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JPS5939902B2 - Complementary insulated gate field effect semiconductor device - Google Patents
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JPS5939902B2 - Complementary insulated gate field effect semiconductor device - Google Patents

Complementary insulated gate field effect semiconductor device

Info

Publication number
JPS5939902B2
JPS5939902B2 JP50061660A JP6166075A JPS5939902B2 JP S5939902 B2 JPS5939902 B2 JP S5939902B2 JP 50061660 A JP50061660 A JP 50061660A JP 6166075 A JP6166075 A JP 6166075A JP S5939902 B2 JPS5939902 B2 JP S5939902B2
Authority
JP
Japan
Prior art keywords
conductivity type
type
region
electrode
field effect
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
Application number
JP50061660A
Other languages
Japanese (ja)
Other versions
JPS51137385A (en
Inventor
剛 山野
晶彦 安岡
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP50061660A priority Critical patent/JPS5939902B2/en
Publication of JPS51137385A publication Critical patent/JPS51137385A/en
Publication of JPS5939902B2 publication Critical patent/JPS5939902B2/en
Expired legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D89/00Aspects of integrated devices not covered by groups H10D84/00 - H10D88/00
    • H10D89/60Integrated devices comprising arrangements for electrical or thermal protection, e.g. protection circuits against electrostatic discharge [ESD]
    • H10D89/601Integrated devices comprising arrangements for electrical or thermal protection, e.g. protection circuits against electrostatic discharge [ESD] for devices having insulated gate electrodes, e.g. for IGFETs or IGBTs

Landscapes

  • Bipolar Transistors (AREA)
  • Metal-Oxide And Bipolar Metal-Oxide Semiconductor Integrated Circuits (AREA)

Description

【発明の詳細な説明】 本発明は金属、絶縁物、半導体を構成要素としたエンハ
ンスメントチャンネル相補型電界効果半導体装置に関し
、更に詳しくはゲート絶縁膜の保護装置を同一半導体基
板内に設けた相補型電界効果半導体装置に関している。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an enhancement channel complementary field effect semiconductor device whose constituent elements are metals, insulators, and semiconductors, and more specifically to a complementary field effect semiconductor device in which a gate insulating film protection device is provided within the same semiconductor substrate. It concerns field effect semiconductor devices.

従来の電界効果半導体装置て金属、絶縁物、半導体を構
成要素としたエンハンスメントチャンネル型半導体装置
においては、ゲート電極に高電圧を印加するとゲート電
極とチャンネル間を電気的に遮断している絶縁物が絶縁
破壊をおこし装置が永久的に破壊されてしまうという欠
点がある。
In conventional field-effect semiconductor devices, which consist of metals, insulators, and semiconductors, when a high voltage is applied to the gate electrode, the insulator that electrically isolates the gate electrode and channel breaks down. The disadvantage is that it causes dielectric breakdown and permanently destroys the device.

上記装置の取扱い中に静電的に帯電した作業者の衣服等
が上記絶縁物に接触しただけでも絶縁破壊を起こした。
上記絶縁物の絶縁破壊対策としてゲート電極とチャンネ
ル間にダイオードを接続し、ゲート電極にダイオードの
降伏電圧以上の電圧印加を防止している。この従来の保
護方法は、ゲート電極とチャンネル間にダイオードを接
続しダイオードの降伏電圧以上の電圧の印加を防ぎ絶縁
物を保護する方法であるから、ダイオードの降伏電圧が
絶縁物の絶縁破壊電圧より高い場合はその効果はない。
Even if electrostatically charged clothing of a worker came into contact with the insulator while handling the device, dielectric breakdown occurred.
As a measure against dielectric breakdown of the insulator, a diode is connected between the gate electrode and the channel to prevent application of a voltage higher than the breakdown voltage of the diode to the gate electrode. In this conventional protection method, a diode is connected between the gate electrode and the channel to protect the insulator by preventing the application of a voltage higher than the breakdown voltage of the diode. If it is high, there is no effect.

実際の素子の場合、比較的低濃度の基板を使用するため
絶縁物の絶縁破壊電圧よりダイオードの降伏電圧を低く
制御することは困難である。そこで、本発明の目的は、
エンハンスチヤンネル相補型電界効果半導体装置のゲー
ト電極に印加される過大電圧をゲート電極に印加する前
に確実に半導体基板側に流し、ゲート絶縁膜の破壊を防
止した電効果半導体装置を提供するものである。
In the case of actual devices, it is difficult to control the breakdown voltage of the diode to be lower than the breakdown voltage of the insulator because a substrate with a relatively low concentration is used. Therefore, the purpose of the present invention is to
To provide a field effect semiconductor device in which an excessive voltage applied to a gate electrode of an enhanced channel complementary field effect semiconductor device is reliably passed to the semiconductor substrate side before being applied to the gate electrode, thereby preventing breakdown of the gate insulating film. be.

本発明はエンハンスメントチヤンネル相補型電界効果ト
ランジスタが設けられている半導体基板に更に相補型バ
イポーラトランジスタを設け、このバイポーラトランジ
スタを介して上記電界効果トランジスタのゲート電極に
印加される過大電圧を制御する半導体妄置である。以下
に、本発明の実施例によつて本発明の構成乃至作用効果
につき更に説明する。
The present invention provides a semiconductor device that further provides a complementary bipolar transistor on the semiconductor substrate on which the enhancement channel complementary field effect transistor is provided, and controls an excessive voltage applied to the gate electrode of the field effect transistor via the bipolar transistor. It is a place. Hereinafter, the structure, operation and effect of the present invention will be further explained using examples of the present invention.

第1図乃至第2図は本発明に係わるエンハンスメントチ
ヤンネル相補型電界効果トランジスタの上面図及び縦断
面図を示している。
1 and 2 show a top view and a longitudinal sectional view of an enhancement channel complementary field effect transistor according to the present invention.

説明の都合上、要部を拡大して示している。図において
、P型拡散領域2を具備した長方形のN型シリコン基板
1の上部表面にSiO2膜3を形成し、該被膜3の一部
を除去し電極取出し孔4,5,6,7,8,9,10,
11,12,13を穿設する。
For convenience of explanation, important parts are shown enlarged. In the figure, a SiO2 film 3 is formed on the upper surface of a rectangular N-type silicon substrate 1 provided with a P-type diffusion region 2, and a part of the film 3 is removed to form electrode extraction holes 4, 5, 6, 7, 8. ,9,10,
Drill holes 11, 12, and 13.

該電極取出し孔には、P型拡散領域14,15,16,
17,18,19とN型拡散領域20,21,22,2
3,24,25の一部が露出する。さらに真空蒸着法に
より電極取出し孔4,5,6,7,8,9,10,11
,12,13と、P型拡散領域14,15間及びN型拡
散領域24,25間に介在するSiQ2被膜3上に金属
被膜を被着し電極26,27,28,29,30,31
を構成する。P型拡散領域14をP型ソース領域、15
をP型ドレイン領域、N型拡散領域25をN型ソース領
域、24をN型ドレイン領域とし、P型ドレイン領域1
5の電極取出し孔5とN型ドレイン領域24の電極取出
し孔12を金属被膜電極28で接続し、P型及びN型ド
レイン電極とする。P型ソース領域14とN型拡散領域
20の電極取出し孔4を金属被膜電極26で接続し、P
型ソース電極とする。また、N型ソース領域25とP型
拡散領域19の電極取出し孔13を金属被膜電極31で
接続しN型ソース電極とする。P型拡散領域17,19
はP型拡散領域2と、またN型拡散領20,22はN型
シリコン基板とそれぞれ導電的に接続するための領域で
ある。P型拡散領域2及びN型拡散領域23及びP型拡
散領域18で構成されるPNPバイポーラトランジスタ
のP型拡散領域2をP型コレクタ領域、N型拡散領域2
3をN型ベース領域、P型拡散領域18をP型エミツタ
領域とし、N型シリコン基板1及びP型拡散領域16及
びN型拡散領域21で構成されるNPNバイポーラトラ
ンジスタのN型シリコン基板1をN型コレクタ領域、P
型拡散領域16をP型ベース領域、N型拡散領域21を
N型エミツタ領域とする。P型ソース、ドレイン領域1
4,15間及びN型ソース、ドレイン領域25,24間
に介在するSlO2被膜3上の金属被膜をゲート電極と
する。前記ゲート電極と、該電極と同時に被着せしめた
金属被膜電極27でP型エミツタ領域18の電極取出し
孔11とN型エミツタ領域21の電極取出し孔6に接続
する。金属被膜電極27はゲート電極、N型エミツタ電
極、P型エミツタ電極となる。ゲート電極27の金属被
膜はSiO2被膜3を介して該被膜3の下方にあるP型
ソース、ドレイン領域14,15及びN型ソース、ドレ
イン領域25,24の一部に重なるようにする。P型ベ
ース領域16の電極取出し孔7とP型拡散領域17の電
極取出し孔9を金属被膜電極29で接続し、P型ベース
電極とする。
The electrode extraction hole has P-type diffusion regions 14, 15, 16,
17, 18, 19 and N type diffusion regions 20, 21, 22, 2
Parts of numbers 3, 24, and 25 are exposed. Further, electrode extraction holes 4, 5, 6, 7, 8, 9, 10, 11 are formed by vacuum evaporation method.
, 12, 13, and the SiQ2 coating 3 interposed between the P-type diffusion regions 14, 15 and the N-type diffusion regions 24, 25 to form electrodes 26, 27, 28, 29, 30, 31.
Configure. The P-type diffusion region 14 is a P-type source region, 15
is a P-type drain region, the N-type diffusion region 25 is an N-type source region, 24 is an N-type drain region, and the P-type drain region 1
The electrode extraction hole 5 of No. 5 and the electrode extraction hole 12 of the N-type drain region 24 are connected by a metal film electrode 28 to form a P-type and an N-type drain electrode. The P-type source region 14 and the electrode extraction hole 4 of the N-type diffusion region 20 are connected by a metal film electrode 26,
type source electrode. Further, the N-type source region 25 and the electrode extraction hole 13 of the P-type diffusion region 19 are connected by a metal film electrode 31 to form an N-type source electrode. P-type diffusion regions 17, 19
is a region to be electrically conductively connected to the P type diffusion region 2, and the N type diffusion regions 20 and 22 are respectively connected to the N type silicon substrate. The P-type diffusion region 2 of the PNP bipolar transistor, which is composed of the P-type diffusion region 2, the N-type diffusion region 23, and the P-type diffusion region 18, is the P-type collector region and the N-type diffusion region 2.
3 is an N-type base region, and the P-type diffusion region 18 is a P-type emitter region. N-type collector region, P
The type diffusion region 16 is used as a P type base region, and the N type diffusion region 21 is used as an N type emitter region. P-type source and drain region 1
The metal film on the SlO2 film 3 interposed between 4 and 15 and between the N-type source and drain regions 25 and 24 is used as a gate electrode. The gate electrode is connected to the electrode extraction hole 11 of the P-type emitter region 18 and the electrode extraction hole 6 of the N-type emitter region 21 by the metal film electrode 27 deposited at the same time as the gate electrode. The metal film electrode 27 serves as a gate electrode, an N-type emitter electrode, and a P-type emitter electrode. The metal film of the gate electrode 27 is made to overlap with a portion of the P-type source and drain regions 14 and 15 and the N-type source and drain regions 25 and 24 below the film 3 via the SiO2 film 3. The electrode extraction hole 7 of the P-type base region 16 and the electrode extraction hole 9 of the P-type diffusion region 17 are connected by a metal coating electrode 29 to form a P-type base electrode.

またN型ベース領域23の電極取出し孔10とN型拡散
領域22の電極取出し孔8を金属被膜電極30で接続し
、N型ベース電極とする。P型コレクタ領域2の電極は
、P型拡散領域19を介して接続されているN型ソース
電極31とする。またN型コレクタ1の電極はN型拡散
領域20を介して接続されているP型ソース電極26と
する。次にこの様に構成されたエンハンスメントチヤン
ネル相補型電界効果トランジスタの保護動作について説
明する。
Further, the electrode extraction hole 10 of the N-type base region 23 and the electrode extraction hole 8 of the N-type diffusion region 22 are connected by a metal coating electrode 30 to form an N-type base electrode. The electrode of the P-type collector region 2 is an N-type source electrode 31 connected via the P-type diffusion region 19 . Further, the electrode of the N-type collector 1 is assumed to be a P-type source electrode 26 connected via an N-type diffusion region 20. Next, the protection operation of the enhancement channel complementary field effect transistor configured as described above will be explained.

N型ソース電極31に対してP型ソース電極26に正の
電圧を印加する。
A positive voltage is applied to the P-type source electrode 26 with respect to the N-type source electrode 31 .

ゲート電極27の電圧を零とすると、N型ドレイン電極
28とN型ソース電極31間は電気的にしや断状態とな
り、P型ドレイン電極28とP型ソース電極26間は導
通する。またN型エミツタ電極27とP型ベース電極2
9は同電位となるので、NPNバイポーラトランジスタ
のN型エミツタ電極27とN型コレクタ電極26間はし
や断状態であり、N型ベース電極30はP型エミツタ電
極27に対してN型ソース電極31とP型ソース電極2
6間の電圧が逆方向に印加されているため、PNPバイ
ポーラトランジスタのP型エミツタ電極27とP型コレ
クタ電極31間も電気的にしや断状態となる。ここで、
ゲート電極27に負の過大電圧が印加されると、PNP
バイポーラトランジスタは、P型エミツタ電極27とN
型ベース電極30間の逆方向印加電圧が大きくなり、し
や断状態が続くが、NPNバイポーラトランジスタのN
型エミツタ電極27の電圧が負の電圧となるので、P型
ベース電極29からN型エミツタ電極27に電流が流れ
、N型コレクタ電極26とN型エミツタ電極27間が導
通しN型エミツタ電極27の電圧を零に保持する。次に
ゲート電極27にN型ソース電極31とP型ソース電極
26間と同電位の正の電圧を印加すると、N型ドレイン
電極28とN型ソース電極31間は導通し、P型ドレイ
ン電極28とP型ソース電極26間は電気的にしや断状
態となる。また、N型エミツタ電極27に対してP型ベ
ース電極29は、N型ソース電極31とP型ソース電極
26間の電圧が逆方向に印加されているため、NPNバ
イポーラトランジスタのN型エミツタ電極27とN型コ
レクタ電極26間はしや断状態であり、P型エミツタ電
極21とN型ベース電極30間は同電位となるので、P
NPバイポーラトランジスタのP型エミツタ電極27と
P型コレクタ電極31間もしや断状態となる。ここでゲ
ート電極27に過大の正の電圧が印加されると、NI)
NバイポーラトランジスタはN型エミツタ電極27とP
型ベース電極29間の逆方向印加電圧が大きくなりしや
断状態が続くが、PNPバイポーラトランジスタのP型
エミツタ電極27の電圧がN型ベース電極30に対して
正の電圧となるのでP型エミツタ電極27からN型ベー
ス電極30に電流が流れ、P型エミツタ電極27とP型
]レクタ電極31間が導通し、P型工゛ミツタ電極27
の電圧をN型ソース電極31とP型ソース電極26間の
電圧に保持する。以上、ゲート電極27の電圧を上記N
PN及びPNPバイポーラトランジスタの導通により制
限するものである。
When the voltage of the gate electrode 27 is set to zero, the N-type drain electrode 28 and the N-type source electrode 31 are electrically disconnected, and the P-type drain electrode 28 and the P-type source electrode 26 are electrically connected. In addition, the N-type emitter electrode 27 and the P-type base electrode 2
9 are at the same potential, the N-type emitter electrode 27 and the N-type collector electrode 26 of the NPN bipolar transistor are in a disconnected state, and the N-type base electrode 30 is the N-type source electrode with respect to the P-type emitter electrode 27. 31 and P-type source electrode 2
6 is applied in the opposite direction, the P-type emitter electrode 27 and the P-type collector electrode 31 of the PNP bipolar transistor are also electrically disconnected. here,
When a negative excessive voltage is applied to the gate electrode 27, the PNP
The bipolar transistor has a P type emitter electrode 27 and an N
The voltage applied in the reverse direction across the type base electrode 30 increases and the shearing state continues, but the NPN bipolar transistor
Since the voltage of the type emitter electrode 27 becomes a negative voltage, a current flows from the P type base electrode 29 to the N type emitter electrode 27, and conduction occurs between the N type collector electrode 26 and the N type emitter electrode 27. hold the voltage at zero. Next, when a positive voltage having the same potential as that between the N-type source electrode 31 and the P-type source electrode 26 is applied to the gate electrode 27, conduction occurs between the N-type drain electrode 28 and the N-type source electrode 31, and the P-type drain electrode 28 There is an electrically disconnected state between the P-type source electrode 26 and the P-type source electrode 26. Further, since the voltage between the N-type source electrode 31 and the P-type source electrode 26 is applied in the opposite direction to the P-type base electrode 29 with respect to the N-type emitter electrode 27, the N-type emitter electrode 27 of the NPN bipolar transistor and the N-type collector electrode 26 are in a disconnected state, and the P-type emitter electrode 21 and the N-type base electrode 30 are at the same potential.
The P-type emitter electrode 27 and the P-type collector electrode 31 of the NP bipolar transistor are now in a disconnected state. If an excessively positive voltage is applied to the gate electrode 27 here, NI)
The N bipolar transistor has an N type emitter electrode 27 and a P
The voltage applied in the reverse direction between the type base electrodes 29 increases and the disconnection state continues, but since the voltage of the P type emitter electrode 27 of the PNP bipolar transistor becomes a positive voltage with respect to the N type base electrode 30, the P type emitter A current flows from the electrode 27 to the N-type base electrode 30, conduction occurs between the P-type emitter electrode 27 and the P-type rectifier electrode 31, and the P-type emitter electrode 27
is maintained at the voltage between the N-type source electrode 31 and the P-type source electrode 26. As described above, the voltage of the gate electrode 27 is set to the above N
This is limited by the conduction of PN and PNP bipolar transistors.

以上の説明は、N型シリコン基板を使用した相補型電界
効果半導体装置について行なつたが、P型シリコン基板
を使用した相補型電界効果半導体装置についても適用で
きる。
Although the above description has been made regarding a complementary field effect semiconductor device using an N-type silicon substrate, it can also be applied to a complementary field-effect semiconductor device using a P-type silicon substrate.

前述したSiO2被膜はこれのみに限定するものでなく
電気的絶縁物であればよい。半導体材料としてはシリコ
ンのみに限定するものでなく、ゲルマニウム等他の半導
体材料を用いてもよい。
The SiO2 film described above is not limited to this, and any electrical insulator may be used. The semiconductor material is not limited to silicon, and other semiconductor materials such as germanium may be used.

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

第1図は本発明にかかわる装置の土面図、第2図は第1
図のA−N断面図、第3図゛は本発明にか/かわる装置
の回路図である。 尚、各図において同一符号は同一又は相当部分を示し、
1はN型シリコン基板、2はP型拡散領域、3はSiO
2膜、4乃至13は電極取出し孔、14乃至19はP型
拡散領域、20乃至25はN型拡散領域、26乃至31
は金属被膜電極である。
Figure 1 is a soil surface diagram of the device related to the present invention, and Figure 2 is the soil level diagram of the device related to the present invention.
FIG. 3 is a sectional view taken along the line AN in the figure, and is a circuit diagram of a device according to/alternative to the present invention. In each figure, the same reference numerals indicate the same or equivalent parts.
1 is an N-type silicon substrate, 2 is a P-type diffusion region, 3 is SiO
2 membranes, 4 to 13 electrode extraction holes, 14 to 19 P type diffusion regions, 20 to 25 N type diffusion regions, 26 to 31
is a metal coated electrode.

Claims (1)

【特許請求の範囲】[Claims] 1 第2導電型領域を具備した第1導電型半導体基板の
前記基板に第2導電型のソース領域、ドレイン領域及び
上記ソース領域、ドレイン領域間の上記基板表面に絶縁
層を介して設けられたゲート電極とから成る第1の絶縁
ゲート型電界効果トランジスタ、及び前記第2導電型領
域に第1導電型のソース領域、ドレイン領域及び上記ソ
ース領域、ドレイン領域間の上記第2導電型領域表面に
絶縁層を介して設けられたゲート電極とから成る第2の
絶縁ゲート型電界効果トランジスタを設け、上記第1及
び第2絶縁ゲート型電界効果トランジスタのそれぞれの
ドレイン領域及びそれぞれのゲート電極同士を電気的に
接続して成る相補型絶縁ゲート型電界効果半導体に於て
、第1導電型基板に第1導電型の領域を含む領域を形成
し、第1導電型基板と第1導電型の領域を含む領域で構
成されるバイポーラトランジスタの第1導電型基板をコ
レクタとして、第1導電型のエミッタ、第2導電型のベ
ースから成る第1のトランジスタ、及び第2導電型領域
に第2導電型の領域を含む領域を形成し、第2導電型領
域と第2導電型の領域を含む領域で構成されるバイポー
ラトランジスタの第2導電型領域をコレクタとして、第
2導電型のエミッタ、第1導電型のベースから成る第2
のトランジスタをそれぞれ設け、前記第1導電型及び第
2導電型のエミッタを前記ゲート電極と接続するととも
に第1導電型ベースを第1導電型基板に、また第2導電
型ベースを第2導電型領域にそれぞれ接続したことを特
徴とする相補型絶縁ゲート型電界効果半導体装置。
1 A source region and a drain region of a second conductivity type are provided on the substrate of a first conductivity type semiconductor substrate having a second conductivity type region and an insulating layer is provided on the surface of the substrate between the source region and the drain region. a first insulated gate field effect transistor comprising a gate electrode, a source region and a drain region of a first conductivity type in the second conductivity type region, and a surface of the second conductivity type region between the source region and the drain region; A second insulated gate field effect transistor comprising a gate electrode provided through an insulating layer is provided, and the respective drain regions of the first and second insulated gate field effect transistors and the respective gate electrodes are electrically connected to each other. In a complementary insulated gate field effect semiconductor which is connected to each other, a region including a region of the first conductivity type is formed in the substrate of the first conductivity type, and a region of the first conductivity type is connected to the substrate of the first conductivity type. A bipolar transistor has a first conductivity type substrate as a collector, a first conductivity type emitter, a second conductivity type base, and a second conductivity type region as a collector. The second conductivity type region of the bipolar transistor, which is composed of a second conductivity type region and a second conductivity type region, is used as a collector, a second conductivity type emitter, and a first conductivity type emitter. The second consisting of the base of
transistors are provided, the emitters of the first conductivity type and the second conductivity type are connected to the gate electrode, and the base of the first conductivity type is connected to the substrate of the first conductivity type, and the base of the second conductivity type is connected to the substrate of the second conductivity type. A complementary insulated gate field effect semiconductor device characterized in that each region is connected to the other.
JP50061660A 1975-05-22 1975-05-22 Complementary insulated gate field effect semiconductor device Expired JPS5939902B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP50061660A JPS5939902B2 (en) 1975-05-22 1975-05-22 Complementary insulated gate field effect semiconductor device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP50061660A JPS5939902B2 (en) 1975-05-22 1975-05-22 Complementary insulated gate field effect semiconductor device

Publications (2)

Publication Number Publication Date
JPS51137385A JPS51137385A (en) 1976-11-27
JPS5939902B2 true JPS5939902B2 (en) 1984-09-27

Family

ID=13177588

Family Applications (1)

Application Number Title Priority Date Filing Date
JP50061660A Expired JPS5939902B2 (en) 1975-05-22 1975-05-22 Complementary insulated gate field effect semiconductor device

Country Status (1)

Country Link
JP (1) JPS5939902B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62165969A (en) * 1986-01-17 1987-07-22 Sanyo Electric Co Ltd CMOS semiconductor device

Also Published As

Publication number Publication date
JPS51137385A (en) 1976-11-27

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