JPS594867B2 - Method of manufacturing field effect transistor - Google Patents
Method of manufacturing field effect transistorInfo
- Publication number
- JPS594867B2 JPS594867B2 JP489378A JP489378A JPS594867B2 JP S594867 B2 JPS594867 B2 JP S594867B2 JP 489378 A JP489378 A JP 489378A JP 489378 A JP489378 A JP 489378A JP S594867 B2 JPS594867 B2 JP S594867B2
- Authority
- JP
- Japan
- Prior art keywords
- substrate
- region
- field effect
- effect transistor
- semiconductor layer
- 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
Links
Landscapes
- Junction Field-Effect Transistors (AREA)
Description
【発明の詳細な説明】
本発明は、電界効果トランジスタ、特に高周波化、高出
力化に適した構造を容易に実現することができる製造方
法を提供するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention provides a manufacturing method that can easily realize a field effect transistor, particularly a structure suitable for high frequency and high output.
従来、縦形構造の電界効果トランジスタとして、第1図
、第2図に示す如き、埋め込みゲート形構造及び表面配
線構造の素子があつた。Conventionally, field effect transistors with a vertical structure include devices with a buried gate structure and a surface wiring structure, as shown in FIGS. 1 and 2.
図中1はドレイン領域となる高不純物濃速の半導体基板
、2は基板1より低不純物濃度の半導体層、3は基板1
と反対導電型を有するゲート領域、4は基板1と同一導
電型のソース領域である。これらの構造における欠点は
、高周波特性を向上させようとすると出力が低下すると
いうことである。その理由5 は、第1図、第2図にお
いて、高出力を得ようとして面積を大きくして電流を大
きくしようとすると、ゲート3とドレイン1間の静電容
量が増加して、周波数特性が低下する。また、高電圧動
作をさせようとして、ゲート3とドレイン1の距離を1
0大きくすると電流通路が長くなつてチャンネルの直列
抵抗が大きくなり、電流が流れにくくなつて大出力にな
らない。高周波特性を向上するため静電容量を小さくし
ようとして半導体層2を厚くすると、同じように電流が
流れにくくなり高出力に15ならない。以上のような欠
点を補う構造として第3図に示す如き構造が提案された
。この構造は、ドレイン領域1から高濃度領域11がソ
ース領域4に対向する領域で突出し、ゲート3から拡が
る空気層の縁20の形に沿うように形成されている20
ため、ゲート・ ドレイン間の静電容量を増加させるこ
となく電流通路の直列抵抗を下げ、大電流を出しうる。
上記構造が高周波化、高出力化に適した構造であること
は上記説明より明らかであるが、それを25実現するこ
とは極めて困難であつた。In the figure, 1 is a semiconductor substrate with a high impurity concentration that becomes a drain region, 2 is a semiconductor layer with a lower impurity concentration than the substrate 1, and 3 is a substrate 1
4 is a gate region having a conductivity type opposite to that of the substrate 1, and a source region 4 having the same conductivity type as the substrate 1. A drawback of these structures is that the output decreases when trying to improve high frequency characteristics. Reason 5 is that in Figures 1 and 2, if you try to increase the area and increase the current in order to obtain high output, the capacitance between the gate 3 and the drain 1 will increase, and the frequency characteristics will change. descend. In addition, in order to operate at a high voltage, the distance between gate 3 and drain 1 was reduced by 1
If the value is set to 0, the current path will become longer and the series resistance of the channel will increase, making it difficult for current to flow and preventing high output. If the semiconductor layer 2 is made thicker in an attempt to reduce the capacitance in order to improve high frequency characteristics, it will similarly become difficult for current to flow and high output will not be achieved. A structure as shown in FIG. 3 has been proposed as a structure to compensate for the above-mentioned drawbacks. In this structure, a high concentration region 11 protrudes from a drain region 1 in a region facing a source region 4 and is formed along the shape of an edge 20 of an air layer extending from a gate 3.
Therefore, the series resistance of the current path can be lowered and a large current can be generated without increasing the capacitance between the gate and drain.
Although it is clear from the above description that the above structure is suitable for higher frequencies and higher outputs, it has been extremely difficult to realize this.
すなわち、このような構造を得る方法として、先ず上記
突出した領域11を含む厚さまで半導体層2を気相成長
法などで成長させ、次いで領域11となるべき部分に基
板1と同一導電形の不純30物を高濃度に拡散して領域
11を形成した後、再び半導体層2を所望の厚さまで成
長させる方法や、基板1の所定表面領域を選択的に掘削
して凹部を形成した後、この凹部を形成した基板1上に
半導体層2を気相成長によつて形成し、上記凹部を投3
5影した半導体層2の表面層にゲート領域3を、上部凹
部以外の基板1の表面領域を投影した半導体層2の表面
層にソース領域4を形成する方法が提、Cl−案されて
いるが、前者の方法による場合は、半導体層2を形成す
るための気相成長を2度に分けて行う必要があり、また
後者の方法による場合は、半導体層2にも凹部が形成さ
れることになるので、ゲート領域3やソース領域4形成
のための写真製版が困難になるという不都合があつた。That is, as a method for obtaining such a structure, first, the semiconductor layer 2 is grown by a vapor phase growth method or the like to a thickness that includes the protruding region 11, and then an impurity having the same conductivity type as that of the substrate 1 is added to the portion that is to become the region 11. 30 at a high concentration to form the region 11, and then grow the semiconductor layer 2 again to a desired thickness, or selectively excavate a predetermined surface region of the substrate 1 to form a recess. A semiconductor layer 2 is formed by vapor phase growth on a substrate 1 in which a recessed portion is formed, and the recessed portion is
A method is proposed in which the gate region 3 is formed in the surface layer of the semiconductor layer 2 which is projected from the surface of the semiconductor layer 2, and the source region 4 is formed in the surface layer of the semiconductor layer 2 which is projected by the surface region of the substrate 1 other than the upper concave portion. However, when using the former method, it is necessary to perform vapor phase growth in two steps to form the semiconductor layer 2, and when using the latter method, recesses are also formed in the semiconductor layer 2. Therefore, there was an inconvenience that photolithography for forming the gate region 3 and source region 4 became difficult.
この発明はこのような点に鑑みてなされたもので、ゲー
ト・ドレイン間の容量を増大させることなくドレイン抵
抗を小さくして大出力化を可能にした構造の電界効果ト
ランジスタを容易に実現することのできる製造方法を提
供することを目的とする。This invention was made in view of the above points, and an object of the present invention is to easily realize a field effect transistor having a structure that enables high output by reducing drain resistance without increasing the capacitance between the gate and drain. The purpose is to provide a manufacturing method that allows for
以下、図を参照してこの発明の一実施例について説明す
る。An embodiment of the present invention will be described below with reference to the drawings.
先ず第4図aに示すように、n+形半導体基板1の所定
表面領域上に、半導体酸化膜等の絶縁膜6を被着する。
次に第4図bに示すように、上記絶縁膜6をマスクとし
て基板1と同一導電形と対与する高濃度の不純物を拡散
あるいはイオン注入等で基板1に導入し、高濃度領域1
0を形成する。ここで上記導入する不純物としては、基
板1中の不純物よりも半導体中での拡散速度が大きいも
のが選ばれる。一例として、基板1中の不純物がアンチ
モンのときには、砒素とかりンが使用できる。これらの
不純物としてl族、族以外の不純物が使用できることは
当然である。その ト後、絶縁膜6を除去して、第4図
cに示すように、高濃度領域10を含む基板1の一主面
上に、n−形半導体層2を気相成長法によつて形成する
。次いで第4図dに示すように、通常の方法、例えば拡
散マスクを使用した熱拡散法でゲート領域3お 5よび
ソース領域4を形成する。するとこの工程の過程におい
て、基板1と領域10中の不純物の拡散速度の差によつ
て、第4図dに示すように、半導体層2中に領域10か
ら高濃度領域11がソース領域4に対向するように突出
して形成される。このように拡散によつて突出する領域
11は、拡散が中央部で深く、周辺部では横に広がるた
め浅くなるように形成されるので、その形状はゲート領
域3から拡がる突之層の縁の形状に沿う形を容易にとり
得る。なお、以上はnチャンネルの電界効果トランジン
タの製造を例にとつて説明したが、この発明はPチヤン
ネルの電界効果トランジスタの製造にも適用できること
はいうまでもない。First, as shown in FIG. 4a, an insulating film 6 such as a semiconductor oxide film is deposited on a predetermined surface region of an n+ type semiconductor substrate 1. As shown in FIG.
Next, as shown in FIG. 4b, using the insulating film 6 as a mask, a high concentration impurity having the same conductivity type as the substrate 1 is introduced into the substrate 1 by diffusion or ion implantation.
form 0. Here, as the impurity to be introduced, one whose diffusion rate in the semiconductor is higher than that of the impurity in the substrate 1 is selected. For example, when the impurity in the substrate 1 is antimony, arsenic and karin can be used. It is a matter of course that impurities other than group I and group I can be used as these impurities. After that, the insulating film 6 is removed and, as shown in FIG. Form. Next, as shown in FIG. 4d, gate regions 3 and 5 and source regions 4 are formed by a conventional method, such as thermal diffusion using a diffusion mask. Then, during this process, due to the difference in the diffusion rate of impurities between the substrate 1 and the region 10, the high concentration region 11 from the region 10 in the semiconductor layer 2 becomes the source region 4, as shown in FIG. 4d. They are formed to protrude so as to face each other. In this way, the region 11 that protrudes due to diffusion is formed so that the diffusion is deep in the center and shallow in the peripheral region because it spreads laterally, so its shape is similar to that of the edge of the protruding layer extending from the gate region 3. It can easily take a shape that follows the shape. Although the above description has been made by taking as an example the manufacture of an n-channel field effect transistor, it goes without saying that the present invention can also be applied to the manufacture of a p-channel field effect transistor.
以上述べたようにこの発明の方法によれば、ドレインと
なる半導体基板の不純物より拡散速度の大きい不純物を
上記基板の一部領域に導入することにより、従来方法の
ように気相成長を2度に分けて行つたり、エツチングし
たりすることなく、周波数特性のすぐれた大出力電界効
果トランジスタを容易に得ることができる。As described above, according to the method of the present invention, by introducing an impurity having a higher diffusion rate than the impurity of the semiconductor substrate that becomes the drain into a partial region of the substrate, vapor phase growth is performed twice as in the conventional method. A high output field effect transistor with excellent frequency characteristics can be easily obtained without performing separate etching or etching.
第1図および第2図はそれぞれ従来の電界効果トランジ
スタを示す断面図、第3図は改良された構造を有する電
界効果トランジスタを示す断面図、第4図a−dはこの
発明の一実施例を示す工程順の断面図である。
図において、1は半導体基板、2は半導体層、3はゲー
ト領域、4はソース領域、10および11は高濃度領域
である。1 and 2 are sectional views showing a conventional field effect transistor, FIG. 3 is a sectional view showing a field effect transistor having an improved structure, and FIGS. 4 a to 4 d are an embodiment of the present invention. FIG. In the figure, 1 is a semiconductor substrate, 2 is a semiconductor layer, 3 is a gate region, 4 is a source region, and 10 and 11 are high concentration regions.
Claims (1)
領域に上記基板の不純物より拡散速度の大きい不純物を
含む上記基板と同一導電型の低比抵抗半導体領域を選択
的に形成する工程、上記半導体領域を含む上記基板の一
主面上に上記基板と同一導電型の高比抵抗半導体層を形
成する工程、上記半導体領域を投影した上記半導体層の
表面領域に上記基板と同一導電型の低比抵抗ソース領域
を形成する工程を含む電界効果トランジスタの製造方法
。 2 高比抵抗半導体層は気相成長法により形成されるこ
とを特徴とする特許請求の範囲第1項記載の電界効果ト
ランジスタの製造方法。[Scope of Claims] 1. A low resistivity semiconductor region having the same conductivity type as the substrate and containing an impurity having a higher diffusion rate than the impurities of the substrate is selectively formed in a predetermined surface region of a low resistivity semiconductor substrate serving as a drain region. a step of forming a high resistivity semiconductor layer of the same conductivity type as the substrate on one main surface of the substrate including the semiconductor region; A method for manufacturing a field effect transistor, including a step of forming a conductive type low resistivity source region. 2. The method for manufacturing a field effect transistor according to claim 1, wherein the high resistivity semiconductor layer is formed by a vapor phase growth method.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP489378A JPS594867B2 (en) | 1978-01-19 | 1978-01-19 | Method of manufacturing field effect transistor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP489378A JPS594867B2 (en) | 1978-01-19 | 1978-01-19 | Method of manufacturing field effect transistor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5497382A JPS5497382A (en) | 1979-08-01 |
| JPS594867B2 true JPS594867B2 (en) | 1984-02-01 |
Family
ID=11596341
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP489378A Expired JPS594867B2 (en) | 1978-01-19 | 1978-01-19 | Method of manufacturing field effect transistor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS594867B2 (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0183973U (en) * | 1987-11-27 | 1989-06-05 |
-
1978
- 1978-01-19 JP JP489378A patent/JPS594867B2/en not_active Expired
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0183973U (en) * | 1987-11-27 | 1989-06-05 |
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5497382A (en) | 1979-08-01 |
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