Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JPH0821714B2 - Insulated gate field effect transistor - Google Patents
[go: Go Back, main page]

JPH0821714B2 - Insulated gate field effect transistor - Google Patents

Insulated gate field effect transistor

Info

Publication number
JPH0821714B2
JPH0821714B2 JP63308043A JP30804388A JPH0821714B2 JP H0821714 B2 JPH0821714 B2 JP H0821714B2 JP 63308043 A JP63308043 A JP 63308043A JP 30804388 A JP30804388 A JP 30804388A JP H0821714 B2 JPH0821714 B2 JP H0821714B2
Authority
JP
Japan
Prior art keywords
region
cell
field effect
effect transistor
drain
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
Application number
JP63308043A
Other languages
Japanese (ja)
Other versions
JPH02154468A (en
Inventor
隆美 寺嶋
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.)
Sanken Electric Co Ltd
Original Assignee
Sanken Electric 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 Sanken Electric Co Ltd filed Critical Sanken Electric Co Ltd
Priority to JP63308043A priority Critical patent/JPH0821714B2/en
Publication of JPH02154468A publication Critical patent/JPH02154468A/en
Publication of JPH0821714B2 publication Critical patent/JPH0821714B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D30/00Field-effect transistors [FET]
    • H10D30/60Insulated-gate field-effect transistors [IGFET]
    • H10D30/64Double-diffused metal-oxide semiconductor [DMOS] FETs
    • H10D30/66Vertical DMOS [VDMOS] FETs
    • 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
    • H10D62/124Shapes, relative sizes or dispositions of the regions of semiconductor bodies or of junctions between the regions
    • H10D62/126Top-view geometrical layouts of the regions or the junctions
    • H10D62/127Top-view geometrical layouts of the regions or the junctions of cellular field-effect devices, e.g. multicellular DMOS transistors or IGBTs
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D30/00Field-effect transistors [FET]
    • H10D30/60Insulated-gate field-effect transistors [IGFET]
    • H10D30/64Double-diffused metal-oxide semiconductor [DMOS] FETs
    • H10D30/66Vertical DMOS [VDMOS] FETs
    • H10D30/662Vertical DMOS [VDMOS] FETs having a drift region having a doping concentration that is higher between adjacent body regions relative to other parts of the drift region
    • 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
    • H10D62/13Semiconductor regions connected to electrodes carrying current to be rectified, amplified or switched, e.g. source or drain regions
    • H10D62/149Source or drain regions of field-effect devices
    • H10D62/151Source or drain regions of field-effect devices of IGFETs 
    • H10D62/156Drain regions of DMOS transistors
    • H10D62/157Impurity concentrations or distributions

Landscapes

  • Insulated Gate Type Field-Effect Transistor (AREA)

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明はマルチセルタイプの絶縁ゲート電界効果トラン
ジスタの高耐圧化構造に関するものである。
The present invention relates to a high breakdown voltage structure of a multi-cell type insulated gate field effect transistor.

〔従来の技術〕[Conventional technology]

今日、電力用絶縁ゲート電界効果トランジスタは高周波
スイツチング電源を始めとして広い分野で使用されてい
る。従来のこの種の電界効果トランジスタは第5図に示
すように出発母材となるn+形領域1aとその上面にエピタ
キシヤル成長させて形成したn形領域1bとから成るドレ
イン領域1と、n形領域の表面に露出する部分を有して
n形領域に包囲されたp形領域から成るバルク領域2
と、バルク領域2の表面に露出する部分を有してバルク
領域2に包囲された環状のn+形領域から成るソース領域
3と、バルク領域2の表面側に絶縁膜4を介して形成さ
れたゲート電極5と、バルク領域2及びソース領域3に
接触するソース電極(第1の主電極)6と、ドレイン領
域1に接触するドレイン電極(第2の主電極)7とを有
する。なお、ゲート電極5とソース電極6とは絶縁膜10
を介して電気的に絶縁されている。このように構成され
た電界効果トランジスタにおいては、ソース電極6とド
レイン電極7との間にドレイン電極7側を正とする電圧
VDSを印加し、さらにゲート電極5にソース電極6に対
して正のオン電圧を印加すると、ゲート電極5の下のバ
ルク領域6がn形に反転してチヤンネルが形成され、ド
レイン領域1からソース領域3へと主として縦方向にド
レイン電流IDが流れる。ここで、上記の電圧VDSが増加
すると、第5図に模式的に示すように空乏層8が拡が
る。空乏層8はブレークダウンが生じるまでこの電圧を
支える。なお空乏層8は、ドレイン領域1とセル領域9
(バルク領域2)との間のpn接合から伸びる空乏層とゲ
ート電極5の電界効果によりゲート電極下に拡がる空乏
層とが一体化したものである。
Insulated gate field effect transistors for electric power are used in a wide range of fields such as high frequency switching power supplies. As shown in FIG. 5, a conventional field effect transistor of this type has a drain region 1 consisting of an n + type region 1a as a starting base material and an n type region 1b formed by epitaxial growth on its upper surface, Bulk region 2 comprising a p-type region surrounded by an n-type region and having a portion exposed on the surface of the shape region 2
A source region 3 formed of an annular n + -type region surrounded by the bulk region 2 and having a portion exposed on the surface of the bulk region 2, and a source region 3 formed on the surface side of the bulk region 2 via an insulating film 4. A gate electrode 5, a source electrode (first main electrode) 6 in contact with the bulk region 2 and the source region 3, and a drain electrode (second main electrode) 7 in contact with the drain region 1. The gate electrode 5 and the source electrode 6 are formed of an insulating film 10
It is electrically insulated through. In the field effect transistor configured as described above, a voltage between the source electrode 6 and the drain electrode 7 with the drain electrode 7 side being positive is provided.
When V DS is applied and a positive on-voltage is applied to the gate electrode 5 with respect to the source electrode 6, the bulk region 6 under the gate electrode 5 is inverted into an n-type to form a channel, and the drain region 1 A drain current I D mainly flows in the vertical direction to the source region 3. Here, when the voltage V DS increases, the depletion layer 8 expands as schematically shown in FIG. Depletion layer 8 supports this voltage until breakdown occurs. The depletion layer 8 is formed in the drain region 1 and the cell region 9
The depletion layer extending from the pn junction with the (bulk region 2) and the depletion layer extending under the gate electrode due to the electric field effect of the gate electrode 5 are integrated.

〔発明が解決しようとする課題〕[Problems to be Solved by the Invention]

第5図の電界効果トランジスタは、第6図に示すよう
にソース領域3とそれを包囲するバルク領域2から成る
多数個の島状領域(以下、セル領域と称する)9がドレ
イン領域1に形成されているマルチセルタイプの電界効
果トランジスタとなつている。周知のように、セル領域
9の4つの角部は図示のように丸めてはあつても、直線
状の辺部に比べると電界集中が生じ易い。このため、高
耐圧化を図る上では不利である。
As shown in FIG. 6, in the field effect transistor of FIG. 5, a large number of island-shaped regions (hereinafter, referred to as cell regions) 9 including a source region 3 and a bulk region 2 surrounding the source region 3 are formed in the drain region 1. It is used as a multi-cell type field effect transistor. As is well known, even if the four corners of the cell region 9 are rounded as shown in the figure, the electric field concentration is more likely to occur as compared with the straight side portions. Therefore, it is disadvantageous in achieving high breakdown voltage.

そこで、本発明の目的は、オン抵抗が低く且つ耐圧が
高いマルチセルタイプの絶縁ゲート電界効果トランジス
タを提供することにある。
Therefore, it is an object of the present invention to provide a multi-cell type insulated gate field effect transistor having a low on-resistance and a high breakdown voltage.

[課題を解決するための手段] 上記目的を達成するための本発明は、実施例を示す図
面の符号を参照して説明すると、バルク領域2とこのバ
ルク領域2の中に形成されたソース領域3とから成るセ
ル領域9がドレイン領域1内に島状に複数個配置されて
いるマルチセルタイプの絶縁ゲート電界効果トランジス
タにおいて、前記複数個のセル領域は第1のセル領域と
前記第1のセル領域に対して互いに等しい間隔を有して
前記第1のセル領域の周囲に配置された複数の第2のセ
ル領域とを有し、前記第1及び第2のセル領域の平面形
状は略正四角形又は略正六角形であり、前記第1のセル
領域の互いに対向する複数の対の角部を結ぶ複数の仮想
直線の延長線上に前記第2のセル領域のそれぞれが配置
され、前記第2のセル領域の中心及び角部が前記仮想直
線の延長線上に位置し、前記第1のセル領域の角部とこ
れに隣り合う前記第2のセル領域の角部との間の距離が
前記第1のセル領域の辺部とこれに隣り合う前記第2の
セル領域の辺部との間の距離よりも小さく設定され、前
記ドレイン領域1は高不純物濃度の第1の領域(例えば
n+形領域)1aと前記第1の領域1aよりも不純物濃度が低
い第2の領域(例えばn形領域)1bと前記第2の領域1b
よりも不純物濃度が高い第3の領域(例えばn+形領域)
1cとを有し、前記第1の領域1aにドレイン電極7が接続
され、前記第2の領域1bは前記第1の領域1aに隣接して
いると共に前記バルク領域2と前記第1の領域1aとの間
に介在し且つエピタキシャル成長で形成され、前記第3
の領域1cは前記第1のセル領域と前記2のセル領域との
対向間に配置されていることを特徴とする絶縁ゲート電
界効果トランジスタに係わるものである。
[Means for Solving the Problems] The present invention for achieving the above object will be described with reference to the reference numerals of the drawings showing an embodiment. The bulk region 2 and a source region formed in the bulk region 2 will be described below. In a multi-cell type insulated gate field effect transistor in which a plurality of cell regions 9 composed of 3 are arranged in the drain region 1 in an island shape, the plurality of cell regions are the first cell region and the first cell region. A plurality of second cell regions that are arranged around the first cell region at equal intervals with respect to the region, and the planar shapes of the first and second cell regions are substantially positive. Each of the second cell regions is a quadrangle or a substantially regular hexagon, and each of the second cell regions is arranged on an extension line of a plurality of virtual straight lines that connect a plurality of corner portions of the first cell region that face each other. The center and corner of the cell area The distance between the corner of the first cell region and the corner of the second cell region adjacent to the corner of the first cell region, which is located on the extension line of the virtual straight line, is the same as the side of the first cell region. Is set smaller than the distance between the sides of the second cell region adjacent to each other, and the drain region 1 has a high impurity concentration in the first region (for example,
n + -type region) 1a, a second region (for example, n-type region) 1b having an impurity concentration lower than that of the first region 1a, and the second region 1b
Third region with a higher impurity concentration than that (eg n + type region)
1c, the drain electrode 7 is connected to the first region 1a, the second region 1b is adjacent to the first region 1a, and the bulk region 2 and the first region 1a. And is formed by epitaxial growth.
The region 1c is related to the insulated gate field effect transistor, which is arranged between the first cell region and the second cell region facing each other.

[発明の作用及び効果] 本発明の絶縁ゲート電界効果トランジスタでは、第1
のセル領域と第2のセル領域の対向間のドレイン領域の
上部に高不純物濃度の領域1cが形成されているためオン
抵抗の減少が図られている。このようにドレイン領域の
上部に高不純物濃度の第3の領域を形成すると、セル領
域の角部の耐圧が低くなり易いが、本発明では第1のセ
ル領域の互いに対向する対の角部を結ぶ仮想直線の延長
線上に第2のセル領域の中心及び対の角部を配置し、第
1及び第2のセル領域の角部の相互間の距離を辺部の相
互間の距離よりも小さく設定したので、第1及び第2の
セル領域の角部の間のドレイン領域が辺部間のドレイン
領域に先立つて空乏層に満たされる。このため、電界集
中の起り易い第1及び第2のセル領域の角部の降伏電圧
が上昇し、耐圧の低下が抑制される。また、第1及び第
2のセル領域の辺部の間の距離は角部の間の距離よりも
大きいので、辺部の間に比較的大面積のドレイン領域が
存在し、ここがドレイン電流の通路として有効に働く。
結果として、オン抵抗が小さく且つ高耐圧化した絶縁ゲ
ート電界効果トランジスタを提供できる。
[Operation and Effect of the Invention] In the insulated gate field effect transistor of the present invention, the first
Since the high impurity concentration region 1c is formed above the drain region between the cell region and the second cell region facing each other, the on-resistance is reduced. When the third region having a high impurity concentration is formed above the drain region as described above, the breakdown voltage of the corner portion of the cell region tends to be low. However, in the present invention, the pair of corner portions of the first cell region facing each other are formed. The center of the second cell region and the pair of corners are arranged on the extension of the connecting virtual straight line, and the distance between the corners of the first and second cell regions is smaller than the distance between the sides. Since it is set, the drain region between the corners of the first and second cell regions is filled with the depletion layer prior to the drain region between the sides. For this reason, the breakdown voltage at the corners of the first and second cell regions where electric field concentration is likely to occur increases and the breakdown voltage is suppressed from decreasing. In addition, since the distance between the sides of the first and second cell regions is larger than the distance between the corners, there is a relatively large drain region between the sides, which is the drain current. Effectively works as a passage.
As a result, it is possible to provide an insulated gate field effect transistor having a low on-resistance and a high breakdown voltage.

[実施例] 本発明の実施例に係わる絶縁ゲート電界効果トランジ
スタを第1図〜第3図に基づいて説明する。なお、第1
図〜第3図において、第5図及び第6図と実質的に同一
の部分には同一の符号を付してその説明を省略する。
[Embodiment] An insulated gate field effect transistor according to an embodiment of the present invention will be described with reference to FIGS. The first
In FIGS. 3 to 3, parts that are substantially the same as those in FIGS. 5 and 6 are given the same reference numerals, and description thereof will be omitted.

本実施例の絶縁ゲート電界効果トランジスタは従来例
と同様にソース領域3とそれを包囲するバルク領域2か
ら成るセル領域9がドレイン領域1内に島状に点在した
マルチセルタイプの絶縁ゲート電界効果トランジスタで
ある。なお、ソース領域3はバルク領域2内に環状に形
成されており、ソース領域3の内側の孔にはバルク領域
2が侵入している。セル領域9は第1図に示すように平
面形状が略正四角形となつており、それぞれ4つの角部
とそれら角部の間に形成された略直線状の4つの辺部と
を有している。角部は従来例と同様に電界集中を緩和す
るように円弧状に丸められている。
The insulated gate field effect transistor of this embodiment is a multi-cell type insulated gate field effect in which a cell region 9 composed of a source region 3 and a bulk region 2 surrounding the source region 3 is scattered in an island shape in a drain region 1 as in the conventional example. It is a transistor. The source region 3 is formed in a ring shape in the bulk region 2, and the bulk region 2 penetrates into the hole inside the source region 3. As shown in FIG. 1, the cell region 9 has a planar shape of a substantially square shape, and has four corner portions and four substantially linear side portions formed between the corner portions. There is. The corners are rounded in an arc shape so as to alleviate the electric field concentration as in the conventional example.

本実施例の従来例と異なる点は上記のセル領域9の平
面配置にある。即ち、ある1つのセル領域(以下、第1
のセル領域と称する)9の4つの角部にはそれぞれ異つ
た4つのセル領域(以下、第2のセル領域と称する)9
が近接して配置されている。また、第1のセル領域9と
第2のセル領域9とはその角部で互いに対向しており、
第1のセル領域9と第2のセル領域9との間隔は角部で
小さく、辺部で大きくなつている。なお、4つの第2の
セル領域9は第1のセル領域9に対してほぼ等間隔で配
置されている。上記の4つの第2のセル領域9のそれぞ
れもそれ自体を第1のセル領域として、それぞれの4つ
の角部には上記の第1のセル領域9を含む4つのセル領
域9が第2のセル領域9となつてそれらの角部が近接し
て配置されている。
The difference of this embodiment from the conventional example is the planar arrangement of the cell region 9 described above. That is, a certain cell region (hereinafter, referred to as the first
4 cell regions (hereinafter referred to as second cell regions) 9 which are different from each other at the four corners of the cell region 9).
Are placed close together. Further, the first cell region 9 and the second cell region 9 face each other at their corners,
The distance between the first cell region 9 and the second cell region 9 is small at the corners and large at the sides. The four second cell regions 9 are arranged at substantially equal intervals with respect to the first cell region 9. Each of the above-mentioned four second cell regions 9 is itself also the first cell region, and four cell regions 9 including the above-mentioned first cell region 9 are provided as the second cell regions at the respective four corners. The corners of the cell region 9 are arranged close to each other.

ドレイン領域1はドレイン電極7が接続されている不
純物濃度の比較的高いn+形の第1の領域1aと、この第1
の領域1aよりも不純物濃度の低いn形の第2の領域1b
と、この第2の領域1bよりも不純物濃度の高いn+形の第
3の領域1cとを有する。第2の領域1bは第5図と同様に
第1の領域1aの上にエピタキシャル成長で形成された領
域であってp形バルク領域2と第3の領域1cの下に配置
されている。第3の領域1cはセル領域9の対向間に配設
され、ドレイン領域1の最も上に形成されている。この
n+形の第3の領域1cはドレイン電流の通路に配置されて
いるので、オン抵抗を低くする作用効果を有する。高不
純物濃度の第3の領域1cを設けると、セル領域9の角度
の耐圧が低くなり易いが、本実施例ではセル領域9の配
置を第1図に示す配置にすることによって高耐圧化を図
り、第3の領域1cによる耐圧低下を抑制している。これ
によりオン抵抗が高い電界効果トランジスタを提供する
ことができる。
The drain region 1 includes an n + -type first region 1a having a relatively high impurity concentration, to which the drain electrode 7 is connected, and the first region 1a.
N-type second region 1b having a lower impurity concentration than the first region 1a
And an n + type third region 1c having an impurity concentration higher than that of the second region 1b. The second region 1b is a region formed by epitaxial growth on the first region 1a similarly to FIG. 5, and is arranged below the p-type bulk region 2 and the third region 1c. The third region 1c is arranged between the cell regions 9 facing each other, and is formed at the uppermost part of the drain region 1. this
Since the n + -type third region 1c is arranged in the drain current path, it has the effect of lowering the on-resistance. If the third region 1c having a high impurity concentration is provided, the angular breakdown voltage of the cell region 9 tends to be low, but in this embodiment, the arrangement of the cell region 9 is changed to the arrangement shown in FIG. The decrease in breakdown voltage due to the third region 1c is suppressed. This makes it possible to provide a field effect transistor having high on-resistance.

本実施例の電界効果トランジスタでは、ソース領域6
とドレイン電極7との間にドレイン電極7側を正とする
ドレイン・ソース間電圧VDSを印加すると、従来例の電
界効果トランジスタと同様に第2図に示す空乏層8が拡
がる。空乏層8はドレイン・ソース間電圧VDSが増大す
るにつれてその拡がりが大きくなる。本実施例では、ド
レイン・ソース間電圧VDSが増加してセル領域9とドレ
イン領域1によつて形成されるpn接合の逆方向降伏電圧
VB(セル領域9の間隔が十分大きい場合の値)より小さ
い所定の電圧VDS1に達したとき、第3図に模式的に示す
ように、第1のセル領域9と第2のセル領域9の間隔が
小さくなつている角部においてpn接合から横方向に延び
る空乏層が深く交絡していると見なせる空乏層8が形成
されるよう、第1のセル領域9と第2のセル領域9との
間隔が比較的小さく決定されている。第1のセル領域9
と第2のセル領域9との間隔が大きくなつている辺部に
おいては、電圧VDS1印加時に、第2図に示すようにpn接
合から横方向に延びる空乏層が交絡していないか又は交
絡していたとしても比較的浅い空乏層8が形成される。
以上のように、本実施例の電界効果トランジスタでは、
ドレイン・ソース間電圧VDSを増大すると、ブレークダ
ウンが生じる前にセル領域9の角部が対向した部分のド
レイン領域1が他のドレイン領域1に先立つてなめらか
に連続した空乏層8によつて満たされる。これによつ
て、電界集中の起こり易い角部の耐圧が向上し、耐圧の
大きい絶縁ゲート電界効果トランジスタを実現できる。
一方、第6図に示す従来の絶縁ゲート電界効果トランジ
スタに逆方向バイアス電圧VDS1を印加したときの角部に
おける空乏層8の拡がりは第5図に模式的に示すよう
に、近接する2つのセル領域9の角部の対向間隔が大き
くなつているため、空乏層8は電界集中を有効に緩和で
きるようになめらかに連続しない。また、従来例であつ
ても、対向する2つのセル領域9の間隔を小さくすれ
ば、本実施例のように角部の対向する領域に電界集中を
緩和する空乏層を容易に形成でき、耐圧向上の効果はそ
れなりに得られる。しかしながら、従来例の構造では辺
部の相互間隔が狭くなりすぎるためオン抵抗が増大す
る。本実施例では、角部の相互間隔が狭められるため、
この部分ではオン抵抗が増大するが、逆に辺部の相互間
隔が大きくなるためオン抵抗は減少する。結果として、
トータルのオン抵抗はセル領域の間隔を狭めていない状
態の従来例の絶縁ゲート電界効果トランジスタと同等の
小さい値となる。
In the field effect transistor of this embodiment, the source region 6
When a drain-source voltage V DS having a positive polarity on the drain electrode 7 side is applied between the drain electrode 7 and the drain electrode 7, the depletion layer 8 shown in FIG. 2 expands as in the field effect transistor of the conventional example. The spread of the depletion layer 8 increases as the drain-source voltage V DS increases. In this embodiment, the drain-source voltage V DS is increased and the reverse breakdown voltage of the pn junction formed by the cell region 9 and the drain region 1 is increased.
When a predetermined voltage V DS1 smaller than V B (value when the distance between the cell regions 9 is sufficiently large) is reached, as shown schematically in FIG. 3, the first cell region 9 and the second cell region 9 The first cell region 9 and the second cell region 9 are formed so that a depletion layer 8 that can be regarded as deeply entangled with the depletion layer extending laterally from the pn junction is formed at a corner portion where the distance between 9 is small. The interval between and is determined to be relatively small. First cell area 9
In the side portion where the distance between the second cell region 9 and the second cell region 9 is large, the depletion layer extending laterally from the pn junction is not entangled or entangled when the voltage V DS1 is applied, as shown in FIG. Even if it does, a relatively shallow depletion layer 8 is formed.
As described above, in the field effect transistor of this embodiment,
When the drain-source voltage V DS is increased, before the breakdown occurs, the drain region 1 at the portion where the corners of the cell region 9 face each other is smoothed continuously by the depletion layer 8 preceding other drain regions 1. It is filled. As a result, the breakdown voltage at the corner where electric field concentration is likely to occur is improved, and an insulated gate field effect transistor with a high breakdown voltage can be realized.
On the other hand, the spread of the depletion layer 8 at the corner when the reverse bias voltage V DS1 is applied to the conventional insulated gate field effect transistor shown in FIG. 6 is, as schematically shown in FIG. Since the opposing distance between the corners of the cell region 9 is large, the depletion layer 8 is not smoothly continuous so that the electric field concentration can be effectively alleviated. Further, even in the conventional example, if the distance between the two opposing cell regions 9 is made small, it is possible to easily form the depletion layer for relaxing the electric field concentration in the regions where the corners face each other as in the present embodiment, and the breakdown voltage is increased. The effect of improvement is obtained as it is. However, in the structure of the conventional example, the on-resistance increases because the mutual spacing of the sides becomes too narrow. In this embodiment, since the mutual intervals of the corners are narrowed,
Although the on-resistance increases in this portion, the on-resistance decreases conversely because the mutual intervals of the sides increase. as a result,
The total on-resistance has a small value equivalent to that of the conventional insulated gate field effect transistor in the state where the distance between the cell regions is not narrowed.

本実施例以外の構造であつても耐圧を向上させること
は可能である。例えば、本実施例の電界効果トランジス
タにおいて、第1のセル領域9の代わりにp形領域から
成る内部FLRを配置させることが考えられる。しかしな
がら、この構造ではチツプ上の電界効果トランジスタの
実働面積が減少してしまう。また、従来例の電界効果ト
ランジスタにおいて、セル領域9の平面形状を円形とし
て耐圧を向上することも考えられる。しかしながら、こ
の構造ではチヤンネル幅(セル領域9の周辺長)が小さ
くなり、電流容量が大きくとれなくなる。以上のよう
に、本実施例は絶縁ゲート電界効果トランジスタの高耐
圧化構造として最適な構造といえる。
It is possible to improve the breakdown voltage even with a structure other than that of this embodiment. For example, in the field effect transistor of this embodiment, it is conceivable to dispose the internal FLR formed of the p-type region instead of the first cell region 9. However, this structure reduces the active area of the field effect transistor on the chip. Further, in the field-effect transistor of the conventional example, it may be possible to improve the breakdown voltage by making the planar shape of the cell region 9 circular. However, in this structure, the channel width (peripheral length of the cell region 9) becomes small, and the current capacity cannot be made large. As described above, this example can be said to be the most suitable structure as a high breakdown voltage structure for an insulated gate field effect transistor.

本実施例の効果を要約すると以下のとおりである。 The effects of this embodiment are summarized as follows.

(1)耐圧の弱い点である角部の耐圧が向上し、高耐圧
の絶縁ゲート電界効果トランジスタを実現できる。
(1) The breakdown voltage at the corner, which is a weak point, is improved, and a high breakdown voltage insulated gate field effect transistor can be realized.

(2)オン抵抗の比較的小さい絶縁ゲート電界効果トラ
ンジスタを実現できる。
(2) An insulated gate field effect transistor having a relatively small on-resistance can be realized.

(3)面積効率の良い絶縁ゲート電界効果トランジスタ
が実現できる。
(3) An insulated gate field effect transistor with good area efficiency can be realized.

〔変形例〕(Modification)

本発明は上述の実施例に限定されるものでなく、例え
ば次の変形が可能なものである。
The present invention is not limited to the above-mentioned embodiments, and the following modifications are possible, for example.

(1)第4図に示すようにセル領域9の平面形状を略六
角形としてもよい。
(1) The planar shape of the cell region 9 may be substantially hexagonal as shown in FIG.

(2)バルク領域2が部分的に深く形成された周知のデ
イープベース構造の絶縁ゲート電界効果トランジスタに
も有効である。
(2) It is also effective for a well-known deep base insulated gate field effect transistor in which the bulk region 2 is partially deeply formed.

(3)本発明はセル領域の平面形状が実質的に四角形ま
たは六角形であれば有効である。例えば、四角形の角部
を実施例のように円弧状にしたり、テーパーを形成した
セル領域であつても有効である。なお、テーパーを形成
した場合には、それぞれのテーパー部分が対向するよう
に近接する2つのセル領域を配置する。
(3) The present invention is effective when the planar shape of the cell region is substantially quadrangular or hexagonal. For example, it is effective to make the corners of a quadrangle into an arc shape as in the embodiment or to form a tapered cell region. When the taper is formed, two adjacent cell regions are arranged so that the respective tapered portions face each other.

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

第1図は本発明の実施例に係わる絶縁ゲート電界効果ト
ランジスタの半導体基板の表面の一部を示す平面図、 第2図は第1図のII-II線に対応する部分の断面図、 第3図は第1図のIII-III線に対応する部分の断面図、 第4図は変形例の絶縁ゲート電界効果トランジスタの半
導体基板の表面の一部を示す平面図、 第5図は従来の絶縁ゲート電界効果トランジスタを示す
第6図のV-V線に対応する部分の断面図、 第6図は従来の絶縁ゲート電界効果トランジスタの半導
体基板の表面の一部を示す平面図である。 1……半導体基板、2……バルク領域、3……ソース領
域、9……セル領域。
1 is a plan view showing a part of the surface of a semiconductor substrate of an insulated gate field effect transistor according to an embodiment of the present invention, FIG. 2 is a sectional view of a portion corresponding to line II-II in FIG. FIG. 3 is a sectional view of a portion corresponding to the line III-III in FIG. 1, FIG. 4 is a plan view showing a part of the surface of a semiconductor substrate of an insulated gate field effect transistor of a modification, and FIG. FIG. 6 is a cross-sectional view of a portion corresponding to line VV in FIG. 6 showing an insulated gate field effect transistor, and FIG. 6 is a plan view showing a part of the surface of a semiconductor substrate of a conventional insulated gate field effect transistor. 1 ... Semiconductor substrate, 2 ... Bulk region, 3 ... Source region, 9 ... Cell region.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】バルク領域(2)とこのバルク領域(2)
の中に形成されたソース領域(3)とから成るセル領域
(9)がドレイン領域(1)内に島状に複数個配置され
ているマルチセルタイプの絶縁ゲート電界効果トランジ
スタにおいて、 前記複数個のセル領域は第1のセル領域と前記第1のセ
ル領域に対して互いに等しい間隔を有して前記第1のセ
ル領域の周囲に配置された複数の第2のセル領域とを有
し、 前記第1及び第2のセル領域の平面形状は略正四角形又
は略正六角形であり、 前記第1のセル領域の互いに対向する複数の対の角部を
結ぶ複数の仮想直線の延長線上に前記第2のセル領域の
それぞれが配置され、 前記第2のセル領域の中心及び角部が前記仮想直線の延
長線上に位置し、 前記第1のセル領域の角部とこれに隣り合う前記第2の
セル領域の角部との間の距離が前記第1のセル領域の辺
部とこれに隣り合う前記第2のセル領域の辺部との間の
距離よりも小さく設定され、 前記ドレイン領域(1)は高不純物濃度の第1の領域
(1a)と前記第1の領域(1a)よりも不純物濃度が低い
の第2の領域(1b)と前記第2の領域(1b)よりも不純
物濃度が高い第3の領域(1c)とを有し、 前記第1の領域(1a)にドレイン電極(7)が接続さ
れ、 前記第2の領域(1b)は前記第1の領域(1a)に隣接し
ていると共に前記バルク領域(2)と前記第1の領域
(1a)との間に介在し且つエピタキシャル成長で形成さ
れ、 前記第3の領域(1c)は前記第1のセル領域と前記2の
セル領域との対向間に配置されていることを特徴とする
絶縁ゲート電界効果トランジスタ。
1. A bulk region (2) and this bulk region (2)
In a multi-cell type insulated gate field effect transistor, wherein a plurality of cell regions (9) formed of a source region (3) formed in the drain region (1) are arranged in an island shape in the drain region (1). The cell region has a first cell region and a plurality of second cell regions arranged around the first cell region at equal intervals with respect to the first cell region, The planar shape of the first and second cell regions is a substantially regular quadrangle or a substantially regular hexagon, and the first cell region has a plurality of imaginary straight lines extending from a plurality of imaginary straight lines that connect a pair of opposing corners of the first cell region. Each of two cell regions is arranged, a center and a corner portion of the second cell region are located on an extension line of the virtual straight line, and a corner portion of the first cell region and the second cell region adjacent to the corner portion. The distance between the corner of the cell region is the first Is set to be smaller than the distance between the side of the region and the side of the second cell region adjacent thereto, and the drain region (1) and the first region (1a) having a high impurity concentration A second region (1b) having an impurity concentration lower than that of the first region (1a) and a third region (1c) having an impurity concentration higher than that of the second region (1b), The drain electrode (7) is connected to the first region (1a), the second region (1b) is adjacent to the first region (1a), and the bulk region (2) and the first region (1a) are connected to each other. The third region (1c) is interposed between the region (1a) and formed by epitaxial growth, and the third region (1c) is disposed between the first cell region and the second cell region facing each other. Insulated gate field effect transistor.
JP63308043A 1988-12-06 1988-12-06 Insulated gate field effect transistor Expired - Lifetime JPH0821714B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63308043A JPH0821714B2 (en) 1988-12-06 1988-12-06 Insulated gate field effect transistor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63308043A JPH0821714B2 (en) 1988-12-06 1988-12-06 Insulated gate field effect transistor

Publications (2)

Publication Number Publication Date
JPH02154468A JPH02154468A (en) 1990-06-13
JPH0821714B2 true JPH0821714B2 (en) 1996-03-04

Family

ID=17976194

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63308043A Expired - Lifetime JPH0821714B2 (en) 1988-12-06 1988-12-06 Insulated gate field effect transistor

Country Status (1)

Country Link
JP (1) JPH0821714B2 (en)

Families Citing this family (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH04363069A (en) * 1990-09-24 1992-12-15 Nippondenso Co Ltd Vertical semiconductor device
JPH04273167A (en) * 1991-02-28 1992-09-29 Sharp Corp Vertical type power mosfet
TW290735B (en) * 1994-01-07 1996-11-11 Fuji Electric Co Ltd
US6107661A (en) * 1995-09-29 2000-08-22 Nippondenso Co., Ltd. Semiconductor device and method of manufacturing same
JP5687128B2 (en) * 2011-05-06 2015-03-18 三菱電機株式会社 Semiconductor device and manufacturing method thereof

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2644989B2 (en) * 1984-05-09 1997-08-25 株式会社東芝 Conduction modulation type MOSFET
JPH0687506B2 (en) * 1988-03-18 1994-11-02 三洋電機株式会社 Power MOSFET

Also Published As

Publication number Publication date
JPH02154468A (en) 1990-06-13

Similar Documents

Publication Publication Date Title
JP5741567B2 (en) Semiconductor device
USRE47198E1 (en) Power semiconductor device
US10978580B2 (en) Insulated gate bipolar transistor and diode
US5753942A (en) Power semiconductor devices having arcuate-shaped source regions for inhibiting parasitic thyristor latch-up
JPH03270273A (en) Semiconductor device and its manufacture
CN108682688B (en) Composite gate IGBT chip with three-dimensional channel
JP2004022693A (en) Semiconductor device
JP2023040134A (en) semiconductor equipment
US11264451B2 (en) Semiconductor device exhibiting soft recovery characteristics
JP2008277352A (en) Semiconductor device
US7276772B2 (en) Semiconductor device
US7196376B2 (en) Trench-type power MOSFET with embedded region at the bottom of the gate and increased breakdown voltage
JPH0354868A (en) Mos type semiconductor device
JP2000077663A (en) Field effect type semiconductor device
KR100873419B1 (en) Power semiconductor devices with high breakdown voltage, low on-resistance and small switching losses
JPH0588554B2 (en)
KR910004318B1 (en) Cells in Vertical D MOS Transistors
JP2023053145A (en) RC-IGBT semiconductor device
JPH0821714B2 (en) Insulated gate field effect transistor
US6563169B1 (en) Semiconductor device with high withstand voltage and a drain layer having a highly conductive region connectable to a diffused source layer by an inverted layer
US11189698B2 (en) Semiconductor power device
JP2006269633A (en) Power semiconductor device
JP4264316B2 (en) Semiconductor device and manufacturing method thereof
JPH0612823B2 (en) Bidirectional power high speed MOSFET device
JPH01238174A (en) Vertical mosfet