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JPH0213826B2 - - Google Patents
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JPH0213826B2 - - Google Patents

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Publication number
JPH0213826B2
JPH0213826B2 JP675679A JP675679A JPH0213826B2 JP H0213826 B2 JPH0213826 B2 JP H0213826B2 JP 675679 A JP675679 A JP 675679A JP 675679 A JP675679 A JP 675679A JP H0213826 B2 JPH0213826 B2 JP H0213826B2
Authority
JP
Japan
Prior art keywords
gate
electrode
semiconductor layer
type
fet
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
JP675679A
Other languages
Japanese (ja)
Other versions
JPS5598868A (en
Inventor
Hideki Hayashi
Kenichi Kikuchi
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.)
Sumitomo Electric Industries Ltd
Original Assignee
Sumitomo Electric Industries 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 Sumitomo Electric Industries Ltd filed Critical Sumitomo Electric Industries Ltd
Priority to JP675679A priority Critical patent/JPS5598868A/en
Publication of JPS5598868A publication Critical patent/JPS5598868A/en
Publication of JPH0213826B2 publication Critical patent/JPH0213826B2/ja
Granted legal-status Critical Current

Links

Description

【発明の詳細な説明】 本発明は、半導体としてシリコンを用いた絶縁
ゲート型電界効果半導体装置の改良に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an improvement in an insulated gate field effect semiconductor device using silicon as a semiconductor.

従来、例えば第1図に見られるようなMIS(金
属・絶縁物・半導体構造)・FET(電界効果トラ
ンジスタ)が知られている。
Conventionally, MIS (metal-insulator-semiconductor structure) and FET (field effect transistor) as shown in FIG. 1, for example, have been known.

図に於いて、1は例えばP型シリコン半導体基
板、2はフイールド用絶縁膜、3はゲート絶縁
膜、4はn+型ソース領域、5はn+型ドレイン領
域、6はソース電極、7はドレイン電極、8はゲ
ート電極をそれぞれ示す。
In the figure, 1 is, for example, a P-type silicon semiconductor substrate, 2 is a field insulating film, 3 is a gate insulating film, 4 is an n + type source region, 5 is an n + type drain region, 6 is a source electrode, and 7 is a 8 indicates a drain electrode, and 8 indicates a gate electrode.

このような構造を有するMIS・FETでは、ゲ
ートに印加する電圧レベルに依りソース・ドレイ
ン間に流れるチヤネル電流を制御するものであ
る。
In a MIS/FET having such a structure, the channel current flowing between the source and drain is controlled depending on the voltage level applied to the gate.

また、第2図に見られるようなシヨツトキ・ゲ
ート型FETも知られている。
In addition, a short gate type FET as shown in FIG. 2 is also known.

図に於いて、11は半絶縁性基板、12は例え
ばエピタキシヤル成長のn型半導体層、13は
n+型ソース領域、14はn+型ドレイン領域、1
5はオーミツク・コンタクトのソース電極、16
はオーミツク・コンタクトのドレイン電極、17
はシヨツトキ・コンタクトのゲート電極である。
In the figure, 11 is a semi-insulating substrate, 12 is, for example, an epitaxially grown n-type semiconductor layer, and 13 is a semi-insulating substrate.
n + type source region, 14 is n + type drain region, 1
5 is the source electrode of the ohmic contact, 16
is the drain electrode of the ohmic contact, 17
is the gate electrode of the shot contact.

このFETもゲート電極17に印加する電圧の
レベルに依りチヤネル電流を制御するものであ
る。
This FET also controls the channel current depending on the level of the voltage applied to the gate electrode 17.

さて、一般的にFETを高速動作させるにはゲ
ート長を出来る限り短かくしなければならない。
しかしながら、第1図について説明したMIS・
FETでは、ドレイン接合に空乏層が発生するか
ら、ゲート長が余り短かいと該空乏層がソース領
域に達し、所謂パンチ・スルーの状態になり易
い。従つて、ゲート長を極端に短かくすることは
出来ない。
Now, generally speaking, in order to operate a FET at high speed, the gate length must be kept as short as possible.
However, the MIS and
In a FET, a depletion layer is generated at the drain junction, so if the gate length is too short, the depletion layer reaches the source region, which tends to cause a so-called punch-through condition. Therefore, the gate length cannot be made extremely short.

これに対し、第2図について説明したシヨツト
キ・ゲート型FETではp・n接合を用いていな
いから、空乏層は発生せず、パンチ・スルーの惧
れはなく、製作技術上許容される範囲でゲート長
を短かくすることができる。また、キヤリヤはパ
ルク中を流れるものであるから、キヤリヤが半導
体層表面のチヤネル中を流れる第1図のMIS・
FETと比較するとキヤリヤ移動度は大である。
しかしながら、シヨツトキ・ゲート型FETも良
いことづくめではなく、例えば、デイプレツシヨ
ン型のものでは入出力が逆極性になつているの
で、次段との結合が困難であり、また、エンハン
スメント型ではゲート入力が順方向であるから、
余り大きな電圧を印加することはできず、従つて
大きな論理振幅が得られない。
On the other hand, since the shot gate type FET explained with reference to FIG. The gate length can be shortened. Also, since the carrier flows in the pulp, the MIS in Fig. 1 where the carrier flows in the channel on the surface of the semiconductor layer.
Carrier mobility is large compared to FET.
However, shot gate type FETs are not full of good features; for example, depletion type FETs have input and output with opposite polarity, making it difficult to connect to the next stage, and enhancement type FETs have gate input is in the forward direction, so
It is not possible to apply a very large voltage, and therefore a large logic amplitude cannot be obtained.

本発明は、順方向にあまり大きな電圧を印加す
ることができないシヨツトキ・ゲート型FETの
欠点を克服するためになされたもので、シヨツト
キ・ゲート型FETにおいてゲート電極と半導体
層との間に絶縁膜をもうけて絶縁ゲート型FET
とし、ゲート長を短くしてもパンチ・スルーの惧
れがないこと、一般のMIS・FETに比べてキヤ
リヤ移動度が大であることなどのシヨツトキ・ゲ
ート型FETの長所はそのまま保持し、しかも、
順方向にも電圧を印加できるので大きな論理振幅
が得られるようにしたものであり、以下、これを
詳細に説明する。
The present invention was made in order to overcome the drawback of the shot-gate type FET, in which a very large voltage cannot be applied in the forward direction. Insulated gate type FET
This design maintains the advantages of shot gate type FETs, such as no fear of punch-through even when the gate length is shortened, and higher carrier mobility than general MIS FETs. ,
Since voltage can also be applied in the forward direction, a large logic amplitude can be obtained, and this will be explained in detail below.

第3図は本発明一実施例の要部側断面図であ
る。
FIG. 3 is a side sectional view of a main part of an embodiment of the present invention.

図に於いて、21は半絶縁性シリコン単結晶基
板、22は気相エピタキシヤル成長法にて形成さ
れた例えば不純物濃度が1×1017〔原子/cm3〕で
厚さが約0.2〔μm〕のn型シリコン半導体層、2
3,24は例えば通常の気相拡散法で選択的に形
成された例えば表面不純物濃度が1×1019〔原
子/cm3〕であるn+型ソース領域及びn+型ドレイ
ン領域、25は例えば熱酸化法にて形成された厚
さ例えば0.15〔μm〕のゲート絶縁膜、26は、オ
ーミツク・コンタクトのソース電極、27はオー
ミツク・コンタクトのドレイン電極、28はそれ
等電極と同時に形成したゲート電極である。尚、
ゲート電極28を形成後、温度500〔℃〕で時間20
〔分〕間程度の熱処理を行なうと良い。
In the figure, 21 is a semi-insulating silicon single crystal substrate, and 22 is a semi-insulating silicon single crystal substrate formed by vapor phase epitaxial growth, for example, with an impurity concentration of 1×10 17 [atoms/cm 3 ] and a thickness of about 0.2 [μm]. ] n-type silicon semiconductor layer, 2
3 and 24 are n + type source regions and n + type drain regions having a surface impurity concentration of, for example, 1×10 19 [atoms/cm 3 ], which are selectively formed by, for example, a normal vapor phase diffusion method; 25 is, for example, A gate insulating film with a thickness of, for example, 0.15 [μm] formed by thermal oxidation, 26 a source electrode of an ohmic contact, 27 a drain electrode of an ohmic contact, and 28 a gate electrode formed at the same time as these electrodes. It is. still,
After forming the gate electrode 28, the temperature was 500 [℃] for 20 hours.
It is recommended that the heat treatment be performed for about [minutes].

このようにして得られた本発明MIS・FETは
シヨツトキ・ゲート型FETと略同じ原理で動作
し、ゲート電極28に印加される電圧に依つて空
乏層の長さが変化して半導体層22中を流れるチ
ヤネル電流が制御されるものである。
The MIS-FET of the present invention obtained in this way operates on substantially the same principle as the shot-gate type FET, and the length of the depletion layer changes depending on the voltage applied to the gate electrode 28. The channel current flowing through is controlled.

本発明に依るMIS・FETは次に列挙する効果
を得ることができる。
The MIS/FET according to the present invention can obtain the following effects.

(1) ソース領域及びドレイン領域はエピタキシヤ
ル成長の半導体層と同導電型であるから電圧が
印加されても空乏層は発生せず、パンチ・スル
ーが起き難い。従つて、ゲート長を製造可能な
限り短かくすることができ、高速化、高集積化
に有効である。
(1) Since the source region and the drain region have the same conductivity type as the epitaxially grown semiconductor layer, no depletion layer is generated even when a voltage is applied, and punch-through is less likely to occur. Therefore, the gate length can be made as short as possible, which is effective for higher speed and higher integration.

(2) キヤリヤはバルク中を移動するので従来の
MIS・FETに比較してキヤリヤ移動度が大で
ある。
(2) Since the carrier moves in bulk, conventional
Carrier mobility is large compared to MIS/FET.

(3) ゲート絶縁膜を有しているので、従来のシヨ
ツトキ・ゲート型FETとは異なりエンハンス
メント・モードで使用したときでも順方向にゲ
ート電圧を加えることができ、大きな論理振幅
を取出すことができる。
(3) Since it has a gate insulating film, unlike conventional shot gate type FETs, gate voltage can be applied in the forward direction even when used in enhancement mode, and large logic amplitude can be obtained. .

(4) ウエハ(基板+半導体層)としてシリコンを
用いているので、良質の酸化絶縁膜を形成して
利用することができる。
(4) Since silicon is used as the wafer (substrate + semiconductor layer), a high-quality oxide insulating film can be formed and used.

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

第1図及び第2図は従来例の要部側断面図、第
3図は本発明一実施例の要部側断面図である。 図に於いて、21は基板、22は半導体層、2
3,24はソース領域とドレイン領域、25はゲ
ート絶縁膜、26,27はソース電極とドレイン
電極、28はゲート電極である。
1 and 2 are side sectional views of main parts of a conventional example, and FIG. 3 is a side sectional view of main parts of an embodiment of the present invention. In the figure, 21 is a substrate, 22 is a semiconductor layer, 2
3 and 24 are a source region and a drain region, 25 is a gate insulating film, 26 and 27 are a source electrode and a drain electrode, and 28 is a gate electrode.

Claims (1)

【特許請求の範囲】[Claims] 1 半絶縁性単結晶基板にエピタキシヤル成長さ
れた一導電型シリコン半導体層を有する半導体ウ
エハ、前記シリコン半導体層と同導電型且つそれ
より高濃度であるソース領域及びドレイン領域、
該領域間に形成されたゲート絶縁膜及びその上の
ゲート電極、前記ソース領域にコンタクトするソ
ース電極及び前記ドレイン領域とコンタクトする
ドレイン電極を備えてなることを特徴とする絶縁
ゲート型電界効果半導体装置。
1. A semiconductor wafer having a silicon semiconductor layer of one conductivity type epitaxially grown on a semi-insulating single crystal substrate, a source region and a drain region having the same conductivity type as the silicon semiconductor layer and having a higher concentration than the silicon semiconductor layer;
An insulated gate field effect semiconductor device comprising a gate insulating film formed between the regions, a gate electrode thereon, a source electrode in contact with the source region, and a drain electrode in contact with the drain region. .
JP675679A 1979-01-23 1979-01-23 Insulated gate type field effect semiconductor device Granted JPS5598868A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP675679A JPS5598868A (en) 1979-01-23 1979-01-23 Insulated gate type field effect semiconductor device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP675679A JPS5598868A (en) 1979-01-23 1979-01-23 Insulated gate type field effect semiconductor device

Publications (2)

Publication Number Publication Date
JPS5598868A JPS5598868A (en) 1980-07-28
JPH0213826B2 true JPH0213826B2 (en) 1990-04-05

Family

ID=11647023

Family Applications (1)

Application Number Title Priority Date Filing Date
JP675679A Granted JPS5598868A (en) 1979-01-23 1979-01-23 Insulated gate type field effect semiconductor device

Country Status (1)

Country Link
JP (1) JPS5598868A (en)

Families Citing this family (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5812365A (en) * 1981-07-15 1983-01-24 Japan Electronic Ind Dev Assoc<Jeida> Thin film transistor and manufacture thereof
US5698864A (en) * 1982-04-13 1997-12-16 Seiko Epson Corporation Method of manufacturing a liquid crystal device having field effect transistors
US5736751A (en) * 1982-04-13 1998-04-07 Seiko Epson Corporation Field effect transistor having thick source and drain regions
US6294796B1 (en) * 1982-04-13 2001-09-25 Seiko Epson Corporation Thin film transistors and active matrices including same
FR2527385B1 (en) * 1982-04-13 1987-05-22 Suwa Seikosha Kk THIN FILM TRANSISTOR AND LIQUID CRYSTAL DISPLAY PANEL USING THIS TYPE OF TRANSISTOR
CA2061796C (en) * 1991-03-28 2002-12-24 Kalluri R. Sarma High mobility integrated drivers for active matrix displays

Also Published As

Publication number Publication date
JPS5598868A (en) 1980-07-28

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