JPS62234370A - Gto thyristor - Google Patents

Gto thyristor

Info

Publication number
JPS62234370A
JPS62234370A JP7781786A JP7781786A JPS62234370A JP S62234370 A JPS62234370 A JP S62234370A JP 7781786 A JP7781786 A JP 7781786A JP 7781786 A JP7781786 A JP 7781786A JP S62234370 A JPS62234370 A JP S62234370A
Authority
JP
Japan
Prior art keywords
electrode
gate electrode
gate
base layer
outer circumference
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.)
Pending
Application number
JP7781786A
Other languages
Japanese (ja)
Inventor
Yoshikazu Takahashi
良和 高橋
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.)
Fuji Electric Co Ltd
Original Assignee
Fuji 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 Fuji Electric Co Ltd filed Critical Fuji Electric Co Ltd
Priority to JP7781786A priority Critical patent/JPS62234370A/en
Publication of JPS62234370A publication Critical patent/JPS62234370A/en
Pending legal-status Critical Current

Links

Landscapes

  • Thyristors (AREA)

Abstract

PURPOSE:To facilitate drawing-out of a large current by a method wherein the outer circumference of a base layer is extended to the same plane as emitter layers and a gate electrode is extended onto that plane and a gate electrode unit which is unified with but electrically insulated from an electrode unit pressed against a main electrode is pressed and contacted with the extension of the gate electrode. CONSTITUTION:The outer circumference of a silicon substrate 1 which has 4 layers of PNPN has a PNP structure and the circumference of a P-type base layer 12 is extended to the same plane as emitter layers 11. Bevel shape formed on the side surface of the lower layers is extended onto the side surface of the outer circumference of the P-type base layer 12. A gate electrode 22 formed on the bottom of a recessed part 13 is connected to a gate elec trode 23 formed on the outer circumference of the P-type base layer 12 through an Al layer 24. As the outer circumference is the gate part, the effective area of cathode is not reduced. A gate contact electrode unit 8 is formed solidly on the outer circumference of a contact electrode unit 3 with an insulator 7. As a lower surface electrode 81 is pressed against the gate electrode 23 on the same plane as cathodes 21, the gate electrode 23 receives the same pressure as the cathodes and is contacted with the electrode layer 81. With this constitution, a large contact area can be obtained and a large current can be drawn out.

Description

【発明の詳細な説明】[Detailed description of the invention] 【発明の属する技術分野】[Technical field to which the invention pertains]

本発明は、分割されたエミッタ層に設けられる一方の主
電極と、そのエミッタ層を取り囲むベース層に設けられ
るゲート電極とを備え、主電極に電極体が圧接するGT
Oサイリスタに関する。
The present invention provides a GT comprising one main electrode provided on a divided emitter layer and a gate electrode provided on a base layer surrounding the emitter layer, and in which an electrode body is in pressure contact with the main electrode.
Regarding O thyristor.

【従来技術とその問題点】[Prior art and its problems]

GTOサイリスタの大電流化が進むにつれてゲート引出
し電流も大きくなってきた。従来公知のGTOサイリス
タのゲート構造は、第2図に示す中心ゲート構造、第3
図に示す外周部ワイヤボンディング構造、第4図に示す
中間リング構造がある。中心ゲート構造では、pnpn
4層を有するシリコン基板lのnエミッタ層11に設け
られているカソード電極21に圧接する電極層31を有
する接触体3の中央に設けられた凹部32内に収容した
皿ばね5により、ゲート導体4の先端の電極体41がp
ベース層12に設けられたり蒸着層などからなるゲート
電極22の中央部に圧接する。しかしこの構造ではゲー
ト電極体41の接触面積が非常に小さいため、大電流を
引出すことが不可能となる。外周部ワイヤボンディング
構造では、ゲート電極22の外周部に導線6がワイヤボ
ンディングされるが、ワイヤボンディングでは導線6に
流れる電流が大きくなればなる程、熱疲労による長期信
鯨性の低下がはなはだしくなる。中間リング構造では、
カソード接触電極体3に絶縁材33を介して埋め込まれ
、ゲート導体4に接続された環状電極体42が環状ゲー
ト電極23に圧接する。このようにカソード電極体3と
ゲート電極体42が一体化されていて、ゲート電極23
およびカソード電極21が等しい圧力で圧接されている
点ではすぐれているが、カソード電極21のパターンを
環状ゲート電極23をはさんで設けるため、主電流の均
一化を図るためにはゲート電8i23に大面積をとるわ
けにはいかず、大きなゲート電流を引出すためには、環
状ゲート電極を多段に設ける必要があり、接触電極体の
構造も極端に?jl雑になる。
As the current of the GTO thyristor increases, the gate extraction current also increases. The gate structures of conventionally known GTO thyristors include a central gate structure shown in FIG.
There is an outer peripheral wire bonding structure shown in the figure and an intermediate ring structure shown in FIG. In the center gate structure, pnpn
A gate conductor is formed by a disc spring 5 accommodated in a recess 32 provided at the center of a contact body 3 having an electrode layer 31 in pressure contact with a cathode electrode 21 provided on an n emitter layer 11 of a silicon substrate l having four layers. The electrode body 41 at the tip of 4 is p
It is pressed against the center of a gate electrode 22 provided on the base layer 12 or made of a vapor deposited layer. However, in this structure, the contact area of the gate electrode body 41 is very small, making it impossible to draw a large current. In the outer periphery wire bonding structure, the conductor 6 is wire-bonded to the outer periphery of the gate electrode 22, but in wire bonding, the larger the current flowing through the conductor 6, the more the long-term stability is deteriorated due to thermal fatigue. . In the intermediate ring structure,
An annular electrode body 42 embedded in the cathode contact electrode body 3 via an insulating material 33 and connected to the gate conductor 4 is pressed against the annular gate electrode 23 . In this way, the cathode electrode body 3 and the gate electrode body 42 are integrated, and the gate electrode 23
This is excellent in that the cathode electrodes 21 and 21 are pressed together with equal pressure, but since the pattern of the cathode electrode 21 is provided with the annular gate electrode 23 in between, in order to equalize the main current, it is necessary to It is not possible to take up a large area, and in order to extract a large gate current, it is necessary to provide annular gate electrodes in multiple stages, and the structure of the contact electrode body must also be extremely large. jl becomes sloppy.

【発明の目的】[Purpose of the invention]

本発明は、ベース層に設けられたゲート電極玄圧接する
電極体によって接続することにより信鯨性を高め、しか
も十分大きな接触面積で電極体と接触して大電流をゲー
トから引出すことのできるGTOサイリスクを提供する
ことを目的とする。
The present invention improves reliability by connecting the gate electrode provided in the base layer with an electrode body that is in pressure contact with the gate electrode, and also makes it possible to draw a large current from the gate by contacting the electrode body with a sufficiently large contact area. The purpose is to provide cyrisk.

【発明の要点】[Key points of the invention]

本発明は、上面側のエミッタ層に隣接するベース層が外
周部において、エミッタ層と同一平面まで延長されてゲ
ート電極がその面上まで延長され、そのゲート電極延長
部に前記エミッタ層上の主電極に圧接する電極体と一体
で、電気的にそれと絶縁されたゲート電極体に圧接する
ことにより上記の目的を達成するものである。また、両
ベース層間のpn接合が露出する半導体基板側面に形成
されるベベル成形をベース層と共にエミッタ層と同一平
面まで延長できるから、耐圧を向上させるのに有効であ
る。
In the present invention, the base layer adjacent to the emitter layer on the upper surface side is extended to the same plane as the emitter layer at the outer periphery, and the gate electrode is extended to the surface thereof, and the gate electrode extension part is attached to the main layer on the emitter layer. The above object is achieved by press-contacting the gate electrode body, which is integrated with the electrode body and is electrically insulated from the electrode body. Furthermore, the bevel formed on the side surface of the semiconductor substrate where the pn junction between both base layers is exposed can be extended to the same plane as the emitter layer together with the base layer, which is effective in improving the breakdown voltage.

【発明の実施例】[Embodiments of the invention]

第1図は本発明の一実施例を示し、第2図ないし第4図
と共通の部分には同一の符号が付されている。第2図な
いし第4図と比較すれば明らかなようにpnpn4層を
有するシリコン基板1の外周部はdv/dt耐量を損な
わないように0層拡散を行わず、pnp構造となってお
り、pベース層12がnエミッタ層11と同一平面まで
延びている。このpベース層12の外周部側面には、下
層側の側面に形成されたベベル形状が延長されている。 外周部は、第2図ないし第4図の従来例でもゲート部と
して形成されている部分なのでカソード有効面積を減少
させることはない。基板12上面から堀り込まれた凹部
13の底面に被着するゲート電極22は、pベース層1
2の外周部の上面に形成されたゲート電極23とM層2
4によって接続されている。カソード電8i21に圧接
する電極層31を有する接触電極体3の外周には、絶縁
物7を介してゲート接触電極体8が一体に形成され、そ
の下面の電極層81がカソード電極21と同一平面にあ
るゲート電極23に圧接する。従ってゲート電8i23
はカソード電極と等しい加圧力を受けて電1Ji81と
接触する。
FIG. 1 shows an embodiment of the present invention, and parts common to FIGS. 2 to 4 are given the same reference numerals. As is clear from a comparison with FIGS. 2 to 4, the outer periphery of the silicon substrate 1 having four pnpn layers has a pnp structure without 0-layer diffusion so as not to impair the dv/dt withstand capability. Base layer 12 extends to the same plane as n emitter layer 11 . The bevel shape formed on the side surface of the lower layer is extended on the side surface of the outer peripheral portion of the p base layer 12 . Since the outer peripheral portion is also formed as a gate portion in the conventional examples shown in FIGS. 2 to 4, the effective area of the cathode is not reduced. The gate electrode 22, which is attached to the bottom surface of the recess 13 dug from the top surface of the substrate 12, is formed of the p base layer 1.
The gate electrode 23 and the M layer 2 formed on the upper surface of the outer periphery of the M layer 2
Connected by 4. A gate contact electrode body 8 is integrally formed on the outer periphery of the contact electrode body 3 having an electrode layer 31 in pressure contact with the cathode electrode 8i21 via an insulator 7, and the electrode layer 81 on the lower surface thereof is on the same plane as the cathode electrode 21. It is pressed into contact with the gate electrode 23 located at. Therefore gate electric 8i23
contacts the electrode 1Ji81 under a pressure equal to that of the cathode electrode.

【発明の効果】【Effect of the invention】

本発明によれば、ゲート電極を半導体基板の外周部まで
延長させ、そこで電極体を圧接することによって接触面
積を大きくでき、大電流の引出しが可能になった。また
、電極体と圧接するゲート電極が設けられるベース層外
周部を最上層のエミッタ層と同一平面まで延長させるこ
とにより、主電極と圧接する電極体と一体に板状に形成
できるゲート電極体を用いることができ、ti体構造が
単純となり、主電極、ゲート電極が等しい加圧力で接触
するので信鯨性が向上した。この結果、従来の同じ大き
さのGTOサイリスタにくらべ、ゲートインピーダンス
が大幅に減少し、可制御電流が40%程度上昇した。さ
らに、ゲートが設けられろベース層の側面が長くなり、
その部分までベベル面を延長することにより、アノード
・カソード間順耐圧が向上するという効果が得られた。 これらの効果は、実施例と異なってゲート電極をnベー
ス層に設けるGTOサイリスタにおいても同様に得るこ
とができる。
According to the present invention, by extending the gate electrode to the outer periphery of the semiconductor substrate and pressing the electrode body there, the contact area can be increased, and a large current can be drawn out. In addition, by extending the outer periphery of the base layer, where the gate electrode is in pressure contact with the electrode body, to the same plane as the uppermost emitter layer, the gate electrode body can be formed into a plate shape integrally with the electrode body that is in pressure contact with the main electrode. The structure of the Ti body is simple, and the main electrode and the gate electrode are brought into contact with the same pressing force, resulting in improved reliability. As a result, compared to a conventional GTO thyristor of the same size, the gate impedance was significantly reduced and the controllable current increased by about 40%. Additionally, the sides of the base layer are longer when the gate is provided;
By extending the bevel surface to that portion, the effect of improving the forward breakdown voltage between the anode and cathode was obtained. These effects can be similarly obtained in a GTO thyristor in which the gate electrode is provided in the n-base layer, unlike the embodiment.

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

第1図は本発明の一実施例のシリコン基板および接触電
極体の断面図、第2図、第3図、第4図はそれぞれ従来
のGTOサイリスクのシリコン基板および接触電極体の
断面図である。 l:シリコン基板、11:nエミッタ層、12:9ベ一
ス層、21:カソード電極、22.23:ゲート電極、
3:カソード接触電極体、7:絶縁物、8:ゲート接触
電極体。
FIG. 1 is a cross-sectional view of a silicon substrate and a contact electrode body according to an embodiment of the present invention, and FIGS. 2, 3, and 4 are cross-sectional views of a silicon substrate and a contact electrode body of a conventional GTO SIRISK, respectively. . l: silicon substrate, 11: n emitter layer, 12: 9 base layer, 21: cathode electrode, 22.23: gate electrode,
3: cathode contact electrode body, 7: insulator, 8: gate contact electrode body.

Claims (1)

【特許請求の範囲】[Claims] 1)複数の領域に分割されたエミッタ層表面に一方の主
電極が設けられ、隣接するベース層のエミッタ層領域を
取り囲む領域表面にゲート電極が設けられ、前記主電極
に電極体が圧接するものにおいて、前記ベース層が外周
部において前記エミッタ層と同一平面まで延びてゲート
電極がその面上まで延長され、該ゲート電極延長部に主
電極に圧接する電極体と一体で、それと電気的に絶縁さ
れたゲート電極体が圧接することを特徴とするGTOサ
イリスタ。
1) One main electrode is provided on the surface of the emitter layer divided into a plurality of regions, a gate electrode is provided on the surface of the region surrounding the emitter layer region of the adjacent base layer, and the electrode body is in pressure contact with the main electrode. In this case, the base layer extends to the same plane as the emitter layer at the outer periphery, and the gate electrode is extended to the same plane as the emitter layer, and the gate electrode extension part is integral with an electrode body that presses against the main electrode and is electrically insulated therefrom. A GTO thyristor characterized in that the gate electrode body is in pressure contact with the gate electrode body.
JP7781786A 1986-04-04 1986-04-04 Gto thyristor Pending JPS62234370A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP7781786A JPS62234370A (en) 1986-04-04 1986-04-04 Gto thyristor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7781786A JPS62234370A (en) 1986-04-04 1986-04-04 Gto thyristor

Publications (1)

Publication Number Publication Date
JPS62234370A true JPS62234370A (en) 1987-10-14

Family

ID=13644579

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7781786A Pending JPS62234370A (en) 1986-04-04 1986-04-04 Gto thyristor

Country Status (1)

Country Link
JP (1) JPS62234370A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02143563A (en) * 1988-11-25 1990-06-01 Fuji Electric Co Ltd Thyristor
JPH0382080A (en) * 1989-08-24 1991-04-08 Mitsubishi Electric Corp Bipolar type semiconductor switching device
JPH03108764A (en) * 1989-04-11 1991-05-08 Fuji Electric Co Ltd Semiconductor device

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02143563A (en) * 1988-11-25 1990-06-01 Fuji Electric Co Ltd Thyristor
JPH03108764A (en) * 1989-04-11 1991-05-08 Fuji Electric Co Ltd Semiconductor device
JPH0382080A (en) * 1989-08-24 1991-04-08 Mitsubishi Electric Corp Bipolar type semiconductor switching device

Similar Documents

Publication Publication Date Title
US7893457B2 (en) Bipolar mosfet devices and methods for their use
GB1112301A (en) Controlled rectifier with improved turn-on and turn-off characteristics
US3794890A (en) Thyristor with amplified firing current
JP4416288B2 (en) Reverse conduction thyristor
JPS62234370A (en) Gto thyristor
JPS60263461A (en) Manufacture of high withstand voltage longitudinal transistor
KR970013149A (en) Schottky barrier diodes
JPH01253274A (en) Reverse conduction gto thyristor
JP2796470B2 (en) Self-extinguishing thyristor and manufacturing method thereof
JP3334509B2 (en) Semiconductor device
JPS584828B2 (en) Amplification gate type thyristor
JPS5923115B2 (en) Mesa type semiconductor device
JPH10135489A (en) Diode
JPS642441Y2 (en)
JPH07202202A (en) Mos device chip for electric power and package assembly
JPS6339972Y2 (en)
JP4078895B2 (en) Semiconductor device
JP2002134523A (en) Semiconductor element
JP3910699B2 (en) GTO thyristor
JP2782758B2 (en) Semiconductor integrated circuit
JPH0543474Y2 (en)
JPS6112069A (en) Semiconductor device
JPH0243337B2 (en)
JPH0129795Y2 (en)
JP2854655B2 (en) Light firing thyristor