と、前記第1と第2の高濃度キャリヤ領域との
間の半導体基板表面に絶縁膜を介して設けられたゲート
′kt&と(4) からなる半導体装置を提供するものである。この半導体
装[1こおL(ではゲート電極にかける電圧1こよって
、第1と第2の^m度不純物領域との間に流れる電流を
制御し、従来構造のような遷移領域を持たない特性を実
現することが可能となる。
The gist is a semiconductor substrate and a portion of the surface of the semiconductor substrate.
a first high-concentration impurity-containing region having the same type as the substrate and a second high-concentration impurity having a second conductivity type different from that of the substrate provided on another part of the surface of the semiconductor substrate; The present invention provides a semiconductor device comprising a gate 'kt&' (4) provided on the surface of a semiconductor substrate between a containing region and the first and second high concentration carrier regions with an insulating film interposed therebetween. In this semiconductor device [1×L], the current flowing between the first and second impurity regions is controlled by applying a voltage of 1× to the gate electrode, and it does not have a transition region like the conventional structure. It becomes possible to realize the characteristics.

以下本発明の動作原理を実施例図面を参照して詳細に説
明する。
The operating principle of the present invention will be explained in detail below with reference to the drawings of the embodiments.

第3図は本発明の一実施例を示す断面模式図である1、
第3図において第1図と1ilじ1号のものは第1図と
同等物で10」−機能を示す。11は一部を型を有する
基板、12は該基鈑11と同じ導電性を有する第1の高
濃度不純物含有領域、13は該^#良度純物含有領域1
2とは異る第2の導電型を有する第2の高濃度不純物含
有領域である。2つの高濃度不純物含有領域12.13
の基板1との接合における不純物#農はI X 10’
%n−3以上でその分布はステク7′状であることが望
ましい。この実現は容易ではないか、基板1表面に拡散
定数の小さい砒素をイオンイ/グランテーシビンして接
合を作る場合、表l1II磯凝I X 10”鍋−3で
接合深さ03μmであれはは(5) ぼこの条件を満足する。なお、2つの高濃度不純物含有
領域12.13はそれぞれソース、ドレインと呼ぶ。
FIG. 3 is a schematic cross-sectional view showing one embodiment of the present invention.
In FIG. 3, the one shown in FIG. 1 and No. 1 is equivalent to that in FIG. 11 is a substrate partially having a mold, 12 is a first high-concentration impurity-containing region having the same conductivity as the substrate 11, and 13 is the ^# benign purity-containing region 1.
This is a second high concentration impurity-containing region having a second conductivity type different from No. 2. Two high concentration impurity containing regions 12.13
The impurity in the bonding with substrate 1 is I x 10'
%n-3 or more, it is desirable that the distribution be in the shape of a stem 7'. Isn't it easy to realize this?If you make a bond by ionizing/granting arsenic with a small diffusion constant on the surface of the substrate 1, Table 1 II Isoko I (5) Satisfy the Boko condition.The two high-concentration impurity-containing regions 12 and 13 are called a source and a drain, respectively.

半導体基板11にP型を用いてこの新規半導体装置の動
作を説明すると次のようになる1、ソース12とドレイ
ン13の間のバイアス電圧(ドレイン電圧)は、p  
nの接合が逆バイアスとなるようソース12は零電位、
ドレイン13が正電圧となっている。
The operation of this new semiconductor device using a P-type semiconductor substrate 11 is explained as follows. 1. The bias voltage (drain voltage) between the source 12 and the drain 13 is p
The source 12 is at zero potential so that the n junction is reverse biased.
The drain 13 is at a positive voltage.

なお、基板1は電極を接続しないがその電位はほぼソー
ス12の電位で決する。いま、ゲート電極5の電圧の絶
対値が小さく、基板表面に蓄積層又は反転層の高濃度キ
ャリヤ領域が形成されてないとすると、基板11とドレ
イン13とのp−n+接合において厚い空乏層が基板1
1内に形成されるので、ソース12とドレイン13の間
を電流(ドレイン電流)は流れない。一方、ゲート電極
5に充分に大きい負電圧を印加し、基板表面に高濃度の
止孔の蓄積層を形成すると、基板表面における該蓄積層
とドレイン13との接合は等測的なp+−n+接合とな
り、表面における空乏層はほとんど広がらす、この接(
6) 合は高電界となる。この空乏層の幅が数十へ以下となる
とこの空乏層内をキャリアはトンネルで通過でき、また
空乏層幅がこれ以上でも電界が1thyycm以上にな
るとアバランシェが起こり、ソース12とドレイン13
の間に電流が流れるようになる。またゲート電極5にし
きい値電圧より高い電圧を印加し、基板表面1こ高濃度
の電子の反転層を形成すると、該反転層とドレイン13
とは接続され、基板表面における接合はソース12と前
記反転層との間に形成され等測的なl)++−接合とな
り、表面における空乏層はほとんど広がらずこの接合は
高電界となる。この結果、該接合において前述の蓄積層
とドレイン13との接合さ同様アバランシ・又はキャリ
アのトンネルが起こり、ソース12とドレイン13の間
に電流が流れるようになる。このようにゲート電圧によ
りドレイン電流I流を制御することができる。
Although no electrode is connected to the substrate 1, its potential is determined approximately by the potential of the source 12. Now, assuming that the absolute value of the voltage of the gate electrode 5 is small and a high concentration carrier region of an accumulation layer or an inversion layer is not formed on the substrate surface, a thick depletion layer is formed at the p-n+ junction between the substrate 11 and the drain 13. Board 1
1, no current (drain current) flows between the source 12 and drain 13. On the other hand, if a sufficiently large negative voltage is applied to the gate electrode 5 to form a highly concentrated pore-stopping accumulation layer on the substrate surface, the junction between the accumulation layer and the drain 13 on the substrate surface is an isometric p+-n+ This junction (
6) A high electric field will result. When the width of this depletion layer is less than several tens of tens of meters, carriers can tunnel through this depletion layer, and even if the width of the depletion layer is larger than this, avalanche occurs and the source 12 and drain 13
Current will begin to flow between. Furthermore, when a voltage higher than the threshold voltage is applied to the gate electrode 5 to form an electron inversion layer with a high concentration on the substrate surface, the inversion layer and the drain 13
The junction at the substrate surface is formed between the source 12 and the inversion layer and becomes an isometric l)++-junction, and the depletion layer at the surface hardly spreads and this junction becomes a high electric field. As a result, similar to the junction between the storage layer and the drain 13 described above, avalanche or carrier tunneling occurs at this junction, and current flows between the source 12 and the drain 13. In this way, the drain current I can be controlled by the gate voltage.

本発明はこのような原理によっているため、アバランシ
ェ又はキャリアのトンネルが起こる才では全く電流が流
れず、第2図すのような弱反転類(7) 域は存在せず、第2図の理想特性(点111iりに近い
特性が得られる。ただし、本発明1こよる半導体装置で
は素子の導通状態で電流を制限する機構が無いので、こ
の電流制限のための抵抗、又は能動デバイスの特価的な
抵抗を直列に入れておくのが望ましい。
Since the present invention is based on this principle, when avalanche or carrier tunneling occurs, no current flows at all, and the weak inversion class (7) region shown in Figure 2 does not exist, and the ideal shown in Figure 2 is avoided. Characteristics (characteristics close to point 111i can be obtained. However, since the semiconductor device according to the present invention does not have a mechanism to limit the current when the element is in a conductive state, it is necessary to use a resistor for limiting the current or a special price of the active device. It is desirable to insert a resistor in series.

本発明による新規半導体装置においては微細化及び高速
化が計れる可能性を有するが、この他に従来の能動半導
体装置にないいくつかの特徴を有している。第1は動作
がゲート電圧に関して両極性であることであり、第2は
基板の導電型によらず同一プロセスで形成できることで
あり、第3はドレイン電流がアバランシェ又はトンネル
効果により電流が流れるため、ドレイン電圧に対するド
レイン電流の特性は非飽和特性であることである。
The novel semiconductor device according to the present invention has the potential for miniaturization and high speed, but also has several other features not found in conventional active semiconductor devices. The first is that the operation is bipolar with respect to the gate voltage, the second is that it can be formed in the same process regardless of the conductivity type of the substrate, and the third is that the drain current flows due to avalanche or tunnel effect. The characteristics of drain current with respect to drain voltage are non-saturation characteristics.

以上、本発明による′#規半導体装置の構造及び動作に
ついてP型基板を用いて説明してきたが、基板をn型に
した場合も同様に実現できることは明らかである。また
、半導体基板の替りに薄膜又は厚膜半導体で構成しても
本発明によるMr規牛導(8) 体装置が実現できることも明らかである。
Although the structure and operation of the semiconductor device according to the present invention have been described above using a P-type substrate, it is clear that the structure and operation of the semiconductor device according to the present invention can be similarly realized even when the substrate is an n-type substrate. It is also clear that the Mr. conductor device according to the present invention can be realized by using a thin film or thick film semiconductor instead of a semiconductor substrate.

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

第1図は従来構造MO8トランジスタの模式図であり、
lは一導電型を有する半導体基板、2は該基板1と異る
第2の導電型を有する不純物含有領域、3は該不純物含
有領域2と同じ極性を有する不純物含有領域、4は基板
1の上に形成された絶縁膜、5はゲート電極である。 第2図は従来構造MO8)ランジスタのドレイン電圧に
対するドレイン電流の弱反転特性であり、実線は従来構
造MO8)2ンジスタの特性、点線は理想的なスイッチ
ングトランジスタの特性、aはソースおよびドレインの
接合リーク電流の流れる領域、bは弱反転領域、VTは
 しきい値電圧、Cは強攻転領域である。 第3図は本発明の一東施例を示す断面模式図であり、第
1図と同じ番号のものは同等物で同一機能を示し、11
は一導電型を有する基板、12は該基板と同じ導電型を
有する第1の高濃度不純物含有(9) (10)
FIG. 1 is a schematic diagram of a conventional structure MO8 transistor,
1 is a semiconductor substrate having one conductivity type, 2 is an impurity-containing region having a second conductivity type different from that of the substrate 1, 3 is an impurity-containing region having the same polarity as the impurity-containing region 2, and 4 is a semiconductor substrate of the substrate 1; The insulating film formed thereon, 5, is a gate electrode. Figure 2 shows the weak reversal characteristics of the drain current with respect to the drain voltage of the conventional structure MO8) transistor, the solid line is the characteristic of the conventional structure MO8)2 transistor, the dotted line is the characteristic of an ideal switching transistor, and a is the junction of the source and drain. The region where leakage current flows, b is the weak reversal region, VT is the threshold voltage, and C is the strong reversal region. FIG. 3 is a schematic cross-sectional view showing the first embodiment of the present invention. Items with the same numbers as in FIG. 1 are equivalent and have the same functions, and 11
12 is a first high-concentration impurity-containing substrate having the same conductivity type as the substrate (9) (10)

Claims (1)

【特許請求の範囲】[Claims] 半導体基板と、該半導体基板表面の一部に設けられた当
該基板と同型の第1の高濃度不純物含有領域さ、前記半
導体基板表面の他の一部に設けられた当該基板と逆型の
第2の高濃度不純物含有領域と、前記第1と第2の高濃
度不純物含有領域との間の半導体基板表面に絶縁膜を介
して設けられた電極とからなることを特徴きする半導体
装置。
a semiconductor substrate, a first high-concentration impurity-containing region of the same type as the substrate provided on a part of the surface of the semiconductor substrate, and a first high concentration impurity-containing region of the opposite type to the substrate provided on another part of the surface of the semiconductor substrate. 1. A semiconductor device comprising: two high concentration impurity containing regions; and an electrode provided on the surface of the semiconductor substrate between the first and second high concentration impurity containing regions with an insulating film interposed therebetween.
JP56194992A 1981-12-03 1981-12-03 Semiconductor device Expired - Lifetime JPH0612821B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56194992A JPH0612821B2 (en) 1981-12-03 1981-12-03 Semiconductor device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56194992A JPH0612821B2 (en) 1981-12-03 1981-12-03 Semiconductor device

Publications (2)

Publication Number Publication Date
JPS5896766A true JPS5896766A (en) 1983-06-08
JPH0612821B2 JPH0612821B2 (en) 1994-02-16

Family

ID=16333730

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56194992A Expired - Lifetime JPH0612821B2 (en) 1981-12-03 1981-12-03 Semiconductor device

Country Status (1)

Country Link
JP (1) JPH0612821B2 (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04277680A (en) * 1991-03-05 1992-10-02 Nec Corp Tunnel transistor and manufacture of the same
US5616944A (en) * 1990-05-21 1997-04-01 Canon Kabushiki Kaisha Diode and semiconductor device having a controlled intrinsic or low impurity concentration region between opposite conductivity type semiconductor regions
US5686739A (en) * 1991-08-06 1997-11-11 Nec Corporation Three terminal tunnel device

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* Cited by examiner, † Cited by third party
Title
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SUPPLEMENT TO THE JOURNAL OF THE JAPAN SOCIETY OF APPLIED PHYSICS=1974 *

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5616944A (en) * 1990-05-21 1997-04-01 Canon Kabushiki Kaisha Diode and semiconductor device having a controlled intrinsic or low impurity concentration region between opposite conductivity type semiconductor regions
EP0458570B1 (en) * 1990-05-21 1997-10-08 Canon Kabushiki Kaisha Diode and semiconductor device having such a diode
JPH04277680A (en) * 1991-03-05 1992-10-02 Nec Corp Tunnel transistor and manufacture of the same
US5686739A (en) * 1991-08-06 1997-11-11 Nec Corporation Three terminal tunnel device

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