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JP2594942B2 - Method for manufacturing semiconductor device - Google Patents
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JP2594942B2 - Method for manufacturing semiconductor device - Google Patents

Method for manufacturing semiconductor device

Info

Publication number
JP2594942B2
JP2594942B2 JP62114613A JP11461387A JP2594942B2 JP 2594942 B2 JP2594942 B2 JP 2594942B2 JP 62114613 A JP62114613 A JP 62114613A JP 11461387 A JP11461387 A JP 11461387A JP 2594942 B2 JP2594942 B2 JP 2594942B2
Authority
JP
Japan
Prior art keywords
gate electrode
ion implantation
semiconductor device
layer
gate
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
JP62114613A
Other languages
Japanese (ja)
Other versions
JPS63281470A (en
Inventor
信敏 松永
勝 宮崎
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.)
Hitachi Ltd
Original Assignee
Hitachi 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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP62114613A priority Critical patent/JP2594942B2/en
Publication of JPS63281470A publication Critical patent/JPS63281470A/en
Application granted granted Critical
Publication of JP2594942B2 publication Critical patent/JP2594942B2/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
    • 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
    • H10D62/13Semiconductor regions connected to electrodes carrying current to be rectified, amplified or switched, e.g. source or drain regions
    • H10D62/149Source or drain regions of field-effect devices
    • H10D62/161Source or drain regions of field-effect devices of FETs having Schottky gates

Landscapes

  • Junction Field-Effect Transistors (AREA)

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は半導体装置の製造方法に係り、特にトランジ
スタの種々の特性を劣化させず、かつ低い寄生抵抗を持
ち化合物半導体装置の製造方法に関する。
Description: BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method for manufacturing a semiconductor device, and more particularly to a method for manufacturing a compound semiconductor device that does not deteriorate various characteristics of a transistor and has low parasitic resistance.

〔従来の技術〕[Conventional technology]

従来の電界効果トランジスタは、第2図,第3図に記
載のように、ゲート耐圧,短チヤネル効果,寄生抵抗等
のトランジスタの諸特性のうちいずれか1つあるいは2
つに着目して高い性能を得ており、上記のすべてが高性
能ではなかつた。すなわち第2図のトランジスタでは、
低抵抗層9がゲート電極3′から十分離れているため、
高いゲート耐圧が得られ、しかもゲート長を短かくした
時に生ずる短チヤネル効果も小さい。ところがこの構造
では、ゲート電極3′とソース電極4の間のかなり大き
な部分を抵抗率の高い能動層5の一部が占めているた
め、ゲートソース間の寄生抵抗が大きく高い性能が得ら
れない。これはトランジスタのしきい値が正のエンハン
スメント型トランジスタにおいては、さらに顕著であ
る。一方、第3図は高耐熱ゲート3を用いた、セルフア
ライメント型電界効果トランジスタである。この場合、
ゲートソース間のほとんどの部分が低抵抗層で、寄生抵
抗は小さく、高性能のトランジスタが得られるが、ゲー
ト電極3に低抵抗層10が近接しているため、ゲート耐圧
が低いという欠点がある。また低抵抗層間の距離が近い
ため、電界が大きく、ゲート長を短かくした時に短チヤ
ネル効果が大きくなる。したがつて、従来の構造では、
上記3つの条件をすべて満足することは困難である。
As shown in FIGS. 2 and 3, the conventional field-effect transistor has one or two of various transistor characteristics such as gate breakdown voltage, short channel effect, and parasitic resistance.
High performance was obtained by paying attention to the above, and all of the above were not high performance. That is, in the transistor of FIG.
Since the low resistance layer 9 is sufficiently separated from the gate electrode 3 ',
A high gate breakdown voltage can be obtained, and the short channel effect generated when the gate length is shortened is small. However, in this structure, a considerably large portion between the gate electrode 3 'and the source electrode 4 is occupied by a part of the active layer 5 having a high resistivity. . This is even more remarkable in an enhancement type transistor having a positive transistor threshold value. On the other hand, FIG. 3 shows a self-alignment type field effect transistor using the high heat resistant gate 3. in this case,
Most of the portion between the gate and the source is a low-resistance layer, the parasitic resistance is small, and a high-performance transistor can be obtained. . Further, since the distance between the low resistance layers is short, the electric field is large, and the short channel effect becomes large when the gate length is made short. Therefore, in the conventional structure,
It is difficult to satisfy all three conditions.

〔発明が解決しようとする問題点〕[Problems to be solved by the invention]

本発明の目的は、ゲート電極3とソース電極4とを間
の低抵抗層の抵抗率を、ゲート電極からの距離に応じて
適当な値に選ぶことによつて、上記3つの条件をすべて
満足する高性能の電界効果トランジスタを有する半導体
装置の製造方法を得ることにある。
It is an object of the present invention to satisfy all of the above three conditions by selecting the resistivity of the low resistance layer between the gate electrode 3 and the source electrode 4 to an appropriate value according to the distance from the gate electrode. To provide a method for manufacturing a semiconductor device having a high-performance field-effect transistor.

〔問題点を解決するための手段〕[Means for solving the problem]

上記目的は、第1図に示すような素子構造の半導体装
置を、ゲート電極やゲート電極の側壁をイオン打込みマ
スクとして用いて製造することによつて達成される。ト
ランジスタのゲート電極3に近接する第1の低抵抗層6
は、このトランジスタが必要とするゲート耐圧が得ら
れ、かつ短チヤネル効果が十分小さいような抵抗率に選
ぶ。この値は必要とされる耐圧によつて異なるが、通常
は200〜1KΩ/□である。また、第1図に示したように
第2の低抵抗層7は直接ゲート電極6には接していない
ため、ゲート耐圧を劣化させずに第1の低抵抗層6より
も低い抵抗率とすることができる。但し、短チヤンネル
効果は、さらにゲートから離れた位置にまでその影響が
及ぶため、短チヤネル効果は十分小さうような抵抗率を
選び、かつゲート耐圧には影響を及ぼさないようにゲー
ト電極3からは離して設ける。通常この長さは0.05〜0.
5μmであり、抵抗率は100〜700Ω/□である。
The above object is achieved by manufacturing a semiconductor device having an element structure as shown in FIG. 1 by using a gate electrode and side walls of the gate electrode as an ion implantation mask. First low resistance layer 6 close to gate electrode 3 of transistor
Is selected so that the gate breakdown voltage required for this transistor is obtained and the short-channel effect is sufficiently small. This value varies depending on the required breakdown voltage, but is usually 200 to 1 KΩ / □. Further, as shown in FIG. 1, the second low-resistance layer 7 is not in direct contact with the gate electrode 6, so that the resistivity is lower than that of the first low-resistance layer 6 without deteriorating the gate breakdown voltage. be able to. However, since the short-channel effect affects the position further away from the gate, the resistivity is selected so that the short-channel effect is sufficiently small, and the gate electrode 3 is connected to the gate electrode 3 so as not to affect the gate breakdown voltage. Are provided separately. Usually this length is 0.05-0.
5 μm, and the resistivity is 100 to 700Ω / □.

上記2つの低抵抗層6,7のみを用いた構造の電界効果
トランジスタは従来考案されているが、上記2つの低抵
抗層のみでは、耐圧を劣化させない程度に近接させるこ
とができず、かつ短チヤネル効果が十分小さいような低
抵抗層7では、ソース2,ゲート3の間の直列抵抗を十分
に小さくしてトランジスタの性能を十分に高めることが
できない。
A field effect transistor having a structure using only the two low-resistance layers 6 and 7 has been conventionally devised. However, only the two low-resistance layers cannot be close enough to the extent that the withstand voltage is not deteriorated, and a short-circuit is required. In the case of the low-resistance layer 7 in which the channel effect is sufficiently small, the series resistance between the source 2 and the gate 3 cannot be sufficiently reduced to sufficiently enhance the performance of the transistor.

そこで第2の低抵抗層7よりさらにゲート電極から離
してしかも7よりさらに低抵抗の第3の低抵抗層8を導
入する。この低抵抗層は1十分高い性能を得るために十
分低い抵抗率を持ち、しかも短チヤネル効果への影響が
ないようにゲート電極3から十分に離して設ける。通常
この長さは、0.3〜1.0μm,抵抗は10〜300Ω/□であ
る。
Therefore, a third low-resistance layer 8 which is further away from the gate electrode than the second low-resistance layer 7 and has a lower resistance than 7 is introduced. This low resistance layer has a sufficiently low resistivity to obtain a sufficiently high performance, and is provided sufficiently away from the gate electrode 3 so as not to affect the short channel effect. Usually, this length is 0.3 to 1.0 μm and the resistance is 10 to 300Ω / □.

〔作用〕[Action]

本発明に係る第1図の如き構造の電界効果トランジス
タでは、ソース,ゲート電極間の低抵抗層が6,7,8の3
層から成つているため、それぞれの抵抗率およびゲート
電極3からの距離に対する自由度が大きく、ゲート耐
圧,短チヤネル効果,トランジスタの直列抵抗のすべて
に対して最適な値をそれぞれ設定することができ、この
設定した抵抗率とゲート電極からの距離をゲート電極や
ゲート電極の側壁をマスクとするイオン打込み法を用い
て確保することにより、より高性能の電界効果トランジ
スタを得ることができる。
In the field-effect transistor having the structure as shown in FIG. 1 according to the present invention, the low-resistance layer between the source and the gate electrode is formed of 6, 7, 8 3
Since it is composed of layers, the degree of freedom with respect to each resistivity and the distance from the gate electrode 3 is large, and optimal values can be set for all of the gate breakdown voltage, short channel effect, and series resistance of the transistor. By securing the set resistivity and the distance from the gate electrode by using the ion implantation method using the gate electrode and the side wall of the gate electrode as a mask, a higher performance field effect transistor can be obtained.

〔実施例〕〔Example〕

(実施例1) 以下、本発明の一実施例を第1図により説明する。 Embodiment 1 Hereinafter, an embodiment of the present invention will be described with reference to FIG.

まず半絶縁性GaAs基板にSiイオンをエネルギー30KeV
で4×1012cm-2のドーズ量で打ち込む。さらにSiO2を保
護膜として800℃で20分間のアニールを行ない、活性化
することで活性層5を形成する。次に耐熱性のシヨツト
キゲート,WSiをゲート金属3として形成する。このゲー
ト金属3をマスクとしてイオン打込みを行なうことで、
第1のn+層6を形成する。さらにSiO2を厚さ2000Å被着
し、反応性イオンエツチング(RIE)でゲート付近を除
いて絶縁膜を除去することで、ゲートの側面に側壁を残
す。この側壁およびゲート電極をマスクとして再びSiイ
オンを打ち込むことで、ゲート電極3から0.3μm離し
て第2のn+層7を形成する。次いでさらに同様の方法で
再び側側を形成して、この側壁およびゲート金属をマス
クとして同様にイオン打込みを行うことでゲート電極3
から0.6μm離して第3のn+層8を形成する。つづいてS
iO2を保護膜として用いて、800℃で20分間アニールして
イオン打込み量を活性化する。以下、通常の方法により
ソースドレイン電極2,4を形成することで電界効果トラ
ンジスタを完成する。この時、第1〜第3のn+層6〜8
のイオン打込みエネルギ,ドーズ量、あるいは側壁の厚
さを最適な値に設定することによりトランジスタのゲー
ト耐圧,短チヤネル効果,寄生直列抵抗のすべてが最適
な値となる高性能の電界効果トランジスタを得ることが
できる。
First, Si ions are applied to a semi-insulating GaAs substrate at an energy of 30 KeV.
With a dose of 4 × 10 12 cm -2 . Further, annealing is performed at 800 ° C. for 20 minutes using SiO 2 as a protective film, and the active layer 5 is formed by activation. Next, a heat-resistant shot gate, WSi, is formed as the gate metal 3. By performing ion implantation using the gate metal 3 as a mask,
A first n + layer 6 is formed. Further, SiO 2 is deposited to a thickness of 2000 mm, and the insulating film is removed by reactive ion etching (RIE) except for the vicinity of the gate, thereby leaving a sidewall on the side surface of the gate. By implanting Si ions again using the side wall and the gate electrode as a mask, the second n + layer 7 is formed at a distance of 0.3 μm from the gate electrode 3. Next, a side is formed again by the same method, and ion implantation is performed in the same manner using the side wall and the gate metal as a mask to thereby form the gate electrode 3.
A third n + layer 8 is formed at a distance of 0.6 μm from the substrate. Then S
Using iO 2 as a protective film, the ion implantation amount is activated by annealing at 800 ° C. for 20 minutes. Hereinafter, the field effect transistor is completed by forming the source / drain electrodes 2 and 4 by an ordinary method. At this time, the first to third n + layers 6 to 8
By setting the ion implantation energy, dose amount, or side wall thickness of the transistor to optimum values, a high-performance field-effect transistor can be obtained in which all of the gate breakdown voltage, short channel effect, and parasitic series resistance of the transistor become optimum values. be able to.

なお、この時打込みイオンとしてSiの代わりにS,Se
等、絶縁膜としてSi3N4,SiON等、またゲート金属材料と
してWN,WAl等を用いることもできる。
At this time, S, Se was used instead of Si as implanted ions.
For example, Si 3 N 4 , SiON or the like can be used as an insulating film, and WN or WAl can be used as a gate metal material.

(実施例2) 本発明のもう1つの例としてn層5〜8の下にp型層
11を埋め込んだトランジスタの製造方法を第4図にあげ
る。このようにp埋込み層11を組み合わせることによ
り、さらに短チヤネル効果を低減でき、さらに高性能の
電界効果トランジスタを得ることができる。
(Example 2) As another example of the present invention, a p-type layer is formed under n layers 5 to 8.
FIG. 4 shows a method of manufacturing a transistor in which 11 is embedded. By combining the p buried layer 11 in this manner, the short channel effect can be further reduced, and a higher performance field effect transistor can be obtained.

〔発明の効果〕〔The invention's effect〕

本発明によれば、互いに相反する関係にある電界効果
トランジスタのゲート耐圧,短チヤネル効果,寄生抵抗
の3つの要素を、3つのn+層6〜8で独立に最適化でき
るため、すべての要求を満足する高性能の電界効果トラ
ンジスタを実現することができる。
According to the present invention, the three elements, that is, the gate breakdown voltage, the short-channel effect, and the parasitic resistance of the field-effect transistors, which are in a mutually contradictory relationship, can be independently optimized by the three n + layers 6 to 8. Can be realized.

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

第1図は本発明の一実施例により作製した電界効果トラ
ンジスタの断面図、第2図,第3図は従来の電界効果ト
ランジスタの断面図をそれぞれ示す。また第4図は本発
明の他の実施例により作製したp埋込みトランジスタの
断面図を示す。 1……半絶縁性基板、2……ソース電極、3……ゲート
電極、4……ドレイン電極、5……n型活性層、6……
第1のn+層、7……第2のn+層、8……第3のn+層、9,
10……従来構造のn+層、11……p型埋込み層。
FIG. 1 is a sectional view of a field-effect transistor manufactured according to one embodiment of the present invention, and FIGS. 2 and 3 are sectional views of a conventional field-effect transistor. FIG. 4 is a sectional view of a p-buried transistor manufactured according to another embodiment of the present invention. DESCRIPTION OF SYMBOLS 1 ... Semi-insulating substrate, 2 ... Source electrode, 3 ... Gate electrode, 4 ... Drain electrode, 5 ... N-type active layer, 6 ...
The first n + layer, 7 ...... second n + layer, 8 ...... third n + layer, 9,
10: n + layer of conventional structure, 11: p-type buried layer.

───────────────────────────────────────────────────── フロントページの続き (56)参考文献 特開 昭61−229369(JP,A) 特開 昭61−152079(JP,A) 特開 昭62−54966(JP,A) 特開 昭61−95570(JP,A) 特開 昭61−56464(JP,A) 特開 昭62−9676(JP,A) ──────────────────────────────────────────────────続 き Continuation of the front page (56) References JP-A-61-229369 (JP, A) JP-A-61-152079 (JP, A) JP-A-62-54966 (JP, A) JP-A-61-54966 95570 (JP, A) JP-A-61-56464 (JP, A) JP-A-62-9676 (JP, A)

Claims (3)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】ゲート電極および能動層形成工程後に、前
記能動層に接続される前記能動層と同一導電型の低抵抗
層を形成する工程を少なくとも有する半導体装置の製造
方法において、前記低抵抗層の形成工程は、前記ゲート
電極をマスクとする第1回のイオン打込み工程と、前記
ゲート電極に厚さが0.05〜0.5μmの第1の側壁を形成
する工程と、前記ゲート電極と前記第1の側壁をマスク
とする第2回のイオン打込み工程と、前記第1の側壁に
さらに側壁を形成して前記ゲート電極からの厚さが0.3
〜1.0μmの第2の側壁を形成する工程と、前記ゲート
電極と前記第2の側壁をマスクとする第3回のイオン打
込み工程を有し、前記第1回のイオン打込み工程で、前
記能動層に隣接し、抵抗率が200〜1000Ω/□の範囲に
ある第1の部分が形成され、前記第1回と前記第2回の
イオン打込み工程で、前記第1の部分に隣接し、抵抗率
が前記第1の部分より低くかつ100〜700Ω/□の範囲に
ある第2の部分が形成され、前記第1回,前記第2回お
よび前記第3回のイオン打込み工程で、前記第2の部分
と隣接し、抵抗率が前記第2の部分より低くかつ10〜30
0Ω/□の範囲にある第3の部分が形成されることを特
徴とする半導体装置の製造方法。
1. A method for manufacturing a semiconductor device, comprising: after a step of forming a gate electrode and an active layer, at least a step of forming a low-resistance layer of the same conductivity type as the active layer connected to the active layer. Forming a first ion implantation step using the gate electrode as a mask, forming a first side wall having a thickness of 0.05 to 0.5 μm on the gate electrode; A second ion implantation step using the side wall as a mask, and further forming a side wall on the first side wall so that the thickness from the gate electrode is 0.3 mm.
Forming a second side wall of about 1.0 μm and a third ion implantation step using the gate electrode and the second side wall as a mask, wherein the first ion implantation step A first portion adjacent to the layer and having a resistivity in the range of 200 to 1000 Ω / □ is formed, and in the first and second ion implantation steps, A second portion having a lower rate than the first portion and in a range of 100 to 700 Ω / □ is formed, and the second, third, and third ion implantation steps perform the second ion implantation. And the resistivity is lower than that of the second portion and 10-30.
A method for manufacturing a semiconductor device, wherein a third portion having a range of 0Ω / □ is formed.
【請求項2】前記ゲート電極にWSiを用い、前記能動層
にGaAsを用いる特許請求の範囲第1項に記載の半導体装
置の製造方法。
2. The method for manufacturing a semiconductor device according to claim 1, wherein WSi is used for said gate electrode and GaAs is used for said active layer.
【請求項3】前記半導体装置の製造方法は、前記能動層
の前記ゲート電極と反対側面上に前記能動層と反対導電
型の化合物半導体層を形成する工程を有する特許請求の
範囲第1項又は第2項に記載の半導体装置の製造方法。
3. The method for manufacturing a semiconductor device according to claim 1, further comprising a step of forming a compound semiconductor layer having a conductivity type opposite to that of said active layer on a side of said active layer opposite to said gate electrode. 3. The method for manufacturing a semiconductor device according to claim 2.
JP62114613A 1987-05-13 1987-05-13 Method for manufacturing semiconductor device Expired - Lifetime JP2594942B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62114613A JP2594942B2 (en) 1987-05-13 1987-05-13 Method for manufacturing semiconductor device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62114613A JP2594942B2 (en) 1987-05-13 1987-05-13 Method for manufacturing semiconductor device

Publications (2)

Publication Number Publication Date
JPS63281470A JPS63281470A (en) 1988-11-17
JP2594942B2 true JP2594942B2 (en) 1997-03-26

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JP (1) JP2594942B2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP3356817B2 (en) * 1992-07-30 2002-12-16 住友電気工業株式会社 Method for manufacturing field effect transistor
JP3298601B2 (en) * 1994-09-14 2002-07-02 住友電気工業株式会社 Field effect transistor and method of manufacturing the same

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* Cited by examiner, † Cited by third party
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JPS6156464A (en) * 1984-08-28 1986-03-22 Fujitsu Ltd Semiconductor device
JPS6195570A (en) * 1984-10-16 1986-05-14 Nec Corp Junction gate field effect transistor
JPS61152079A (en) * 1984-12-26 1986-07-10 Hitachi Ltd Manufacture of schottky gate type fet
JPS61229369A (en) * 1985-04-04 1986-10-13 Nec Corp Manufacture of semiconductor device
JPH0815158B2 (en) * 1985-09-04 1996-02-14 株式会社日立製作所 Method for manufacturing Schottky gate field effect transistor

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