JPS6188567A - Semiconductor device - Google Patents
Semiconductor deviceInfo
- Publication number
- JPS6188567A JPS6188567A JP59209876A JP20987684A JPS6188567A JP S6188567 A JPS6188567 A JP S6188567A JP 59209876 A JP59209876 A JP 59209876A JP 20987684 A JP20987684 A JP 20987684A JP S6188567 A JPS6188567 A JP S6188567A
- Authority
- JP
- Japan
- Prior art keywords
- wafer
- field effect
- compound semiconductor
- effect transistor
- semiconductor device
- 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.)
- Granted
Links
Classifications
-
- 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
- H10D62/40—Crystalline structures
- H10D62/405—Orientations of crystalline planes
-
- 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]
-
- 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
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D84/00—Integrated devices formed in or on semiconductor substrates that comprise only semiconducting layers, e.g. on Si wafers or on GaAs-on-Si wafers
- H10D84/01—Manufacture or treatment
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D84/00—Integrated devices formed in or on semiconductor substrates that comprise only semiconducting layers, e.g. on Si wafers or on GaAs-on-Si wafers
- H10D84/01—Manufacture or treatment
- H10D84/0123—Integrating together multiple components covered by H10D12/00 or H10D30/00, e.g. integrating multiple IGBTs
- H10D84/0126—Integrating together multiple components covered by H10D12/00 or H10D30/00, e.g. integrating multiple IGBTs the components including insulated gates, e.g. IGFETs
- H10D84/0158—Integrating together multiple components covered by H10D12/00 or H10D30/00, e.g. integrating multiple IGBTs the components including insulated gates, e.g. IGFETs the components including FinFETs
Landscapes
- 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、化合物半導体ウェハ上に複数の電界効果型ト
ランジスタを形成した場合、その全ての特性を均一化す
るのに有効な構成をもった半導体装置に関する。[Detailed Description of the Invention] [Industrial Application Field] The present invention has a configuration that is effective for uniformizing all the characteristics when a plurality of field effect transistors are formed on a compound semiconductor wafer. Related to semiconductor devices.
従来、GaAsウェハに電界効果型トランジスタを形成
する場合、主表面が(100)面であるGaAsウェハ
にドレイン電流が<011>軸と平行に流れる向きを採
っている。Conventionally, when a field effect transistor is formed on a GaAs wafer, a drain current is oriented to flow parallel to the <011> axis in the GaAs wafer whose main surface is a (100) plane.
このようにするのは、諸素子の形成が完了したGaAs
ウェハをチップに分離する場合に襞間し易いことが主た
る理由になっている。This is done after the formation of the various elements is completed.
The main reason for this is that it is easy to create creases when separating the wafer into chips.
また、現在、化合物半導体を材料とする集積回路は、そ
の実用化に向けて多くの開発・研究かなされているが、
その場合、集積回路に含まれ電界効果型トランジスタの
特性を均一化することが不可欠である。Furthermore, currently, much development and research is being carried out on integrated circuits made of compound semiconductors with the aim of putting them into practical use.
In this case, it is essential to equalize the characteristics of the field effect transistors included in the integrated circuit.
通常、GaAsウェハに複数の電界効果型トランジスタ
を形成した場合、各電界効果型トランジスタの闇値電圧
■いのバラツキは大きいことが知られている。It is known that normally, when a plurality of field effect transistors are formed on a GaAs wafer, there is a large variation in the dark value voltage of each field effect transistor.
この理由は、G a A s 基板とパノシヘーション
用絶縁膜との間のストレスに依って電界効果型トランジ
スタのチャネル領域にピエゾ電荷が生ずる為であるとさ
れている(Chang、M、F、ほか、Appl、Ph
ys、Lett、、vol。The reason for this is said to be that piezoelectric charges are generated in the channel region of the field effect transistor due to the stress between the Ga As substrate and the pannosification insulating film (Chang, M. F., et al. Appl, Ph.
ys, Lett,, vol.
45、no、3.pp、279−281.Aug。45, no, 3. pp, 279-281. Aug.
1.1984>。1.1984>.
第3図は(100)面を主面とするGaAsウェハにド
レイン電流が<01丁>軸に平行となるよう電界効果型
トランジスタを形成した場合、闇値電圧Vいがパッシベ
ーション用絶縁膜の膜厚に依存して如何に変化するかを
表す線図である。Figure 3 shows that when a field effect transistor is formed on a GaAs wafer whose main surface is the (100) plane so that the drain current is parallel to the <01> axis, the dark value voltage V is the thickness of the passivation insulating film. It is a diagram showing how it changes depending on thickness.
図では、縦軸に闇値電圧Vいを、横軸にゲート長L9を
それぞれ採り、バソシヘーション用絶縁膜である二酸化
シリコン(SiOz)膜の厚さdをバラメークとしであ
る。In the figure, the vertical axis represents the dark voltage V, the horizontal axis represents the gate length L9, and the thickness d of the silicon dioxide (SiOz) film, which is an insulating film for absorption, is varied.
図から判るように、短チャネルになると闇値電圧Vth
はS i O2膜の厚さdに依って大きなバラツキを生
じている。尚、この種の半導体装置を短チヤネル化する
ことは集積度を向上する面で不可欠であるのは云うまで
もない。As can be seen from the figure, when the channel becomes short, the dark value voltage Vth
has a large variation depending on the thickness d of the S i O2 film. It goes without saying that shortening the channels of this type of semiconductor device is essential for improving the degree of integration.
−mに、化合物半導体を用いた集積回路は、シリコン半
導体を用いた集積回路と比較すると未だに不安定な面が
多い。-m, integrated circuits using compound semiconductors are still unstable in many aspects compared to integrated circuits using silicon semiconductors.
前記のような集積回路に於いて、その中に含まれている
多数の電界効果型トランジスタの特性、特に、闇値電圧
Vいが不均一であると集積回路全体が動作不能となる。In the above-mentioned integrated circuit, if the characteristics of the large number of field effect transistors included therein, especially the dark value voltage V, are non-uniform, the entire integrated circuit becomes inoperable.
従って、そのようなものは不良品として取り扱わなけれ
ばならないので、その製造歩留りは非常に低いものとな
っている。Therefore, such products must be treated as defective products, resulting in a very low manufacturing yield.
本発明は、化合物半導体ウェハに形成する複数の電界効
果型トランジスタの方向を通期に選択することに依り、
闇値電圧■5、の均一化を図っている。The present invention achieves the following by selecting the direction of a plurality of field effect transistors formed on a compound semiconductor wafer throughout the period.
Efforts are being made to equalize the dark value voltage (■5).
本発明に依る半導体装置では、Nが任意の自然数である
場合に於いて、化合物半導体結晶の(N10)面が主面
になっていて、ドレイン電流の流れる方向が<1N0>
軸と平行になるようにゲート電極、ソース領域、ドレイ
ン領域が形成されている。In the semiconductor device according to the present invention, when N is an arbitrary natural number, the (N10) plane of the compound semiconductor crystal is the main surface, and the direction in which the drain current flows is <1N0>
A gate electrode, a source region, and a drain region are formed parallel to the axis.
前記のような構成を採ると、化合物半導体の同一ウェハ
上に形成された各半導体装置は、そのパッシベーション
用絶縁膜の膜厚の如何に拘わらず闇値電圧Vいは略一定
に維持される。With the above configuration, the dark voltage V of each semiconductor device formed on the same compound semiconductor wafer is maintained substantially constant regardless of the thickness of the passivation insulating film.
第1図は本発明一実施例を説明する為の工程要所に於け
る半導体ウェハの要部平面図を表している。尚、本実施
例ではN=1とした場合であり、従って、半導体ウェハ
の面指数は(110)である。FIG. 1 shows a plan view of the main parts of a semiconductor wafer at key points in the process for explaining one embodiment of the present invention. In this embodiment, N=1, and therefore the surface index of the semiconductor wafer is (110).
図に於いて、1は主面の面指数が(110)であるGa
Asウェハ、2はドレイン電流IDSの方向がGaAs
ウェハ1の<110>軸と平行であるように形成された
電界効果型トランジスタ、2Gはゲート電極、2Sはソ
ース領域、2Dはドレイン領域をそれぞれ示している。In the figure, 1 is Ga whose main surface has a surface index of (110).
As wafer 2, the direction of the drain current IDS is GaAs.
In the field effect transistor formed parallel to the <110> axis of the wafer 1, 2G indicates a gate electrode, 2S indicates a source region, and 2D indicates a drain region.
このような構成にすると、電界効果型トランジスタ2の
チャネル領域では圧電分極の影響、従って、ピエゾ電荷
の影響を受は難くなり、闇値電圧Vいのバラツキはなく
なる。With such a configuration, the channel region of the field-effect transistor 2 is less susceptible to the influence of piezoelectric polarization, and hence to the influence of piezoelectric charges, and variations in the dark value voltage V are eliminated.
第2図は本発明一実施例の効果を説明する為の線図を表
している。FIG. 2 shows a diagram for explaining the effects of one embodiment of the present invention.
図では、縦軸に闇値電圧Vいを、横軸に層間絶縁膜の厚
さdをそれぞれ採ってあり、また、実線は本発明一実施
例の特性線を、そして、○印は従来例の特性線をそれぞ
れ示している。In the figure, the vertical axis represents the dark voltage V, and the horizontal axis represents the thickness d of the interlayer insulating film.The solid line represents the characteristic line of one embodiment of the present invention, and the circle mark represents the conventional example. The characteristic lines of each are shown.
このデータを得た電界効果型トランジスタのゲート長L
9は1.4〔μm〕とした。Gate length L of the field effect transistor from which this data was obtained
9 was set to 1.4 [μm].
図から明らかなように、本実施例の場合、層間絶縁膜に
於ける厚さの如何を問わず闇値電圧Vいの変動は発生し
ていない。As is clear from the figure, in the case of this example, no variation in the dark value voltage V occurs regardless of the thickness of the interlayer insulating film.
本発明に依る半導体装置では、Nが任意の自然数である
場合に於いて、化合物半導体結晶の(N10)面を主面
とし且つドレイン電流の流れる方向が<1N0>軸と平
行であるように形成されている。In the semiconductor device according to the present invention, when N is an arbitrary natural number, the semiconductor device is formed so that the (N10) plane of the compound semiconductor crystal is the main surface and the direction in which the drain current flows is parallel to the <1N0> axis. has been done.
このような構成にすると、ウェハ上に形成された全ての
半導体装置が化合物半導体基板と保護膜との熱膨張率の
相違に起因して発生するストレスの彫金を受けることが
少なくなり、その結果、チャネル領域に圧電分極に依る
ピエゾ電荷が生ずることもなくなり、相互伝導度9.、
lが高く且つ短チヤネル化しても闇値電圧■いが均一に
維持されるので、その製造歩留りは大きく改善され、従
って、化合物半導体集積回路を構成する場合に有効であ
る。With this configuration, all the semiconductor devices formed on the wafer are less likely to be subjected to stress engraving caused by the difference in thermal expansion coefficient between the compound semiconductor substrate and the protective film, and as a result, No piezoelectric charge is generated in the channel region due to piezoelectric polarization, and the mutual conductivity is 9. ,
Even if l is high and the channel is shortened, the dark voltage value l is maintained uniformly, so the manufacturing yield is greatly improved, and it is therefore effective in constructing compound semiconductor integrated circuits.
第1図は本発明一実施例を説明する為の工程要所に於け
る半導体ウェハの要部平面図、第2図は第1図に示した
本発明一実施例の効果を説明する為の線図、第3図は電
界効果型トランジスタの闇値電圧■いがパンシベーショ
ン用絶縁膜の膜厚に依存して変化することを明らかにす
る線図をそれぞれ表している。
図に於いて、1は主面の面指数が(110)であるGa
Asウェハ、2はドレイン電流105の方向がGaAs
ウェハ1の<110>軸と平行であるように形成された
電界効果型トランジスタ、2Gはゲート電極、2Sはソ
ース頭載、2Dはドレイン領域をそれぞれ示している。
特許出願人 冨士通株式会社
代理人弁理士 相 谷 昭 司
代理人弁理士 渡 邊 弘 −
第2図
0 0.5 1.O
N間總繰膜厚 (7−+m)
第3図
Lq(pm)
手続主甫正書
昭和60年3月15日
特許庁長官 志 賀 学 殿
(特許庁審査官 殿)1 事件の表示
昭和59年特許願第209876号2 発明の名称
半導体装置
3 補正をする者
事件との関係 特許出願人
住 所 神奈川県用崎市中原区上小田中1015番地
名称(522)冨士通株式会社
代表者 山 本 卓 眞
4代理人
住 所 東京都港区虎ノ門−丁目20番7号ン・シリ
サイド(WSi)を雷極材゛叫、171ア、吏(1、発
明の名称を、
「化合物半導体電界効果トランジスタ」、と補正する。
(2、特許請求の範囲の記載を、
「Nが任意の自然数であるとした場合に於いて、化合物
半導体結晶の(N10)面を主面とし且つドレイン電流
の流れる方向が<1N0>軸と平行であるように形成さ
れたことを特徴とする化合物半導体重1効果トランジス
タ。」、
と補正する。
(3)明細書第1頁第13行及び第14行、「半導体装
置」、の記載を、
「化合物半導体電界効果トランジスタ」、と補正する。
(4)同第5頁第1行、1半導体ウェハ」、の記載を、
「化合物半導体ウェハ」、
と補正する。
(5)同第6頁第1行及び第2行の記載を、「このデー
タは、GaAsウェハ上にタングステれたショットキ・
バリヤ型電界効果トランジスタ(以下、MESFETと
する)から得られた。」、と補正する。
(6) 同第6頁第5行の記載を、
[の変動は発生していない。
以上の説明は、GaAsMESFETを対象にしたもの
であるが、GaAs以外の化合物半導体ウェハ(例えば
、InP、InGaAsなど)を用いた場合にも同じ効
果を得ることができ、また、ゲート電極にpn接合を用
いた電界効果トランジスタ、或いは、絶縁ゲート型の電
界効果トランジスタやヘテロ接合を用いた電界効果トラ
ンジスタ(HE M Tなと)についても同効である。
」、と補正する。FIG. 1 is a plan view of a main part of a semiconductor wafer at key points in the process for explaining one embodiment of the present invention, and FIG. The diagrams and FIG. 3 are diagrams each showing that the dark voltage of a field effect transistor changes depending on the thickness of the pansivation insulating film. In the figure, 1 is Ga whose main surface has a surface index of (110).
As wafer 2, the direction of the drain current 105 is GaAs.
In the field effect transistor formed parallel to the <110> axis of the wafer 1, 2G indicates a gate electrode, 2S indicates a source head, and 2D indicates a drain region. Patent Applicant Fujitsu Co., Ltd. Representative Patent Attorney Akio Aitani Representative Patent Attorney Hiroshi Watanabe - Figure 2 0 0.5 1. O N repeated film thickness (7-+m) Figure 3 Lq (pm) Procedural master's letter March 15, 1985 Mr. Manabu Shiga, Commissioner of the Patent Office (Mr. Examiner of the Patent Office) 1 Display of case Showa 1959 Patent Application No. 209876 2 Name of the invention Semiconductor device 3 Relationship to the case of the person making the amendment Patent applicant Address 1015 Kamiodanaka, Nakahara-ku, Yozaki City, Kanagawa Prefecture Name (522) Fujitsu Co., Ltd. Representative Yamamoto Taku Shin 4 Agent address: 20-7, Toranomon-chome, Minato-ku, Tokyo, 171 A., N. Silicide (WSi) as a lightning electrode material (1. Name of the invention: ``Compound Semiconductor Field Effect Transistor.'' (2. Amend the claim statement to ``If N is an arbitrary natural number, the (N10) plane of the compound semiconductor crystal is the principal plane, and the direction in which the drain current flows is "A compound semiconductor heavy single-effect transistor characterized by being formed parallel to the <1N0>axis." (3) Page 1, lines 13 and 14 of the specification, "Semiconductor device '' is corrected to read ``compound semiconductor field effect transistor.'' (4) The description ``1 semiconductor wafer,'' page 5, line 1, is corrected to read ``compound semiconductor wafer.'' (5 ) The statement in the first and second lines of page 6 was changed to ``This data is based on a Schottky film made of tungsten on a GaAs wafer.
It was obtained from a barrier type field effect transistor (hereinafter referred to as MESFET). ”, he corrected. (6) The statement on page 6, line 5 of the same document has been changed to: [No change has occurred. The above explanation is for GaAs MESFETs, but the same effect can be obtained when using compound semiconductor wafers other than GaAs (e.g., InP, InGaAs, etc.). The same effect applies to a field effect transistor using an insulated gate type field effect transistor or a field effect transistor using a heterojunction (HEMT). ”, he corrected.
Claims (1)
半導体結晶の(N10)面を主面とし且つドレイン電流
の流れる方向が<1@N@0>軸と平行であるように形
成された半導体装置。When N is an arbitrary natural number, the compound semiconductor crystal is formed so that the (N10) plane is the main surface and the direction in which the drain current flows is parallel to the <1@N@0> axis. Semiconductor equipment.
Priority Applications (5)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59209876A JPS6188567A (en) | 1984-10-08 | 1984-10-08 | Semiconductor device |
| EP85307129A EP0178133B1 (en) | 1984-10-08 | 1985-10-04 | Semiconductor integrated circuit device |
| KR1019850007310A KR900000584B1 (en) | 1984-07-11 | 1985-10-04 | Semiconductor integrated circuit device |
| DE8585307129T DE3581159D1 (en) | 1984-10-08 | 1985-10-04 | SEMICONDUCTOR ARRANGEMENT WITH INTEGRATED CIRCUIT. |
| US07/158,043 US4791471A (en) | 1984-10-08 | 1988-02-16 | Semiconductor integrated circuit device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59209876A JPS6188567A (en) | 1984-10-08 | 1984-10-08 | Semiconductor device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6188567A true JPS6188567A (en) | 1986-05-06 |
| JPH033933B2 JPH033933B2 (en) | 1991-01-21 |
Family
ID=16580104
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP59209876A Granted JPS6188567A (en) | 1984-07-11 | 1984-10-08 | Semiconductor device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6188567A (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH06216394A (en) * | 1993-01-14 | 1994-08-05 | Nec Corp | Field effect transistor |
| US5698888A (en) * | 1995-04-24 | 1997-12-16 | Nec Corporation | Compound semiconductor field effect transistor free from piezoelectric effects regardless of orientation of gate electrode |
Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS58145168A (en) * | 1982-02-24 | 1983-08-29 | Fujitsu Ltd | Semiconductor device |
-
1984
- 1984-10-08 JP JP59209876A patent/JPS6188567A/en active Granted
Patent Citations (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS58145168A (en) * | 1982-02-24 | 1983-08-29 | Fujitsu Ltd | Semiconductor device |
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH06216394A (en) * | 1993-01-14 | 1994-08-05 | Nec Corp | Field effect transistor |
| US5442227A (en) * | 1993-01-14 | 1995-08-15 | Nec Corporation | Field effect transistor having a low threshold voltage shift |
| US5698888A (en) * | 1995-04-24 | 1997-12-16 | Nec Corporation | Compound semiconductor field effect transistor free from piezoelectric effects regardless of orientation of gate electrode |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH033933B2 (en) | 1991-01-21 |
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