JPS61229366A - Semiconductor device - Google Patents

Semiconductor device

Info

Publication number
JPS61229366A
JPS61229366A JP60070365A JP7036585A JPS61229366A JP S61229366 A JPS61229366 A JP S61229366A JP 60070365 A JP60070365 A JP 60070365A JP 7036585 A JP7036585 A JP 7036585A JP S61229366 A JPS61229366 A JP S61229366A
Authority
JP
Japan
Prior art keywords
region
well
impurity concentration
channel region
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
Application number
JP60070365A
Other languages
Japanese (ja)
Other versions
JPH0550863B2 (en
Inventor
Kiyoshi Nishimura
清 西村
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.)
Rohm Co Ltd
Original Assignee
Rohm Co 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 Rohm Co Ltd filed Critical Rohm Co Ltd
Priority to JP60070365A priority Critical patent/JPS61229366A/en
Publication of JPS61229366A publication Critical patent/JPS61229366A/en
Publication of JPH0550863B2 publication Critical patent/JPH0550863B2/ja
Granted 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
    • H10D62/17Semiconductor regions connected to electrodes not carrying current to be rectified, amplified or switched, e.g. channel regions
    • H10D62/213Channel regions of field-effect devices
    • H10D62/221Channel regions of field-effect devices of FETs

Landscapes

  • Metal-Oxide And Bipolar Metal-Oxide Semiconductor Integrated Circuits (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は、たとえば、MO3電界効果トランジスタな
どの半導体装置に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to semiconductor devices such as MO3 field effect transistors.

〔従来の技術〕[Conventional technology]

一般に、電界効果トランジスタは、第6図および第7図
に示すように、N型シリコンなどの一導電型の半導体基
板2に反対導電型の導電領域としてのpウェル(wel
l) 4が形成され、このpウェル4には、一定の間隔
を置いてpウェル4とは反対導電型のソース領域6およ
びドレイン領域8が形成され、これらソース領域6およ
びドレイン領域8の間にはチャンネル領域10が形成さ
れている。半導体基板2、pウェル4、ソース領域6お
よびドレイン領域8の表面は、酸化膜12で覆われてい
るとともに、ソース領域6およびドレイン領域80表面
にはソース電極14、ドレイン電極16が形成され、チ
ャンネル領域10を覆う酸化膜13は他の部分より薄く
設定され、この薄い酸化膜13の表面には、アルミニウ
ムなどの蒸着によってゲート電極18が形成されている
Generally, as shown in FIGS. 6 and 7, a field effect transistor includes a semiconductor substrate 2 of one conductivity type, such as N-type silicon, and a p-well (well) as a conductive region of the opposite conductivity type.
l) 4 is formed, and in this p-well 4, a source region 6 and a drain region 8 of the opposite conductivity type to that of the p-well 4 are formed at regular intervals, and between these source region 6 and drain region 8, A channel region 10 is formed therein. The surfaces of the semiconductor substrate 2, p-well 4, source region 6, and drain region 8 are covered with an oxide film 12, and a source electrode 14 and a drain electrode 16 are formed on the surfaces of the source region 6 and drain region 80. The oxide film 13 covering the channel region 10 is set thinner than other parts, and a gate electrode 18 is formed on the surface of this thin oxide film 13 by vapor deposition of aluminum or the like.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

従来、このような電界効果トランジスタでは、半導体基
板2の表面に、ソース領域6、ドレイン領域8およびチ
ャンネル領域10を形成する部分を考慮することなく、
無差別に不純物の拡散またはイオン注入を行ってpウェ
ル4を形成しているので、pウェル4の中心およびその
表面層が最も高い不純物濃度となり、その平面方向およ
び深さ方向に濃度勾配を呈する。すなわち、チャンネル
領域10の不純物濃度もソース領域6およびドレイン領
域8の近傍の不純物濃度も均一なプロファイルとなって
いる。
Conventionally, in such a field effect transistor, the portions on the surface of the semiconductor substrate 2 where the source region 6, drain region 8, and channel region 10 are formed are not considered.
Since the p-well 4 is formed by indiscriminate impurity diffusion or ion implantation, the center of the p-well 4 and its surface layer have the highest impurity concentration, and a concentration gradient is exhibited in the plane direction and depth direction. . That is, the impurity concentration of the channel region 10 and the impurity concentrations near the source region 6 and drain region 8 have a uniform profile.

このため、この種の電界効果トランジスタでは、周波数
特性、耐圧、闇値電圧vtnなどの電気的特性が固定し
、これらの特性を任意に設定することが困難であり、特
性の異なるデバイスを同一半導体基板上に任意に形成す
ることができなかった。
For this reason, in this type of field effect transistor, electrical characteristics such as frequency characteristics, breakdown voltage, and dark voltage vtn are fixed, making it difficult to set these characteristics arbitrarily, and devices with different characteristics can be integrated into the same semiconductor. It could not be formed arbitrarily on the substrate.

また、従来のものは、チャンネル領域10の不純物濃度
が一様であるため、半導体装置が双方向性となり、方向
性を設定することができなかった。
Furthermore, in the conventional device, since the impurity concentration in the channel region 10 is uniform, the semiconductor device becomes bidirectional, and the directionality cannot be set.

そこで、この発明は、周波数特性、耐圧、闇値電圧VT
Hなどの電気的特性が任意に設定でき、しかも、方向性
を持たせた半導体装置を提供しようとするものである。
Therefore, this invention provides frequency characteristics, breakdown voltage, dark value voltage VT
The present invention aims to provide a semiconductor device in which electrical characteristics such as H can be arbitrarily set and which has directionality.

〔問題点を解決するための手段〕 この発明を第1図および第2図に示す実施例を参照して
説明する。
[Means for Solving the Problems] The present invention will be described with reference to the embodiments shown in FIGS. 1 and 2.

すなわち、−導電型の半導体基板20に設置した反対導
電型の導電領域(pウェル22)に、ソース領域26お
よびドレイン領域28が設置されている。これらソース
領域26およびドレイン領域28の間には、チャンネル
領域24が形成され、このチャンネル領域24には、ゲ
ート電極38が臨ませられている。
That is, a source region 26 and a drain region 28 are provided in a conductive region (p well 22) of an opposite conductivity type provided in a semiconductor substrate 20 of a -conductivity type. A channel region 24 is formed between the source region 26 and the drain region 28, and a gate electrode 38 faces the channel region 24.

′このような半導体装置において、前記チャンネル領域
24の不純物濃度に勾配を持たせ、不純物濃度の低い部
分22aとその高い部分22bが形成されている。
'In such a semiconductor device, the impurity concentration of the channel region 24 has a gradient, and a region 22a with a low impurity concentration and a region 22b with a high impurity concentration are formed.

〔作 用〕[For production]

このような構成によって、チャンネル領域24の不純物
濃度に勾配を持たせ、その不純物を分布させることによ
り、その不純物濃度分布に応じてドリフト効果が生じて
周波数特性および耐圧が改善されるとともに、方向性を
生じる。
With such a configuration, the impurity concentration in the channel region 24 has a gradient and the impurities are distributed, thereby producing a drift effect according to the impurity concentration distribution, improving the frequency characteristics and breakdown voltage, and improving the directionality. occurs.

〔実施例〕〔Example〕

以下、この発明の半導体装置の実施例を図面を参照して
詳細に説明する。
Embodiments of the semiconductor device of the present invention will be described in detail below with reference to the drawings.

第1図および第2図は、この発明の半導体装置の実施例
を示し、第1図はその平面構造、第2図はその■−■線
に沿う断面を表している。
1 and 2 show an embodiment of the semiconductor device of the present invention, with FIG. 1 showing its planar structure, and FIG. 2 showing its cross section along the line ■-■.

第1図および第2図において、N型シリコンなどの一導
電型の半導体基板20に反対導電型の導電領域としての
pウェル22が二方向から形成されている。このpウェ
ル22のほぼ中心領域の不純物濃度が低い部分22aと
、不純物濃度が高い部分22bとに跨ってチャンネル領
域24となるように、pウェル22とは反対導電型のソ
ース領域26およびドレイン領域28が形成されている
1 and 2, a p-well 22 as a conductive region of an opposite conductivity type is formed from two directions on a semiconductor substrate 20 of one conductivity type such as N-type silicon. A source region 26 and a drain region of a conductivity type opposite to that of the p-well 22 are formed so that the channel region 24 spans a region 22a with a low impurity concentration and a region 22b with a high impurity concentration in the almost central region of the p-well 22. 28 is formed.

この実施例では、チャンネル領域24の中央部に ′p
ルウエル2の一方からの周縁部が置かれており、チャン
ネル領域24を中心にして不純物濃度が変化している。
In this embodiment, 'p' is located in the center of the channel region 24.
A peripheral portion from one side of the well 2 is placed, and the impurity concentration changes around the channel region 24.

半導体基板20、pウェル22、ソース領域26および
ドレイン領域28の表面は、酸化膜30で覆われている
とともに、ソース領域26およびドレイン領域28の表
面にはソース電極32、ドレイン電極34が形成されて
いる。
The surfaces of the semiconductor substrate 20, p-well 22, source region 26, and drain region 28 are covered with an oxide film 30, and a source electrode 32 and a drain electrode 34 are formed on the surfaces of the source region 26 and drain region 28. ing.

そして、チャンネル領域24を覆う酸化膜36は、他の
部分より薄く設定され、その表面にはアルミニウムなど
の蒸着によってゲート電極38が形成されている。
The oxide film 36 covering the channel region 24 is set thinner than other parts, and a gate electrode 38 is formed on its surface by vapor deposition of aluminum or the like.

このように、pウェル22を構成する導電領域の不純物
濃度の分布が段階的に変化する領域をチャンネル領域2
4に設定すれば、それに応じたドリフト効果が得られ、
周波数特性、ダイナミック耐圧などの電気的特性の改善
に加えて、従来の双方向性から一方向性の半導体装置と
して構成される。
In this way, the channel region 2 is a region where the impurity concentration distribution of the conductive region constituting the p-well 22 changes stepwise.
If you set it to 4, you can get a corresponding drift effect,
In addition to improving electrical characteristics such as frequency characteristics and dynamic breakdown voltage, the device is configured as a unidirectional semiconductor device instead of the conventional bidirectional one.

次に、この発明の半導体装置の製造方法を第3図ないし
第5図を参照して説明する。
Next, a method of manufacturing a semiconductor device according to the present invention will be explained with reference to FIGS. 3 to 5.

すなわち、この実施例は、pウェル22を不純物の拡散
によって形成する場合を示しており、第3図に示すよう
に、半導体基板20の表面にレジスト膜40を形成して
その表面を覆うとともに、レジスト膜40に選択的に不
純物拡散用の開口42を形成する。この場合、チャンネ
ル領域となる部分は、レジスト膜40で覆い、その周辺
部に開口42を形成し、その間口42から半導体基板2
0の表面層にボロンなどの不純物原子を拡散する。
That is, this embodiment shows a case where the p-well 22 is formed by diffusion of impurities, and as shown in FIG. 3, a resist film 40 is formed on the surface of the semiconductor substrate 20 to cover the surface. An opening 42 for impurity diffusion is selectively formed in the resist film 40. In this case, the portion that will become the channel region is covered with a resist film 40, an opening 42 is formed around the resist film 40, and the semiconductor substrate 2 is opened from the opening 42.
Impurity atoms such as boron are diffused into the surface layer of 0.

不純物の拡散状態は、第4図に示すように、開口42か
ら遠ざかるに従って不純物濃度が低下する。この場合、
pウェル22の周縁部は両側の開口42から拡散される
不純物同士が重なるが、開口42から遠くなるに従って
不純物濃度が低下するので、開口42の直下より低下し
たものとなるとともに、不純物の拡散量および開口42
の位置によってチャンネル領域となる部分の不純物濃度
を制御することができる。
Regarding the diffusion state of impurities, as shown in FIG. 4, the impurity concentration decreases as the distance from the opening 42 increases. in this case,
At the peripheral edge of the p-well 22, the impurities diffused from the openings 42 on both sides overlap, but the impurity concentration decreases as the distance from the opening 42 increases, so that it is lower than directly below the opening 42, and the amount of impurity diffused is and opening 42
The impurity concentration of the portion that becomes the channel region can be controlled by the position of the channel region.

このようにpウェル22を局部的に不純物濃度を制御し
て形成した後、pウェル22には、第5図に示すように
、特定の不純物濃度が得られている領域がチャンネル領
域24となるように、ソース領域26およびドレイン領
域28を通常の製造工程に従って設置する。
After the p-well 22 is formed by controlling the impurity concentration locally in this way, the region of the p-well 22 where a specific impurity concentration is obtained becomes the channel region 24, as shown in FIG. As such, source region 26 and drain region 28 are formed according to conventional manufacturing processes.

そして、半導体基板20、pウェル22、ソース領域2
6およびドレイン領域28の表面に形成された酸化膜3
0のソース領域26およびドレイン領域28にそれぞれ
ソース電極32、ドレイン電極34を形成するとともに
、チャンネル領域  。
Then, a semiconductor substrate 20, a p-well 22, a source region 2
6 and the oxide film 3 formed on the surface of the drain region 28
A source electrode 32 and a drain electrode 34 are formed in the source region 26 and drain region 28 of No. 0, respectively, and a channel region is formed.

24を覆う酸化膜36の表面にゲート電極38を形成し
、第1図および第2図に示す半導体装置が得られる。
A gate electrode 38 is formed on the surface of the oxide film 36 covering the oxide film 24, and the semiconductor device shown in FIGS. 1 and 2 is obtained.

この半導体装置では、pウェル22のチャンネル領域2
4に設定される部分の不純物濃度が任意に制御でき、ま
た、その制御は、同一の半導体基板上の所望の位置で部
分的に行うことができ、周波数特性、闇値、耐圧などの
電気的特性が異なるものを同時に得ることができる。
In this semiconductor device, the channel region 2 of the p-well 22
The impurity concentration of the portion set to 4 can be arbitrarily controlled, and the control can be performed partially at a desired position on the same semiconductor substrate, and electrical characteristics such as frequency characteristics, dark value, and breakdown voltage can be controlled. Products with different characteristics can be obtained at the same time.

なお、この実施例ではpウェル22を不純物拡散によっ
て形成したが、pウェル22は、イオン注入によって形
成してもよい。
In this embodiment, the p-well 22 was formed by impurity diffusion, but the p-well 22 may also be formed by ion implantation.

また、実施例では、N型の半導体基板にpウェルを形成
した場合について説明したが、この発明は、P型の半導
体基板にnウェルを形成する場合にも同様に適用できる
Further, in the embodiment, a case has been described in which a p-well is formed in an N-type semiconductor substrate, but the present invention can be similarly applied to a case in which an n-well is formed in a P-type semiconductor substrate.

〔発明の効果〕〔Effect of the invention〕

以上説明したように、この発明によれば、チャンネル領
域の不純物濃度分布を段階的に異ならせたので、ドリフ
ト効果が得られ、周波数特性、耐圧などの電気的特性が
改善できるとともに、方向性を設定でき、また、同一半
導体基板上で閾値、周波数特性、耐圧などの電気的特性
の異なるものを構成できる。
As explained above, according to the present invention, since the impurity concentration distribution in the channel region is varied in stages, a drift effect can be obtained, and electrical characteristics such as frequency characteristics and breakdown voltage can be improved, and directionality can be improved. It is also possible to configure devices with different electrical characteristics such as threshold values, frequency characteristics, and breakdown voltages on the same semiconductor substrate.

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

第1図はこの発明の半導体装置の実施例の平面構造を示
す説明図、第2図は第1図のn−n線に沿う断面図、第
3図は半導体基板に設置したレジスト膜およびその開口
を示す平面図、第4図は不純物拡散の状況を示す断面図
、第5図は不純物拡散の他の実施例を示す断面図、第6
図は一般的な電界効果トランジスタの電極配置を示す平
面図、第7図は第6図の■−■線に沿う断面図である。 20・・・半導体基板、22・・・導電領域としてのp
ウェル、22a・・・不純物濃度の低い部分、22b・
・・不純物濃度の高い部分、24・・・チャンネル領域
、26・・・ソース領域、28・・・ドレイン領域、3
8・・・ゲート電極。 113図 $4因 第5図
FIG. 1 is an explanatory diagram showing a planar structure of an embodiment of a semiconductor device of the present invention, FIG. 2 is a cross-sectional view taken along the line nn in FIG. 1, and FIG. 3 shows a resist film installed on a semiconductor substrate and its FIG. 4 is a plan view showing the opening, FIG. 4 is a cross-sectional view showing the situation of impurity diffusion, FIG. 5 is a cross-sectional view showing another example of impurity diffusion, and FIG.
The figure is a plan view showing the electrode arrangement of a general field effect transistor, and FIG. 7 is a cross-sectional view taken along the line ■--■ in FIG. 6. 20...Semiconductor substrate, 22...P as a conductive region
Well, 22a... portion with low impurity concentration, 22b...
... portion with high impurity concentration, 24 ... channel region, 26 ... source region, 28 ... drain region, 3
8...Gate electrode. 113 Figure $4 Cause Figure 5

Claims (1)

【特許請求の範囲】[Claims] 一導電型の半導体基板に設置した反対導電型の導電領域
に、ソース領域およびドレイン領域を設置し、これらソ
ース領域およびドレイン領域の間に形成されたチャンネ
ル領域にゲートを臨ませてなる半導体装置において、前
記チャンネル領域の不純物濃度に勾配を持たせたことを
特徴とする半導体装置。
In a semiconductor device in which a source region and a drain region are provided in a conductive region of an opposite conductivity type provided on a semiconductor substrate of one conductivity type, and a gate is made to face a channel region formed between the source region and the drain region. . A semiconductor device characterized in that the impurity concentration of the channel region has a gradient.
JP60070365A 1985-04-03 1985-04-03 Semiconductor device Granted JPS61229366A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP60070365A JPS61229366A (en) 1985-04-03 1985-04-03 Semiconductor device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60070365A JPS61229366A (en) 1985-04-03 1985-04-03 Semiconductor device

Publications (2)

Publication Number Publication Date
JPS61229366A true JPS61229366A (en) 1986-10-13
JPH0550863B2 JPH0550863B2 (en) 1993-07-30

Family

ID=13429336

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60070365A Granted JPS61229366A (en) 1985-04-03 1985-04-03 Semiconductor device

Country Status (1)

Country Link
JP (1) JPS61229366A (en)

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS4975288A (en) * 1972-11-22 1974-07-19
JPS549589A (en) * 1977-05-05 1979-01-24 Centre Electron Horloger Ic using complementary mos transistor

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS4975288A (en) * 1972-11-22 1974-07-19
JPS549589A (en) * 1977-05-05 1979-01-24 Centre Electron Horloger Ic using complementary mos transistor

Also Published As

Publication number Publication date
JPH0550863B2 (en) 1993-07-30

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