JPS63252480A - Vertical mos field-effect transistor - Google Patents
Vertical mos field-effect transistorInfo
- Publication number
- JPS63252480A JPS63252480A JP62089104A JP8910487A JPS63252480A JP S63252480 A JPS63252480 A JP S63252480A JP 62089104 A JP62089104 A JP 62089104A JP 8910487 A JP8910487 A JP 8910487A JP S63252480 A JPS63252480 A JP S63252480A
- Authority
- JP
- Japan
- Prior art keywords
- regions
- region
- effect transistor
- vertical mos
- channel
- 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
- 230000005669 field effect Effects 0.000 title claims description 13
- 239000000758 substrate Substances 0.000 claims abstract description 9
- 239000011159 matrix material Substances 0.000 claims abstract description 4
- 230000005684 electric field Effects 0.000 claims description 16
- 230000015556 catabolic process Effects 0.000 abstract description 5
- 239000010410 layer Substances 0.000 description 7
- 238000010586 diagram Methods 0.000 description 1
- 239000002356 single layer Substances 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L29/00—Semiconductor devices adapted for rectifying, amplifying, oscillating or switching, or capacitors or resistors with at least one potential-jump barrier or surface barrier, e.g. PN junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof ; Multistep manufacturing processes therefor
- H01L29/66—Types of semiconductor device ; Multistep manufacturing processes therefor
- H01L29/68—Types of semiconductor device ; Multistep manufacturing processes therefor controllable by only the electric current supplied, or only the electric potential applied, to an electrode which does not carry the current to be rectified, amplified or switched
- H01L29/76—Unipolar devices, e.g. field effect transistors
- H01L29/772—Field effect transistors
- H01L29/78—Field effect transistors with field effect produced by an insulated gate
- H01L29/7801—DMOS transistors, i.e. MISFETs with a channel accommodating body or base region adjoining a drain drift region
- H01L29/7802—Vertical DMOS transistors, i.e. VDMOS transistors
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L29/00—Semiconductor devices adapted for rectifying, amplifying, oscillating or switching, or capacitors or resistors with at least one potential-jump barrier or surface barrier, e.g. PN junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof ; Multistep manufacturing processes therefor
- H01L29/02—Semiconductor bodies ; Multistep manufacturing processes therefor
- H01L29/06—Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their shape; characterised by the shapes, relative sizes, or dispositions of the semiconductor regions ; characterised by the concentration or distribution of impurities within semiconductor regions
- H01L29/0603—Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their shape; characterised by the shapes, relative sizes, or dispositions of the semiconductor regions ; characterised by the concentration or distribution of impurities within semiconductor regions characterised by particular constructional design considerations, e.g. for preventing surface leakage, for controlling electric field concentration or for internal isolations regions
- H01L29/0607—Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their shape; characterised by the shapes, relative sizes, or dispositions of the semiconductor regions ; characterised by the concentration or distribution of impurities within semiconductor regions characterised by particular constructional design considerations, e.g. for preventing surface leakage, for controlling electric field concentration or for internal isolations regions for preventing surface leakage or controlling electric field concentration
- H01L29/0611—Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their shape; characterised by the shapes, relative sizes, or dispositions of the semiconductor regions ; characterised by the concentration or distribution of impurities within semiconductor regions characterised by particular constructional design considerations, e.g. for preventing surface leakage, for controlling electric field concentration or for internal isolations regions for preventing surface leakage or controlling electric field concentration for increasing or controlling the breakdown voltage of reverse biased devices
- H01L29/0615—Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their shape; characterised by the shapes, relative sizes, or dispositions of the semiconductor regions ; characterised by the concentration or distribution of impurities within semiconductor regions characterised by particular constructional design considerations, e.g. for preventing surface leakage, for controlling electric field concentration or for internal isolations regions for preventing surface leakage or controlling electric field concentration for increasing or controlling the breakdown voltage of reverse biased devices by the doping profile or the shape or the arrangement of the PN junction, or with supplementary regions, e.g. junction termination extension [JTE]
- H01L29/0619—Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their shape; characterised by the shapes, relative sizes, or dispositions of the semiconductor regions ; characterised by the concentration or distribution of impurities within semiconductor regions characterised by particular constructional design considerations, e.g. for preventing surface leakage, for controlling electric field concentration or for internal isolations regions for preventing surface leakage or controlling electric field concentration for increasing or controlling the breakdown voltage of reverse biased devices by the doping profile or the shape or the arrangement of the PN junction, or with supplementary regions, e.g. junction termination extension [JTE] with a supplementary region doped oppositely to or in rectifying contact with the semiconductor containing or contacting region, e.g. guard rings with PN or Schottky junction
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L29/00—Semiconductor devices adapted for rectifying, amplifying, oscillating or switching, or capacitors or resistors with at least one potential-jump barrier or surface barrier, e.g. PN junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof ; Multistep manufacturing processes therefor
- H01L29/02—Semiconductor bodies ; Multistep manufacturing processes therefor
- H01L29/06—Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their shape; characterised by the shapes, relative sizes, or dispositions of the semiconductor regions ; characterised by the concentration or distribution of impurities within semiconductor regions
- H01L29/0684—Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their shape; characterised by the shapes, relative sizes, or dispositions of the semiconductor regions ; characterised by the concentration or distribution of impurities within semiconductor regions characterised by the shape, relative sizes or dispositions of the semiconductor regions or junctions between the regions
- H01L29/0692—Surface layout
- H01L29/0696—Surface layout of cellular field-effect devices, e.g. multicellular DMOS transistors or IGBTs
Landscapes
- Engineering & Computer Science (AREA)
- Microelectronics & Electronic Packaging (AREA)
- Power Engineering (AREA)
- Physics & Mathematics (AREA)
- Ceramic Engineering (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- General Physics & Mathematics (AREA)
- Computer Hardware Design (AREA)
- Insulated Gate Type Field-Effect Transistor (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
この発明は、縦形モス電界効果トランジスタ(縦形MO
S FET )に関するものである。[Detailed Description of the Invention] [Industrial Application Field] This invention relates to a vertical MOS field effect transistor (vertical MOSFET).
SFET).
第2図は従来の縦形MO5FETを示す。図において、
1はn形(第1導電形)基板、2はml記基板1の一ノ
jの主面に形成したnゝドレン領域、3は前記基板の他
方の主面に7トリクス状に形成したp(第2導電形)チ
ャンネル領域、4はこのPチャンネル領域に形成された
nソース@域、5は隣り合うpチャンネルの間の主面と
nソース領域の一部を覆うように形成した酸化膜、6は
この酸化膜の上に形成したゲート電極、7はこのゲート
電極を覆うように形成した絶縁膜、8は前記nソース領
域5に取り付けたソース電極である。FIG. 2 shows a conventional vertical MO5FET. In the figure,
1 is an n-type (first conductivity type) substrate, 2 is an n drain region formed on one main surface of the substrate 1, and 3 is a p region formed in a 7-trix shape on the other main surface of the substrate. (Second conductivity type) channel region, 4 is an n source @ region formed in this P channel region, 5 is an oxide film formed to cover the main surface between adjacent p channels and a part of the n source region , 6 is a gate electrode formed on this oxide film, 7 is an insulating film formed to cover this gate electrode, and 8 is a source electrode attached to the n source region 5.
従来の縦形モス電界効果トランジスタは上記のように構
成したから、縦形モス電界効果トランジスタのしきい値
より高い正電位をゲート電極6に印加すると、Pチャン
ネル領域3の表面部分がnチャンネルに反転し、電流は
第2図(h)。Since the conventional vertical MOS field effect transistor is constructed as described above, when a positive potential higher than the threshold of the vertical MOS field effect transistor is applied to the gate electrode 6, the surface portion of the P channel region 3 is inverted to an n channel. , the current is shown in Figure 2 (h).
(C)の破線で示すように、n+ドレン領域2から、ま
ず、ゲート電極6に向って縦方向に流れ、ついで、隣り
合うpチャンネル領域3間の領域で向きを変え、前記n
チャンネルを通ってnソース領域5に至る。As shown by the broken line in (C), the flow first flows vertically from the n+ drain region 2 toward the gate electrode 6, then changes direction in the region between adjacent p channel regions 3, and the n
It passes through the channel and reaches the n source region 5.
第2図(b)に、ゲート電極に印加した電位がしきい値
に達しない時、すなわちOFF状憇に発生ずる空乏層を
一点鎖線で示す。In FIG. 2(b), a chain line indicates a depletion layer that occurs when the potential applied to the gate electrode does not reach the threshold value, that is, in the OFF state.
従来の縦形モス電界効果トランジスタは、第2図(a)
に示すように、複数のPチャンネル領域3をマトリクス
状に形成したから、第2図(b)のA2〜A2線断面図
に示す隣り合うpチャンネル領域3間の距離と、第2図
(e)の82−82線断面図に示す隣り合うpチャンネ
ル領域3間の距離との比は、t:f了で、pチャンネル
領域3間の距離が異なるため、OFF状憇におけるPチ
ャンネル領域3間での空乏層の拡がりは、一定にならな
い。その結果、第2図(C)に一点鎖線で示すように、
各Pチャンネル領域3か゛ら等距離の位置に、電界が集
中し、その電界が集中する箇所では、なだれ降伏電圧か
低くなるという問題点があった。A conventional vertical MOS field effect transistor is shown in Fig. 2(a).
Since a plurality of P channel regions 3 are formed in a matrix as shown in FIG. ) is the ratio of the distance between adjacent p-channel regions 3 shown in the 82-82 line cross-sectional view. The spread of the depletion layer in the region is not constant. As a result, as shown by the dashed line in Fig. 2(C),
There is a problem in that the electric field is concentrated at a position equidistant from each P channel region 3, and the avalanche breakdown voltage is low at the location where the electric field is concentrated.
この発明は、上記のような問題点を解決するためになさ
れたもので、高耐圧の縦形モス電界効果トランジスタを
得ることを目的とする。The present invention was made to solve the above-mentioned problems, and an object of the present invention is to obtain a vertical MOS field effect transistor with high breakdown voltage.
(問題点を解決するための手段〕
この発明に係る縦形モス電界効果トランジスタは、第1
導電形基板の一方の1簡に第1導電形のドレンを、他方
の主1n1にマトリックス状に配置したチャンネル領域
と、このチャンネル領域内に第1導電形のソースとを有
し、かつ、面記チャンネル間の基板表面にゲートを有す
る縦形モス電界効果トランジスタであって、電界が集中
する領域に、第2導電形の領域を設けたものである。(Means for Solving the Problems) The vertical MOS field effect transistor according to the present invention has a first
A conductive type substrate has a drain of the first conductive type in one main part thereof, a channel region arranged in a matrix in the other main part, and a source of the first conductive type in this channel region, and This vertical MOS field effect transistor has a gate on the substrate surface between the channels, and a region of the second conductivity type is provided in the region where the electric field is concentrated.
(作用)
この発明によって形成した第2導電形の領域は、電界が
集中する領域に、前記電界と逆方向に所定の電界を形成
し、空乏層の拡がりをほぼ一定にする。(Function) The region of the second conductivity type formed according to the present invention forms a predetermined electric field in the opposite direction to the electric field in the region where the electric field is concentrated, thereby making the spread of the depletion layer almost constant.
(実施例)
第1図はこの発明の−・実施例を示す。図において、1
〜8は第2図と同一部分を示す。10は第2導電形の領
域としての1層領域で、電界集中領域、すなわち、各p
チャンネル領域3から等距離の位置に形成してあり、前
記電界と逆方向に所定の電界を発生するものである。(Embodiment) FIG. 1 shows an embodiment of the present invention. In the figure, 1
8 show the same parts as in FIG. 10 is a single-layer region as a region of the second conductivity type, which is an electric field concentration region, that is, each p
It is formed at a position equidistant from the channel region 3, and generates a predetermined electric field in the opposite direction to the electric field.
この実施例の縦形モス電界効果トランジスタは、各pチ
ャンネル領域3から等距離の位置に9層領域10を形成
する構成にしたから、このpMIJ領域10近傍の電界
は、9層領域10が形成する電界により相殺され、第1
図(C)に一点鎖線で示すように、空乏層の拡がりはほ
ぼ一定になる。Since the vertical MOS field effect transistor of this embodiment has a structure in which the 9-layer region 10 is formed at a position equidistant from each p-channel region 3, the electric field near this pMIJ region 10 is generated by the 9-layer region 10. canceled by the electric field, the first
As shown by the dashed line in the figure (C), the spread of the depletion layer becomes almost constant.
(発明の効果〕
以上説明したように、この発明によれば、電界集中領域
に、前記電界と逆方向に所定の電界を発生する構成にし
たので、空乏層の拡がりがほぼ一定になり、高耐圧の縦
形モス電界効果トランジスタを得ることができるいう効
果がある。(Effects of the Invention) As explained above, according to the present invention, since a predetermined electric field is generated in the electric field concentration region in the opposite direction to the electric field, the spread of the depletion layer becomes almost constant and the This has the advantage that a vertical MOS field effect transistor with high breakdown voltage can be obtained.
第1Mはこの発明の一実施例を示す図で、第1図(a)
は縦形モス電界効果トランジスタの一部破断乎面図、第
1図(b)は第1図(a)に示すA、−A、線断面図、
第1図(C)は第1図(a)に示すB、−B、線断面図
である。第2図は従来の縦形モス電界効果トランジスタ
を示す図で、第2図(a)は一部破断乎面図、第2図(
b)は第2図(a)に示すA2−A2線断面図、第2図
(C)は第2図(a)に示すB2−82線断面図である
。
図において、1は口形基板、2はn“トレン領域、3は
Pチャンネル領域、4はnソース領域、6はゲート電極
、10はpH領域である。
なお、図中、同一符号は同一または相当部分を示す。1M is a diagram showing an embodiment of the present invention, and FIG. 1(a)
is a partially cutaway view of a vertical MOS field effect transistor, FIG. 1(b) is a cross-sectional view taken along the line A, -A shown in FIG. 1(a),
FIG. 1(C) is a sectional view taken along the line B and -B shown in FIG. 1(a). Figure 2 shows a conventional vertical MOS field effect transistor; Figure 2(a) is a partially cutaway view;
b) is a sectional view taken along line A2-A2 shown in FIG. 2(a), and FIG. 2(C) is a sectional view taken along line B2-82 shown in FIG. 2(a). In the figure, 1 is a mouth-shaped substrate, 2 is an n-tren region, 3 is a P-channel region, 4 is an n-source region, 6 is a gate electrode, and 10 is a pH region. Show parts.
Claims (1)
他方の主面にマトリックス状に配置した第2導電形のチ
ャンネル領域と、このチャンネル領域内に第1導電形の
ソースとを有し、かつ、前記チャンネル間の基板表面に
ゲートを有する縦形モス電界効果トランジスタにおいて
、電界が集中する領域に、第2導電形の領域を備えたこ
とを特徴とする縦形モス電界効果トランジスタ。A drain of the first conductivity type is provided on one main surface of the first conductivity type substrate,
A vertical MOS electric field having a second conductivity type channel region arranged in a matrix on the other main surface, a first conductivity type source within the channel region, and a gate on the substrate surface between the channels. A vertical MOS field effect transistor characterized in that the effect transistor includes a region of a second conductivity type in a region where an electric field is concentrated.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP62089104A JPS63252480A (en) | 1987-04-09 | 1987-04-09 | Vertical mos field-effect transistor |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP62089104A JPS63252480A (en) | 1987-04-09 | 1987-04-09 | Vertical mos field-effect transistor |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS63252480A true JPS63252480A (en) | 1988-10-19 |
Family
ID=13961580
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP62089104A Pending JPS63252480A (en) | 1987-04-09 | 1987-04-09 | Vertical mos field-effect transistor |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS63252480A (en) |
Cited By (13)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH02292868A (en) * | 1989-05-01 | 1990-12-04 | Nippon Inter Electronics Corp | Field-effect transistor |
JPH03230574A (en) * | 1990-02-06 | 1991-10-14 | Matsushita Electron Corp | Semiconductor device |
US5136349A (en) * | 1989-08-30 | 1992-08-04 | Siliconix Incorporated | Closed cell transistor with built-in voltage clamp |
US5155574A (en) * | 1990-03-20 | 1992-10-13 | Mitsubishi Denki Kabushiki Kaisha | Semiconductor device |
US5420450A (en) * | 1992-09-10 | 1995-05-30 | Kabushiki Kaisha Toshiba | Semiconductor device having stable breakdown voltage in wiring area |
JP2005136166A (en) * | 2003-10-30 | 2005-05-26 | Matsushita Electric Ind Co Ltd | Vertical mosfet |
JP2006019553A (en) * | 2004-07-02 | 2006-01-19 | Matsushita Electric Ind Co Ltd | Vertical semiconductor device |
US7833863B1 (en) | 2003-12-02 | 2010-11-16 | Vishay-Siliconix | Method of manufacturing a closed cell trench MOSFET |
CN102244100A (en) * | 2011-06-28 | 2011-11-16 | 上海宏力半导体制造有限公司 | MOS (metal oxide semiconductor) power semiconductor device |
US8183629B2 (en) | 2004-05-13 | 2012-05-22 | Vishay-Siliconix | Stacked trench metal-oxide-semiconductor field effect transistor device |
US8368126B2 (en) | 2007-04-19 | 2013-02-05 | Vishay-Siliconix | Trench metal oxide semiconductor with recessed trench material and remote contacts |
US8471390B2 (en) | 2006-05-12 | 2013-06-25 | Vishay-Siliconix | Power MOSFET contact metallization |
US9306056B2 (en) | 2009-10-30 | 2016-04-05 | Vishay-Siliconix | Semiconductor device with trench-like feed-throughs |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS607764A (en) * | 1983-06-13 | 1985-01-16 | エヌ・ベ−・フイリツプス・フル−イランペンフアブリケン | Semiconductor device |
-
1987
- 1987-04-09 JP JP62089104A patent/JPS63252480A/en active Pending
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS607764A (en) * | 1983-06-13 | 1985-01-16 | エヌ・ベ−・フイリツプス・フル−イランペンフアブリケン | Semiconductor device |
Cited By (16)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH02292868A (en) * | 1989-05-01 | 1990-12-04 | Nippon Inter Electronics Corp | Field-effect transistor |
US5136349A (en) * | 1989-08-30 | 1992-08-04 | Siliconix Incorporated | Closed cell transistor with built-in voltage clamp |
JPH03230574A (en) * | 1990-02-06 | 1991-10-14 | Matsushita Electron Corp | Semiconductor device |
US5155574A (en) * | 1990-03-20 | 1992-10-13 | Mitsubishi Denki Kabushiki Kaisha | Semiconductor device |
US5420450A (en) * | 1992-09-10 | 1995-05-30 | Kabushiki Kaisha Toshiba | Semiconductor device having stable breakdown voltage in wiring area |
JP2005136166A (en) * | 2003-10-30 | 2005-05-26 | Matsushita Electric Ind Co Ltd | Vertical mosfet |
US7833863B1 (en) | 2003-12-02 | 2010-11-16 | Vishay-Siliconix | Method of manufacturing a closed cell trench MOSFET |
US8183629B2 (en) | 2004-05-13 | 2012-05-22 | Vishay-Siliconix | Stacked trench metal-oxide-semiconductor field effect transistor device |
JP2006019553A (en) * | 2004-07-02 | 2006-01-19 | Matsushita Electric Ind Co Ltd | Vertical semiconductor device |
US8697571B2 (en) | 2006-05-12 | 2014-04-15 | Vishay-Siliconix | Power MOSFET contact metallization |
US8471390B2 (en) | 2006-05-12 | 2013-06-25 | Vishay-Siliconix | Power MOSFET contact metallization |
US8368126B2 (en) | 2007-04-19 | 2013-02-05 | Vishay-Siliconix | Trench metal oxide semiconductor with recessed trench material and remote contacts |
US8883580B2 (en) | 2007-04-19 | 2014-11-11 | Vishay-Siliconix | Trench metal oxide semiconductor with recessed trench material and remote contacts |
US9306056B2 (en) | 2009-10-30 | 2016-04-05 | Vishay-Siliconix | Semiconductor device with trench-like feed-throughs |
US10032901B2 (en) | 2009-10-30 | 2018-07-24 | Vishay-Siliconix | Semiconductor device with trench-like feed-throughs |
CN102244100A (en) * | 2011-06-28 | 2011-11-16 | 上海宏力半导体制造有限公司 | MOS (metal oxide semiconductor) power semiconductor device |
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