JPH0812867B2 - Semiconductor device - Google Patents
Semiconductor deviceInfo
- Publication number
- JPH0812867B2 JPH0812867B2 JP59103859A JP10385984A JPH0812867B2 JP H0812867 B2 JPH0812867 B2 JP H0812867B2 JP 59103859 A JP59103859 A JP 59103859A JP 10385984 A JP10385984 A JP 10385984A JP H0812867 B2 JPH0812867 B2 JP H0812867B2
- Authority
- JP
- Japan
- Prior art keywords
- layer
- semiconductor
- alloy
- semiconductor layer
- resistance
- 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
Links
Classifications
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D64/00—Electrodes of devices having potential barriers
- H10D64/60—Electrodes characterised by their materials
- H10D64/62—Electrodes ohmically coupled to a semiconductor
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D62/00—Semiconductor bodies, or regions thereof, of devices having potential barriers
- H10D62/80—Semiconductor bodies, or regions thereof, of devices having potential barriers characterised by the materials
- H10D62/85—Semiconductor bodies, or regions thereof, of devices having potential barriers characterised by the materials being Group III-V materials, e.g. GaAs
Landscapes
- Junction Field-Effect Transistors (AREA)
- Electrodes Of Semiconductors (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、とくに高抵抗基板上の半導体層
を動作層とする半導体装置に関する。The present invention relates to a semiconductor device, and more particularly to a semiconductor device having a semiconductor layer on a high resistance substrate as an operating layer.
高抵抗性基板上に形成された半導体層を動作層とする
半導体装置は素子間分離が容易である点、および素子相
互を接続する配線が高抵抗基板上に形成されるため寄生
容量が小さいという利点があり超高速ディジタル集積回
路として適している。その最も好適な例がガリウム砒素
電界効果トランジスタ(以下GaAs FETと称す)であろ
う。GaAs FETの最も基本的な断面形状を第1図に示す。
図において、11は比抵抗107Ωcmの半絶縁性GaAs基板、1
2はイオン注入法(注入エネルギー70KeV.注入イオン:Si
+,ドース量2×1012cm-2)により形成した厚さa:約1000
Å,キャリア密度n:2×1017cm-3のn型GaAs層,13は例え
ばAlよりなるゲート電極、14,15はAuGeを蒸着したあ
と、400℃、1分間の加熱合金化により形成されたオー
ム性接触をなす電極(14:ソース、15:ドレイン)であ
る。全ての半導体装置がそうであるように、GaAs FETに
おいても直列寄生抵抗、(この場合にはソース抵抗RS)
の低減が素子特性の改善の上で不可欠である。このこと
は、FETの相互コンダクタンスgmが、RS=0のときの値g
m0の1/(1+gm0RS)になること、すなわち次式が成立
することからも明らかである。A semiconductor device using a semiconductor layer formed on a high-resistance substrate as an operating layer is easy to separate elements from each other, and a wiring connecting the elements to each other is formed on the high-resistance substrate so that parasitic capacitance is small. It has advantages and is suitable as an ultra-high speed digital integrated circuit. The most preferable example would be a gallium arsenide field effect transistor (hereinafter referred to as GaAs FET). Figure 1 shows the most basic cross-sectional shape of a GaAs FET.
In the figure, 11 is a semi-insulating GaAs substrate with a specific resistance of 10 7 Ωcm, 1
2 is an ion implantation method (implantation energy 70 KeV. Implantation ion: Si
+ , The thickness formed by the dose amount 2 × 10 12 cm -2 ): About 1000
Å, n-type GaAs layer with carrier density n: 2 × 10 17 cm -3 , 13 is a gate electrode made of, for example, Al, 14 and 15 are formed by vapor deposition of AuGe and then heat alloying at 400 ° C for 1 minute. Electrodes (14: source, 15: drain) that make ohmic contact. As with all semiconductor devices, GaAs FETs also have series parasitic resistance (source resistance R S in this case).
Is required to improve device characteristics. This is because the transconductance gm of the FET is the value g when R S = 0.
It is also clear from the fact that it becomes 1 / (1 + gm 0 R S ) of m 0 , that is, the following equation holds.
このようにRSの低減化はgmの改善、すなわちFET特性
の改善の上で不可欠であるにも拘らず、従来はそれに対
する対策として、ソース・ゲート間の距離の短縮と接触
比抵抗ρCの低減しか活用されておらず、オーム性接触
の合金化層(アロイ層)の深さの最適化については何ら
注意を払われていなかった。 Thus, although the reduction of R S is indispensable for the improvement of gm, that is, the improvement of FET characteristics, conventionally, as a countermeasure against it, the distance between the source and the gate is shortened and the contact specific resistance ρ C is reduced. However, no attention was paid to the optimization of the depth of the alloyed layer (alloy layer) for ohmic contact.
本発明は従来の半導体装置における上記の如き欠点に
鑑みてなされたものでありその目的はオーミック接触部
寄生抵抗の小さい半導体装置を提供することにある。The present invention has been made in view of the above-mentioned drawbacks of the conventional semiconductor device, and an object thereof is to provide a semiconductor device having a small parasitic resistance of ohmic contact portion.
本発明は、高抵抗性基板上の半導体動作層に少なくと
もオーム性接触をなす電極、とくに電極金属と半導体と
の加熱合金化により形成された合金層を有するオーム性
電極を設けてなる半導体装置において、前記半導体層の
厚みを2000Å以下に設定し、前記合金層と高抵抗基板と
の間に250Å以上の半導体層を残存せしめたことを特徴
とする半導体装置である。The present invention relates to a semiconductor device provided with an electrode which makes at least ohmic contact with a semiconductor operating layer on a high resistance substrate, particularly an ohmic electrode having an alloy layer formed by heat alloying an electrode metal and a semiconductor. The semiconductor device is characterized in that the thickness of the semiconductor layer is set to 2000 Å or less and 250 Å or more of the semiconductor layer is left between the alloy layer and the high resistance substrate.
次に、本発明の原理を簡単に説明する。一般に半導体
結晶へのオーム性接触はドーパントとしての不純物を含
んだ金属と半導体との加熱合金化反応により形成される
ものであり、例えば第1図のGaAs FETの場合には、GaAs
結晶表面にGeを含んだAu膜を形成したあと、約400℃で
熱処理(アロイ)することにより形成している。この際
GaAs結晶中にはn型ドーパントであるGeを大量に含んだ
N+層(合金層)がある一定の深さまで形成される。この
ような合金層の深さは、従来の素子、例えばマイクロ波
用GaAs FETの場合には動作層(半導体層)の厚みに比べ
て無視できる程度であったが、冒頭に記した超高速ディ
ジタル集積回路に用いるGaAs FETにおいては動作層の厚
みが薄い(例えば第1図の場合には1000Å)ため、合金
層の深さは動作層の厚みに対して無視できなくなる。発
明者はこの合金層の深さ(厚み)をどの程度に設定すれ
ばよいか第2図のモデルを用いて計算した。図におい
て、20は半導体層、21はオーム性金属(例えばAu,Ge,N
i)、22は合金層(N+層)である。寄生抵抗RSは、合金
層22に横方向から垂直に入る部分の抵抗R1と合金層22の
下方から廻り込む部分の抵抗R2とよりなりそれらは各々
次式で求められる。Next, the principle of the present invention will be briefly described. Generally, an ohmic contact with a semiconductor crystal is formed by a heat alloying reaction between a metal containing impurities as a dopant and a semiconductor. For example, in the case of the GaAs FET shown in FIG.
It is formed by forming an Au film containing Ge on the crystal surface and then performing a heat treatment (alloy) at about 400 ° C. On this occasion
A large amount of Ge, which is an n-type dopant, was included in the GaAs crystal.
The N + layer (alloy layer) is formed to a certain depth. The depth of such an alloy layer is negligible compared to the thickness of the operating layer (semiconductor layer) in the case of a conventional element, for example, a GaAs FET for microwaves, but the ultra-high-speed digital signal described at the beginning In a GaAs FET used in an integrated circuit, the operating layer is thin (for example, 1000 Å in the case of FIG. 1), so the depth of the alloy layer cannot be ignored with respect to the operating layer thickness. The inventor calculated how much the depth (thickness) of this alloy layer should be set by using the model of FIG. In the figure, 20 is a semiconductor layer, 21 is an ohmic metal (for example, Au, Ge, N
i) and 22 are alloy layers (N + layers). The parasitic resistance R S is composed of a resistance R 1 in a portion that vertically enters the alloy layer 22 from the lateral direction and a resistance R 2 in a portion that wraps around the alloy layer 22 from below, and they are each calculated by the following equation.
ここでwは電極幅、n,μは半導体層のキャリア密度、
電子移動度である。なお、式(4)は通常の伝送線路モ
デルを用いて求めている。計算結果の1例を第3図に示
す。第3図はa=500Å、1000Å、2000Åの各場合につ
いて、t1とRSとの関係を示したもの(ρc=10-6Ωc
m2)であり図中斜線の領域はa−t12250Åの領域、すな
わち合金層22の下方に残っている半導体層20の厚みt2が
250Å以上の領域を示している。図よりRSを十分小さく
するためには、t2を250Å以上にすべきであることが解
り、これが本発明の背景となっている。なお、本発明
(第3図でも)においてはaは2000Åまでしか考えてい
ないが、a>2000Åになると、t2250Åの場合でもRS
は十分小さくなり本発明を適用しなくても寄生抵抗の低
減が成されるためである。また第3図はρcが10-6Ω・
cm2の場合であり、かつ半導体層の比抵抗1/(e・n・
μ)が0.01Ω・cmの場合であるが、ρcがこの値(10-6
Ω・cm2)以上でかつ比抵抗が0.01Ω・cm以下の場合に
も同様にt2≧250オングストロームとすることが必要で
ある。 Where w is the electrode width, n and μ are carrier densities of the semiconductor layer,
The electron mobility. The equation (4) is obtained using a normal transmission line model. An example of the calculation result is shown in FIG. Fig. 3 shows the relationship between t 1 and R S for a = 500Å, 1000Å, 2000Å (ρ c = 10 -6 Ωc
m 2 ), and the shaded area in the figure is the area at −t 1 2250Å, that is, the thickness t 2 of the semiconductor layer 20 remaining below the alloy layer 22
Shows an area of 250 Å or more. From the figure, it is understood that t 2 should be 250 Å or more in order to make R S sufficiently small, which is the background of the present invention. In the present invention (also in FIG. 3), a is only considered up to 2000Å, but when a> 2000Å, even if t 2 250Å, R S
Is sufficiently small, and the parasitic resistance can be reduced without applying the present invention. In Fig. 3, ρ c is 10 -6 Ω ・
cm 2 and the specific resistance of the semiconductor layer is 1 / (e · n ·
μ) is 0.01 Ω · cm, but ρ c is this value (10 -6
It is necessary and resistivity in Ω · cm 2) or more is similar to t 2 ≧ 250 Å in the case of less than 0.01 Ohm · cm.
次に本発明による半導体装置の実施例をGaAs FETの場
合を例にとって説明する。第4図は本発明の実施例を説
明するための図であり、11乃至15は第1図に示す構成部
分と同じである。同一番号を付して説明を省略する。41
は合金層を概念的に示している。このGaAs FETにおいて
は動作層厚みaが1000Åであるために、合金層41の厚み
t1は750Å以下に設定してある。合金層41の厚みの設定
は、蒸着するAuGeの膜厚とアロイ方法(アロイ時間)に
主として依存するものでありt1を500ÅにするためにはA
uGeを1200Å、アロイ時間:1分間(アロイ温度420℃)が
適当であり、更に薄く、例えば300ÅにするにはAuGe厚
みは600Å、アロイ法として短時間アニール(フラッシ
ュアニール)等を適用するのが効果的である。Next, an embodiment of the semiconductor device according to the present invention will be described taking the case of a GaAs FET as an example. FIG. 4 is a diagram for explaining the embodiment of the present invention, and 11 to 15 are the same as the components shown in FIG. The same numbers are assigned and the description is omitted. 41
Indicates the alloy layer conceptually. In this GaAs FET, since the operating layer thickness a is 1000Å, the thickness of the alloy layer 41 is
t 1 is set to 750Å or less. Setting the thickness of the alloy layer 41 is intended primarily dependent on the thickness and alloy method AuGe depositing (alloy time) t 1 in order to 500Å is A
It is appropriate to use 1200 Å for uGe, alloy time: 1 minute (alloy temperature 420 ° C), and to make it thinner, for example, 300 Å, AuGe thickness is 600 Å, and short-time annealing (flash annealing) etc. is applied as an alloy method. It is effective.
以上のように合金層の厚みを規制して合金層と高抵抗
基板との間に250Å以上の半導体層を残存させることに
より従来の如く合金層を半導体層を貫通するごとく設定
した場合に比べRSは約1/2に低減され、gmも約30%改善
することができる効果を有するものである。As described above, by comparing the thickness of the alloy layer and leaving a semiconductor layer of 250 Å or more between the alloy layer and the high-resistance substrate, the alloy layer is set to penetrate the semiconductor layer as in the conventional case. S is reduced to about 1/2, and gm can be improved by about 30%.
第1図は従来の半導体装置を略示的に示す断面図、第2
図は本発明による半導体装置の原理の説明、第3図は半
導体層の厚みと寄生抵抗との関係を示す図、第4図は本
発明の実施例を略示的に示す断面図である。 11……半絶縁性GaAs基板、12……n型GaAs半導体層、13
……ゲート電極、14……ソース電極、15……ドレイン電
極、21……オーム性電極、22……合金層(N+層)、41…
…合金層。FIG. 1 is a sectional view schematically showing a conventional semiconductor device, and FIG.
FIG. 3 is a diagram showing the principle of a semiconductor device according to the present invention, FIG. 3 is a diagram showing the relationship between the thickness of a semiconductor layer and parasitic resistance, and FIG. 4 is a sectional view schematically showing an embodiment of the present invention. 11 ... Semi-insulating GaAs substrate, 12 ... N-type GaAs semiconductor layer, 13
...... Gate electrode, 14 ...... Source electrode, 15 …… Drain electrode, 21 …… Ohm electrode, 22 …… Alloy layer (N + layer), 41 ・ ・ ・
... alloy layer.
Claims (1)
該半導体層とオーム性接触をなし、かつ、該半導体層に
対してドーパントなる不純物を含んだ金属電極と半導体
層との加熱合金化により形成された合金層を有するオー
ム性電極を設けてなる半導体装置であって、該オーム性
電極の半導体層への接触比抵抗が1×10-6Ω・cm2以上
でかつ半導体層の比抵抗が0.01Ω・cm以下であり、前記
半導体動作層の厚みを2000オングストローム以下に設定
し、前記合金層と前記高抵抗半導体基板との間に250オ
ングストローム以上の半導体層を残存せしめたことを特
徴とする半導体装置。1. A semiconductor operating layer on a high resistance semiconductor substrate,
A semiconductor provided with an ohmic electrode which is in ohmic contact with the semiconductor layer and which has an alloy layer formed by thermal alloying of a metal electrode containing a dopant impurity with the semiconductor layer and the semiconductor layer. A contact resistance of the ohmic electrode to the semiconductor layer is 1 × 10 −6 Ω · cm 2 or more, and the semiconductor layer has a specific resistance of 0.01 Ω · cm or less; Is set to 2000 angstroms or less, and a semiconductor layer of 250 angstroms or more is left between the alloy layer and the high resistance semiconductor substrate.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59103859A JPH0812867B2 (en) | 1984-05-23 | 1984-05-23 | Semiconductor device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59103859A JPH0812867B2 (en) | 1984-05-23 | 1984-05-23 | Semiconductor device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS60247976A JPS60247976A (en) | 1985-12-07 |
| JPH0812867B2 true JPH0812867B2 (en) | 1996-02-07 |
Family
ID=14365171
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP59103859A Expired - Lifetime JPH0812867B2 (en) | 1984-05-23 | 1984-05-23 | Semiconductor device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0812867B2 (en) |
Family Cites Families (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5559781A (en) * | 1978-10-30 | 1980-05-06 | Fujitsu Ltd | Method of fabricating semiconductor device |
| JPS5624979A (en) * | 1979-08-08 | 1981-03-10 | Nec Corp | Field effect transistor |
| JPS5898980A (en) * | 1981-12-09 | 1983-06-13 | Hitachi Ltd | Semiconductor device and its manufacturing method |
| JPS58134478A (en) * | 1982-02-04 | 1983-08-10 | Sanyo Electric Co Ltd | Manufacturing method of compound semiconductor FET |
| JPS5979576A (en) * | 1982-10-29 | 1984-05-08 | Fujitsu Ltd | Field effect semiconductor device |
-
1984
- 1984-05-23 JP JP59103859A patent/JPH0812867B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS60247976A (en) | 1985-12-07 |
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