JPS5998559A - Field effect transistor - Google Patents
Field effect transistorInfo
- Publication number
- JPS5998559A JPS5998559A JP57207918A JP20791882A JPS5998559A JP S5998559 A JPS5998559 A JP S5998559A JP 57207918 A JP57207918 A JP 57207918A JP 20791882 A JP20791882 A JP 20791882A JP S5998559 A JPS5998559 A JP S5998559A
- Authority
- JP
- Japan
- Prior art keywords
- layer
- gaas
- effect transistor
- field effect
- source
- 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
Links
Classifications
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D30/00—Field-effect transistors [FET]
- H10D30/80—FETs having rectifying junction gate electrodes
- H10D30/87—FETs having Schottky gate electrodes, e.g. metal-semiconductor FETs [MESFET]
Landscapes
- Electrodes Of Semiconductors (AREA)
- Junction Field-Effect Transistors (AREA)
Abstract
Description
【発明の詳細な説明】
産業上の利用分野
本発明は電界効果トランジスタに関するものであり、特
に相互コンダクタンス?mが高く、高速動作が可能なガ
リウムヒ素からなるショットキバリアゲート型電界効果
トランジスタに関する。DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to field effect transistors, and in particular to transconductance. The present invention relates to a Schottky barrier gate field effect transistor made of gallium arsenide that has a high m and is capable of high-speed operation.
従来例の構成とその問題点
ガリウムヒ素からなる電界効果トランジスタ(以下Ga
As F ICTと記す)は、従来のシリコンを素材と
するFETに比べ、優れた高周波特性を有するFETと
して注目されている。中でもGaAsノ2・、−〕゛
−マリオフ型ショットキバリアゲート型FET(以下ノ
ーマリオフ型GaAs M ICS F E Tと記す
)は高速性と低消費電力性の両者に優れており、ロジッ
クIC,メモリなど種々の応用分野で研究が進められて
いる。Structure of conventional example and its problems Field effect transistor made of gallium arsenide (hereinafter referred to as Ga
AsF ICT) is attracting attention as an FET that has superior high frequency characteristics compared to conventional FETs made of silicon. Among them, GaAs2., -]-Mariov Schottky barrier gate FET (hereinafter referred to as normally-off GaAs MICS FET) is excellent in both high speed and low power consumption, and is widely used in logic ICs, memories, etc. Research is underway in various applied fields.
従来のGaps MESFICTの構造を第1図に示
す。同図において1は半絶縁性GaAs基板、2はバッ
ファ層、3は能動層、4はドレイン電極、6はゲート電
極、6は5102アイソレ一シヨン層、7はソース電極
である。ゲート5とソース7間のシリーズ抵抗Rsの存
在はFITのチャネルコンダクタンスh” ++Rs、
、m )ノm と低下さ也またゲート容量C68と共
に積分回路を構成し伝達速度も低下させる。The structure of a conventional Gaps MESFICT is shown in FIG. In the figure, 1 is a semi-insulating GaAs substrate, 2 is a buffer layer, 3 is an active layer, 4 is a drain electrode, 6 is a gate electrode, 6 is a 5102 isolation layer, and 7 is a source electrode. The presence of the series resistance Rs between the gate 5 and the source 7 increases the FIT channel conductance h'' ++Rs,
.
従来のGaAs MKSFKTでは第1図に示すように
ゲートの直下だけGaAs層をうすくしたリセス構造で
シリーズ抵抗Rsの低減を試みているが、この構成では
能動層のGaAsfエツチングせねばならず、チャネル
厚さtGの制御が難しい。このチャネル厚さtGの膜厚
でノーマリオン、ノーマリ37、ジ
オフの特性が分かれ、例えば能動層のn型GaAsの不
純物濃度が1×1017cIIL−3であったとすると
チャネル厚さtGが8oO人ではノーマリオフ、900
にではノーマリオンになり、このリセス構造ではプロセ
ス上再現性よくノーマリオフ特性を得ることはできなか
った0
発明の目的
本発明は再現性よくノーマリオフ特性を実現しゲート・
ソース間シリーズ抵抗Rsがほとんど零となり、したが
って相互コンダクタンスhが高く、高速動作の可能なG
aAs MESFET f提供すること全目的とするも
のである。In the conventional GaAs MKSFKT, as shown in Figure 1, an attempt is made to reduce the series resistance Rs by using a recessed structure in which the GaAs layer is thinned just below the gate, but with this structure, the active layer GaAsf must be etched, and the channel thickness is reduced. It is difficult to control satG. The characteristics of normally on, normally 37, and geo-off are determined by the channel thickness tG. For example, if the impurity concentration of n-type GaAs in the active layer is 1 x 1017cIIL-3, the channel thickness tG is 8oO, and the normally-off characteristics are different. , 900
However, with this recess structure, it was not possible to obtain normally-off characteristics with good reproducibility due to the process.Objective of the Invention The present invention realizes normally-off characteristics with good reproducibility and
The source-to-source series resistance Rs is almost zero, so the mutual conductance h is high and G enables high-speed operation.
The entire purpose is to provide aAs MESFET f.
発明の構成
本発明の電界効果トランジスタは、能動層がガリウムヒ
素からなるショットキパリアゲート型の電界効果トラン
ジスタであって、ソース電極およびドレイン電極がガリ
ウムアルミニウムヒ素(Ga、、 klxAs ; O
<χ≦1)からなることを特徴゛とするものである。Structure of the Invention The field effect transistor of the present invention is a Schottky pariah gate type field effect transistor in which the active layer is made of gallium arsenide, and the source electrode and the drain electrode are made of gallium aluminum arsenide (Ga, klxAs; O).
<χ≦1).
実施例の説明
以下本発明の電界効果トランジスタを実施例に基すいて
説明する。DESCRIPTION OF EMBODIMENTS The field effect transistor of the present invention will be described below based on embodiments.
本実施例のGaAs MES FETの断面図を第2図
に、そのパターンの平面図を第3図に示す。FIG. 2 shows a cross-sectional view of the GaAs MES FET of this example, and FIG. 3 shows a plan view of its pattern.
半絶縁性GaAs基板1o上にバッフ1層として1−G
aAs層11を1゜0μmの厚さに設けその上に能動層
n−GaAs 12’z800人、電極層n+−4ao
、、A、do、3As 13,18i200OAコンタ
クト層ri+−GaAs層14を200^それぞれ成長
する。成長は膜厚制御の容易なMBE法、uocvn法
などを用いるが本実施例ではMBE法により成長を行っ
た。基板温度は7o○℃、Gaセル温度1100℃、ム
lセfiv温度1150℃、Asセル温度は250℃と
し、n型不純物としてはSnを使いセル温度は780℃
とした。1−GaAs層11、n−GaAs層12、n
−Gao、y Alo、3AS層13゜18、n+G
aAs層14の各層の成長時間はそれぞれ35分、2分
50秒、5分30秒、7分10秒であった。1-G as a buffer layer on a semi-insulating GaAs substrate 1o
An aAs layer 11 with a thickness of 1°0 μm is provided thereon with an active layer of n-GaAs 12'z800 layers and an electrode layer n+-4ao.
,,A,do,3As 13,18i200OA contact layer ri+-GaAs layer 14 is grown 200^, respectively. For growth, the MBE method, uocvn method, etc., which can easily control the film thickness, are used, and in this example, the MBE method was used. The substrate temperature is 7o○°C, the Ga cell temperature is 1100°C, the molecular temperature is 1150°C, the As cell temperature is 250°C, Sn is used as the n-type impurity, and the cell temperature is 780°C.
And so. 1-GaAs layer 11, n-GaAs layer 12, n
-Gao, y Alo, 3AS layer 13°18, n+G
The growth times for each layer of the aAs layer 14 were 35 minutes, 2 minutes 50 seconds, 5 minutes 30 seconds, and 7 minutes 10 seconds, respectively.
得られたウニ・・−にドレイン、ソースへの電流61・
−ジ
注入用コンタクトとしてムuGe/ムU膜15を蒸着し
、コンタクト層n+−GaSS層14とオーミック接触
をとるため合金化熱処理を行なう。ゲート部分はSiO
□膜16膜形6した開孔部を通して電極mGa、、ム8
13,18のエツチングを行なう。The obtained sea urchin...- has a current of 61 to the drain and source.
- A MuGe/MuU film 15 is deposited as a contact for di-implantation, and alloying heat treatment is performed to establish ohmic contact with the contact layer n+-GaSS layer 14. The gate part is SiO
□Membrane 16 Electrode mGa, , Mu8 is passed through the membrane-shaped aperture.
Perform etching steps 13 and 18.
エツチング液としてはI2/KI水溶液を用いた。An I2/KI aqueous solution was used as the etching solution.
このエツチング液によりGaASとGao、5ムl O
07ムSとの選択エツチングが可能であるのでエツチン
グは能動層GaAs12と電極層G a o7ム10.
3ムS13゜18の界面で停止する。したがってゲート
電極17の直下のチャネル厚さtG′はちょうどn−G
aAs12の膜厚に等しい。結晶成長は膜厚の面内均一
性および制御性に優れているMBK成長でなされている
ため、tG′=800Xが常にウエノ1−のどの場所に
でも成りたち、そのため、非常に再現性よくノーマリオ
フ特性が得られる。ショットキーゲート電極17はムl
蒸着およびリフトオフ技術によって形成する。With this etching solution, GaAS and Gao, 5 ml O
Since selective etching is possible for the active layer GaAs 12 and the electrode layer GaAs 10.
It stops at the interface of 3mm S13°18. Therefore, the channel thickness tG' directly under the gate electrode 17 is just n-G
It is equal to the film thickness of aAs12. Since crystal growth is performed by MBK growth, which has excellent in-plane film thickness uniformity and controllability, tG' = 800X is always formed anywhere on Ueno 1-, and therefore normally-off with excellent reproducibility. characteristics are obtained. The Schottky gate electrode 17 is
Formed by vapor deposition and lift-off techniques.
以上のようにして第2図のMKSFET が得られる。In the above manner, the MKSFET shown in FIG. 2 is obtained.
本実施例での各層の不純物濃Vはノ(ラフ16、、−ジ 1×10 備 コンタクト層14が1×10はである。In this example, the impurity concentration V of each layer is 1×10 The contact layer 14 is 1×10.
G a o、y人l、3As電極層13は1X 1Q”
a−’の高濃度であり、比抵抗は3 x 10−4Ωは
と低く、したがって、ゲート・ソース間の抵抗はGao
、、ムlo、5As層13.18のサイドエツチングに
よって生じたlなる距離の能動層n−GaAs層12の
抵抗分だけとなり、数Ωの低抵抗で従来の第1図に示さ
れる構造の電界効果トランジスタの2000に比べると
2桁の改善がなされた。Ga o, y person l, 3As electrode layer 13 is 1X 1Q"
The resistivity is as low as 3 x 10-4Ω, so the resistance between the gate and source is Gao.
,, only the resistance of the active layer n-GaAs layer 12 at a distance of l caused by the side etching of the 5As layer 13 and 18 is reduced, and the electric field of the conventional structure shown in FIG. This is a two-digit improvement compared to the 2000 effect transistor.
このMESFETの静特性としてしきい電圧vTo、1
V、(ドレイン電流20μ人)で、コンダクタンスhが
150m5/鵡、オン抵抗が1500また伝搬遅延時間
は20pSと従来より10倍高速な素子が得られた。As a static characteristic of this MESFET, the threshold voltage vTo, 1
V, (drain current 20 μm), conductance h was 150 m5/parallel, on-resistance was 1500, and propagation delay time was 20 pS, resulting in an element 10 times faster than conventional devices.
vL
なお以上の脱明で述べたソース電極およびドレイン電極
としてのG a、、ム4ムS層はム1組成比i 0.3
と限定するものではなく、0〈χ≦1のすべての範囲の
適用が可能である。またFITのチャンネル型もnチャ
ネルに限定されるものではない。vL Furthermore, the Ga as the source electrode and the drain electrode mentioned in the above clarification, the Mu4MuS layer has a Mu1 composition ratio i 0.3
However, the whole range of 0<χ≦1 is applicable. Furthermore, the channel type of the FIT is not limited to n-channel.
7・、ジ
ゲート電極もムlに限らず0r−Pt、W−シリサイド
など、どのようなものでも可能である。7. The digate electrode is not limited to mulch, and any material such as Or-Pt or W-silicide can be used.
発明の効果
以上述べたように、本発明のように” + −xAlx
人Skソース、ドレイン電極とすることにより高い相互
コンダクタンスym’に有し高速動作のノーマリオフ型
電界効果トランジスタを再現性よく得ることが可能とな
った。Effects of the invention As mentioned above, as in the present invention, "+ -xAlx
By using Sk as the source and drain electrodes, it has become possible to obtain a normally-off field effect transistor with high mutual conductance ym' and high speed operation with good reproducibility.
第1図は従来の電界効果トランジスタの断面図、第2図
は本発明の一実施例の電界効果トランジスタの断面図、
第3図はそのパターン図である010・・・・・・半絶
縁性GaAs基板、11・・・・・・バッファ層1−G
aAs、12−−=能動層n−GaムS、13・・・・
・・ドレイン電極層”−GaO,7A&、3人S114
・・・・・・コンタクト層n+−GaAs、15・・・
・・・ムu(Be/Auメタル、16・・・・・・5i
02.17・・・・・・ゲート電極、18・・・・・・
ソース電極層n”Ga、、klo、、As。
代理人の氏名 弁理士 中 尾 敏 男 ほか1名第1
図FIG. 1 is a sectional view of a conventional field effect transistor, FIG. 2 is a sectional view of a field effect transistor according to an embodiment of the present invention,
FIG. 3 is a pattern diagram thereof. 010...Semi-insulating GaAs substrate, 11...Buffer layer 1-G
aAs, 12--=active layer n-Gamus S, 13...
...Drain electrode layer"-GaO, 7A &, 3 people S114
...Contact layer n+-GaAs, 15...
...mu (Be/Au metal, 16...5i
02.17...Gate electrode, 18...
Source electrode layer n”Ga,, klo,, As. Name of agent: Patent attorney Toshio Nakao and one other person 1st
figure
Claims (1)
極およびドレイン電極がガリウムアルミニウムヒ素(G
a、、klxAs ; O<x≦1)からなることを特
徴とする電界効果トランジスタ。[Scope of Claims] A Schottky Variant type field effect transistor in which one power layer is made of gallium arsenide, the source electrode and the drain electrode are made of gallium aluminum arsenide (G
A field effect transistor characterized in that it consists of a,, klxAs; O<x≦1).
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57207918A JPS5998559A (en) | 1982-11-27 | 1982-11-27 | Field effect transistor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57207918A JPS5998559A (en) | 1982-11-27 | 1982-11-27 | Field effect transistor |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS5998559A true JPS5998559A (en) | 1984-06-06 |
Family
ID=16547711
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP57207918A Pending JPS5998559A (en) | 1982-11-27 | 1982-11-27 | Field effect transistor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5998559A (en) |
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS63119271A (en) * | 1986-11-06 | 1988-05-23 | Nec Corp | Semiconductor integrated circuit |
| US5021361A (en) * | 1986-02-18 | 1991-06-04 | Kabushiki Kaisha Toshiba | Method for making a field effect transistor integrated with an opto-electronic device |
| US5453627A (en) * | 1992-05-14 | 1995-09-26 | Nippon Telegraph And Telephone Corporation | Quantum interference device and complementary logic circuit utilizing thereof |
Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5661169A (en) * | 1979-10-25 | 1981-05-26 | Oki Electric Ind Co Ltd | Preparation of compound semiconductor device |
| JPS57112079A (en) * | 1980-12-29 | 1982-07-12 | Fujitsu Ltd | Field-effect semiconductor device |
-
1982
- 1982-11-27 JP JP57207918A patent/JPS5998559A/en active Pending
Patent Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5661169A (en) * | 1979-10-25 | 1981-05-26 | Oki Electric Ind Co Ltd | Preparation of compound semiconductor device |
| JPS57112079A (en) * | 1980-12-29 | 1982-07-12 | Fujitsu Ltd | Field-effect semiconductor device |
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5021361A (en) * | 1986-02-18 | 1991-06-04 | Kabushiki Kaisha Toshiba | Method for making a field effect transistor integrated with an opto-electronic device |
| JPS63119271A (en) * | 1986-11-06 | 1988-05-23 | Nec Corp | Semiconductor integrated circuit |
| US5453627A (en) * | 1992-05-14 | 1995-09-26 | Nippon Telegraph And Telephone Corporation | Quantum interference device and complementary logic circuit utilizing thereof |
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