JPS641943B2 - - Google Patents
Info
- Publication number
- JPS641943B2 JPS641943B2 JP55099584A JP9958480A JPS641943B2 JP S641943 B2 JPS641943 B2 JP S641943B2 JP 55099584 A JP55099584 A JP 55099584A JP 9958480 A JP9958480 A JP 9958480A JP S641943 B2 JPS641943 B2 JP S641943B2
- Authority
- JP
- Japan
- Prior art keywords
- region
- semiconductor region
- semiconductor
- conductive layer
- regions
- 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
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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
- H10D62/10—Shapes, relative sizes or dispositions of the regions of the semiconductor bodies; Shapes of the semiconductor bodies
- H10D62/102—Constructional design considerations for preventing surface leakage or controlling electric field concentration
- H10D62/103—Constructional design considerations for preventing surface leakage or controlling electric field concentration for increasing or controlling the breakdown voltage of reverse-biased devices
- H10D62/104—Constructional design considerations for preventing surface leakage or controlling electric field concentration for increasing or controlling the breakdown voltage of reverse-biased devices having particular shapes of the bodies at or near reverse-biased junctions, e.g. having bevels or moats
-
- 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
- H10D62/10—Shapes, relative sizes or dispositions of the regions of the semiconductor bodies; Shapes of the semiconductor bodies
- H10D62/17—Semiconductor regions connected to electrodes not carrying current to be rectified, amplified or switched, e.g. channel regions
- H10D62/351—Substrate regions of field-effect devices
- H10D62/357—Substrate regions of field-effect devices of FETs
- H10D62/364—Substrate regions of field-effect devices of FETs of IGFETs
-
- 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
- H10D62/10—Shapes, relative sizes or dispositions of the regions of the semiconductor bodies; Shapes of the semiconductor bodies
- H10D62/17—Semiconductor regions connected to electrodes not carrying current to be rectified, amplified or switched, e.g. channel regions
- H10D62/351—Substrate regions of field-effect devices
- H10D62/357—Substrate regions of field-effect devices of FETs
- H10D62/364—Substrate regions of field-effect devices of FETs of IGFETs
- H10D62/378—Contact regions to the substrate regions
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D64/00—Electrodes of devices having potential barriers
- H10D64/20—Electrodes characterised by their shapes, relative sizes or dispositions
- H10D64/27—Electrodes not carrying the current to be rectified, amplified, oscillated or switched, e.g. gates
Description
【発明の詳細な説明】
本発明は絶縁ゲート電界効果トランジスタの改
良に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to improvements in insulated gate field effect transistors.
絶縁ゲート電界効果トランジスタとして従来、
第1図に示す如く、N-型の半導体基板1内にそ
の主面2側よりN+型の半導体領域3及びP型の
半導体領域4が形成され、又半導体領域4内に主
面2側よりN+型の半導体領域5が形成され、一
方半導体領域4の半導体領域5と半導体基板1の
半導体領域4及び3間の領域6との間の領域7に
於ける主面2側の表面8上に絶縁層9を介して導
電性層10が配され、又半導体領域3及び5に主
面2側より導電性層11及び12がオーミツクに
附され、更に半導体領域4にその領域5よりみて
領域7側とは反対側の領域13に於て主面2側よ
り導電性層14がオーミツクに附されてなり、而
して半導体基板1及び半導体領域3をドレイン領
域、半導体領域5をソース領域、半導体領域4の
半導体領域5と半導体基板1の半導体領域4及び
3間の領域6との間の領域7をチヤンネル形成用
領域、絶縁層9をゲート用絶縁層、導電性層10
をゲート電極、導電性層11及び12を夫々ドレ
イン電極及びソース電極、導電性層14をバツク
ゲート電極とせる構成のものが提案されている。 Conventionally, as an insulated gate field effect transistor,
As shown in FIG. 1, an N + type semiconductor region 3 and a P type semiconductor region 4 are formed in an N - type semiconductor substrate 1 from the main surface 2 side, and in the semiconductor region 4 from the main surface 2 side. An N + type semiconductor region 5 is formed, and a surface 8 on the main surface 2 side in a region 7 between the semiconductor region 5 of the semiconductor region 4 and the region 6 between the semiconductor regions 4 and 3 of the semiconductor substrate 1 A conductive layer 10 is disposed thereon through an insulating layer 9, and conductive layers 11 and 12 are ohmicly applied to the semiconductor regions 3 and 5 from the main surface 2 side, and furthermore, conductive layers 11 and 12 are ohmicly applied to the semiconductor regions 4 and 5 when viewed from the region 5. In the region 13 opposite to the region 7 side, a conductive layer 14 is ohmicly applied from the main surface 2 side, so that the semiconductor substrate 1 and the semiconductor region 3 are used as a drain region, and the semiconductor region 5 is used as a source region. , the region 7 between the semiconductor region 5 of the semiconductor region 4 and the region 6 between the semiconductor regions 4 and 3 of the semiconductor substrate 1 is a channel forming region, the insulating layer 9 is a gate insulating layer, and the conductive layer 10
A configuration has been proposed in which the conductive layers 11 and 12 are used as a gate electrode, the conductive layers 11 and 12 are used as a drain electrode and a source electrode, respectively, and the conductive layer 14 is used as a back gate electrode.
所で斯る絶縁ゲート電界効果トランジスタの構
成によれば、ソース電極としての導電性層12及
びバツクゲート電極としての導電性層14とドレ
イン電極としての導電性層11との間に導電性層
11側を正とする所要の作動電源20を負荷21
を通じて接続し、又導電性層12及び14とゲー
ト電極としての導電性層10との間に制御電圧源
23を接続せる状態で、制御電圧源23より得ら
れる制御電圧の値が所定の値(閾値)以上の値と
なれば、チヤンネル形成用領域としての半導体領
域4の領域7の表面8側にN型反転層によるチヤ
ンネルが形成され、従つてオン状態が得られる
為、負荷21に作動電源20より、導電性層1
1、ドレイン領域としての半導体領域3及び半導
体基板1の領域3及び4間の領域6、チヤンネル
形成用領域としての領域7に形成せるチヤンネ
ル、ソース領域としての半導体領域5、導電性層
12を通つてこの場合の制御電圧の値に応じた値
の電流が供給され、又斯る状態より制御電圧源2
3より得られる制御電圧の値が閾値より低い値を
とれば、上述せるチヤンネルが形成されず、従つ
てオフ状態が得られる為、負荷21に上述せる電
流が供給されないという、絶縁ゲート電界効果ト
ランジスタとしての機能が得られるものである。 According to the structure of such an insulated gate field effect transistor, there is a conductive layer 11 side between the conductive layer 12 as the source electrode, the conductive layer 14 as the back gate electrode, and the conductive layer 11 as the drain electrode. The required operating power source 20 with positive is the load 21
With the control voltage source 23 connected between the conductive layers 12 and 14 and the conductive layer 10 serving as a gate electrode, the value of the control voltage obtained from the control voltage source 23 becomes a predetermined value ( If the value exceeds the threshold (threshold value), a channel is formed by the N-type inversion layer on the surface 8 side of the region 7 of the semiconductor region 4 as a channel formation region, and therefore an on state is obtained, so that the load 21 is connected to the operating power supply. From 20, conductive layer 1
1. Through the semiconductor region 3 as a drain region, the region 6 between regions 3 and 4 of the semiconductor substrate 1, the channel formed in the region 7 as a channel formation region, the semiconductor region 5 as a source region, and the conductive layer 12. In this case, a current of a value corresponding to the value of the control voltage is supplied, and from this state, the control voltage source 2
If the value of the control voltage obtained from 3 takes a value lower than the threshold value, the above-mentioned channel is not formed, and therefore an off state is obtained, so that the above-mentioned current is not supplied to the load 21. This function can be obtained as follows.
又第1図にて上述せる従来の絶縁ゲート電界効
果トランジスタの構成によれば、上述せる絶縁ゲ
ート電界効果トランジスタとしての機能が得られ
るものであるが、ドレイン領域がN-型の半導体
基板1従つてドレイン電極としての導電性層11
の附されてなるN+型従つて比抵抗の低い半導体
領域3に比し高い比抵抗を有する半導体基板1を
含んで構成されていることにより、導電性層11
及び12間の耐圧が、若しドレイン領域を構成せ
る半導体基板1及び半導体領域3が半導体領域3
と同じ比抵抗を有する半導体領域を以つて構成さ
れているものとした場合に比し高く、又その耐圧
は、これを半導体基板1の比抵抗を高くすればす
る程、又半導体領域4及び3間の間隔従つて半導
体基板1の半導体領域4及び3間の領域7の長さ
を大とすればする程、より高くし得るという特徴
を有するものである。 Further, according to the structure of the conventional insulated gate field effect transistor shown in FIG. 1 , the function as the insulated gate field effect transistor described above can be obtained. Conductive layer 11 as a drain electrode
The conductive layer 11 is composed of a semiconductor substrate 1 having a higher specific resistance than an N + type semiconductor region 3 having a low specific resistance.
and 12, if the semiconductor substrate 1 and semiconductor region 3 constituting the drain region are
The higher the resistivity is, the higher the resistivity of the semiconductor substrate 1 is, the higher the breakdown voltage is, the higher the resistivity of the semiconductor substrate 1 is, the higher the resistivity of the semiconductor regions 4 and 3 is. It has the characteristic that the larger the distance between the semiconductor regions 4 and 3, that is, the length of the region 7 between the semiconductor regions 4 and 3 of the semiconductor substrate 1, the higher the height can be made.
然し乍ら第1図にて上述せる絶縁ゲート電界効
果トランジスタの構成の場合、上述せる如く導電
性層11及び12間の耐圧が高いものであるが、
上述せる如くにオン状態が得られている状態での
導電性層12及び11間の抵抗即ち所謂オン抵抗
が高く、従つて上述せる如くオン状態が得られて
いて負荷に電流を供給している状態でのその電流
値を大なるものとして得るに一定の限度を有する
という欠点を有していた。 However, in the case of the structure of the insulated gate field effect transistor described above in FIG. 1, although the breakdown voltage between the conductive layers 11 and 12 is high as described above,
The resistance between the conductive layers 12 and 11, that is, the so-called on-resistance, is high when the on-state is obtained as described above, and therefore, the on-state is obtained as described above and current is supplied to the load. It has the disadvantage that there is a certain limit to the ability to obtain a large current value under certain conditions.
依つて本発明は第1図にて上述せる従来の絶縁
ゲート電界効果トランジスタと同様の絶縁ゲート
電界効果トランジスタとしての機能が得られる
も、上述せる欠点のない新規な絶縁ゲート電界効
果トランジスタを提案せんとするもので、以下詳
述する所より明らかとなるであろう。 Therefore, the present invention proposes a novel insulated gate field effect transistor that can obtain the same function as an insulated gate field effect transistor as the conventional insulated gate field effect transistor shown in FIG. This will become clear from the detailed explanation below.
第2図は本発明に依る絶縁ゲート電界効果トラ
ンジスタの一例を示し、P-型の半導体基板30
の主面31上にN型の半導体層32及びP型の半
導体層33がそれ等の半導体基板30側とは反対
側の主面34及び35をして同一平面内に在らし
めた関係で並置連接して形成され、又半導体層3
2内にその主面34側よりN+型の半導体領域3
6が形成され、更に半導体層33内にその主面3
5側より同様にN+型の半導体領域37が形成さ
れ、尚更に半導体基板30内にその半導体層32
及び33側とは反対側の主面38側よりP+型の
半導体領域39が形成され、一方半導体層33の
半導体領域37及び半導体層32間の領域40に
於ける主面35側の表面42上に絶縁層42を介
して導電性層43が配され、又半導体領域36及
び37に夫々主面34及び35側より導電性層4
4及び45がオーミツクに附され、更に半導体層
33にその領域37よりみて領域40側とは反対
側の領域49に於て主面35側より導電性層46
が附され、尚更に半導体領域39に半導体層32
及び33側とは反対側より導電性層47がオーミ
ツクに附されてなり、従つて半導体領域36によ
るN+型の第1の半導体領域Q1と、半導体層3
2による第1の半導体領域Q1に連接せるN型の
第2の半導体領域Q2と、半導体領域33による
第1の半導体領域Q1には連接せざるも第2の半
導体領域Q2に連接せる第3の半導体領域Q3
と、半導体領域37による第1及び第2の半導体
領域Q1及びQ2には連接せざるも第3の半導体
領域Q3に連接せるN+型の第4の半導体領域Q
4と、半導体層33の領域40による第3の半導
体領域Q3の第2及び第4の半導体領域Q2及び
Q4間の領域B1の表面41による表面S1上に
絶縁層42による絶縁層Iを介して配された導電
性層43による導電性層MGと、第1の半導体領
域Q1にオーミツクに附された導電性層44によ
る導電性層MDと、第4の半導体領域Q4にオー
ミツクに附された導電姓層45による導電性層
MSと、第3の半導体領域Q3にオーミツクに附
された導電姓層46による導電姓層MBとを具備
し、又半導体基板30による等1及び第4の半導
体領域には連接せざるも少くとも第2の半導体領
域Q2の第1及び第3の半導体領域Q1及びQ2
間の領域B2及び第3の半導体領域Q3に連接せ
るP-型の即ち第2の半導体領域Q2に比し高い
比抵抗を有し且P型を有する第5の半導体領域Q
5(図に於ては第2の半導体領域Q2の領域B2
の外、第2の半導体領域Q2の第1の半導体領域
Q1下の領域B3及び第2の半導体領域Q2の第
1の半導体領域Q1よりみて領域B2側とは反対
側の領域B4にも連接している)と、その第5の
半導体領域Q5にP+型の半導体領域39を介し
て附された導電性層47による導電性層MQとを
具備する構成を有し、又半導体層32の半導体層
33及び半導体領域36間の領域に主面34側よ
り半導体基板30側にそれに達することなしに延
長せるU字状の溝Hが形成され、従つて上述せる
第1、第2、第3、第4及び第5の半導体領域Q
1、Q2、Q3、Q4及びQ5、上述せる絶縁層
I、上述せる導電性層MG、MS、MD及びMQの
外、半導体層32の半導体領域36及び半導体層
33の領域による第2の半導体領域Q2の第1及
び第3の半導体領域Q1及びQ3間の領域B2
に、その半導体基板30による第5の半導体領域
Q5の連接せざる側より第5の半導体領域Q5側
にそれに達することなしに延長せる溝Hを具備す
る構成を有する。 FIG. 2 shows an example of an insulated gate field effect transistor according to the present invention, in which a P - type semiconductor substrate 30
An N-type semiconductor layer 32 and a P-type semiconductor layer 33 are placed on the main surface 31 of the semiconductor substrate 30, with the main surfaces 34 and 35 on the opposite side to the semiconductor substrate 30 being in the same plane. The semiconductor layer 3 is formed in a juxtaposed and connected manner.
2, an N + type semiconductor region 3 is formed from the main surface 34 side.
6 is formed, and the main surface 3 is further formed in the semiconductor layer 33.
Similarly, an N + type semiconductor region 37 is formed from the 5 side, and the semiconductor layer 32 is further formed in the semiconductor substrate 30.
A P + type semiconductor region 39 is formed from the main surface 38 side opposite to the 33 side, and a surface 42 on the main surface 35 side in a region 40 between the semiconductor region 37 and the semiconductor layer 32 of the semiconductor layer 33. A conductive layer 43 is disposed thereon through an insulating layer 42, and a conductive layer 4 is disposed on the semiconductor regions 36 and 37 from the principal surfaces 34 and 35, respectively.
4 and 45 are attached to the ohmic, and a conductive layer 46 is further applied to the semiconductor layer 33 from the main surface 35 side in a region 49 on the opposite side to the region 40 side as seen from the region 37.
is attached, and furthermore, a semiconductor layer 32 is attached to the semiconductor region 39.
A conductive layer 47 is attached to the ohmic from the side opposite to the semiconductor region 36 and the N + type first semiconductor region Q1 and the semiconductor layer 33.
an N-type second semiconductor region Q2 connected to the first semiconductor region Q1 by the semiconductor region 33; Semiconductor area Q3
and an N + type fourth semiconductor region Q which is not connected to the first and second semiconductor regions Q1 and Q2 by the semiconductor region 37 but is connected to the third semiconductor region Q3.
4, and a surface 41 of the region B1 between the second and fourth semiconductor regions Q2 and Q4 of the third semiconductor region Q3 by the region 40 of the semiconductor layer 33, and an insulating layer I formed by the insulating layer 42 on the surface S1. A conductive layer MG formed by a conductive layer 43 arranged, a conductive layer MD formed by a conductive layer 44 ohmicly attached to the first semiconductor region Q1, and a conductive layer MD formed ohmicly attached to the fourth semiconductor region Q4. Conductive layer formed by the last layer 45
MS, and a conductive layer MB formed by a conductive layer 46 ohmically attached to the third semiconductor region Q3, and at least connected to the first and fourth semiconductor regions such as by the semiconductor substrate 30. First and third semiconductor regions Q1 and Q2 of second semiconductor region Q2
A fifth semiconductor region Q having a P type and having a resistivity higher than that of the P - type, that is, the second semiconductor region Q2, which is connected to the intervening region B2 and the third semiconductor region Q3.
5 (in the figure, region B2 of the second semiconductor region Q2
In addition, the second semiconductor region Q2 is connected to a region B3 below the first semiconductor region Q1 and a region B4 of the second semiconductor region Q2 on the opposite side to the region B2 side when viewed from the first semiconductor region Q1. ) and a conductive layer MQ formed by a conductive layer 47 attached to the fifth semiconductor region Q5 via a P + type semiconductor region 39, and A U-shaped groove H that can extend from the main surface 34 side to the semiconductor substrate 30 side without reaching there is formed in the region between the layer 33 and the semiconductor region 36, so that the above-mentioned first, second, third, Fourth and fifth semiconductor regions Q
1, Q2, Q3, Q4, and Q5, the above-mentioned insulating layer I, the above-mentioned conductive layers MG, MS, MD, and MQ, as well as a second semiconductor region formed by the semiconductor region 36 of the semiconductor layer 32 and the semiconductor layer 33. Region B2 between the first and third semiconductor regions Q1 and Q3 of Q2
In addition, the semiconductor substrate 30 is provided with a groove H that can extend from the non-contiguous side of the fifth semiconductor region Q5 to the fifth semiconductor region Q5 side without reaching the fifth semiconductor region Q5.
以上が本発明による絶縁ゲート電界効果トラン
ジスタの一例構成であるが、斯る構成によれば、
その第1及び第2の半導体領域Q1及びQ2が第
1図にて上述せる従来の絶縁ゲート電界効果トラ
ンジスタの半導体基板1及び半導体領域3に、第
4の半導体領域Q4が第1図の半導体領域5に、
第3の半導体領域Q3の第2及び第4の半導体領
域Q2及びQ4間の領域B1が第1図の半導体領
域4の半導体領域5と半導体基板1の半導体領域
4及び3間の領域6との間の領域7に、絶縁層I
が第1図の絶縁層9に、導電性層MG、MD、
MS及びMBが夫々第1図の導電性層10、11、
12及び14に対応していることにより、第1及
び第2の半導体領域Q1及びQ2をドレイン領
域、第4の半導体領域Q4をソース領域、第3の
半導体領域Q3の第2及び第4の半導体領域Q2
及びQ4間の領域B1をチヤンネル形成用領域、
絶縁層Iをゲート用絶縁層、導電性層MG、
MD、MS及びMBを夫々ゲート電極、ドレイン
電極、ソース電極及びバツクゲート電極とせる絶
縁ゲート電界効果トランジスタを構成しているこ
と明らかである。 The above is an example of the structure of an insulated gate field effect transistor according to the present invention. According to such a structure,
The first and second semiconductor regions Q1 and Q2 are the semiconductor substrate 1 and semiconductor region 3 of the conventional insulated gate field effect transistor described above in FIG. 1, and the fourth semiconductor region Q4 is the semiconductor region of FIG. 5,
The region B1 between the second and fourth semiconductor regions Q2 and Q4 of the third semiconductor region Q3 is connected to the semiconductor region 5 of the semiconductor region 4 and the region 6 between the semiconductor regions 4 and 3 of the semiconductor substrate 1 in FIG. In the region 7 between, an insulating layer I
is the insulating layer 9 in FIG. 1, and conductive layers MG, MD,
MS and MB are respectively the conductive layers 10 and 11 of FIG.
12 and 14, the first and second semiconductor regions Q1 and Q2 are drain regions, the fourth semiconductor region Q4 is a source region, and the second and fourth semiconductor regions of the third semiconductor region Q3 are Area Q2
and Q4, the region B1 is a channel forming region,
The insulating layer I is an insulating layer for a gate, a conductive layer MG,
It is clear that an insulated gate field effect transistor is constructed in which MD, MS, and MB serve as a gate electrode, a drain electrode, a source electrode, and a back gate electrode, respectively.
従つて第2図にて上述せる本発明による絶縁ゲ
ート電界効果トランジスタの構成によれば、ソー
ス電極としての導電性層MS、バツクゲート電極
としての導電性層MB及び導電性層MQとドレイ
ン電極としての導電性層MDとの間に導電性層
MD側を正とする所要の作動電源50を負荷51
を通じて接続し、又導電性層MS、MB及びMQ
とゲート電極としての導電性層MGとの間に制御
電圧源53を接続せる状態で、制御電圧源53よ
り得られる制御電圧の値が所定の値(閾値)以上
の値となれば、チヤンネル形成用領域としての第
3の半導体領域Q3の領域B1の表面側にN型反
転層によるチヤンネルが形成され、従つてオン状
態が得られる為、負荷51に作動電源50より、
導電性層MD、ドレイン領域としての第1の半導
体領域Q1及び第2の半導体領域Q2の領域B
2、チヤンネル形成用領域としての領域B1に形
成せるチヤンネル、ソース領域としての第4の半
導体領域Q4、導電性層MSを通つてこの場合の
制御電圧の値に応じた値の電流が供給され、又斯
る状態より制御電圧源53より得られる制御電圧
の値が閾値より低い値をとれば、上述せるチヤン
ネルが形成されず、従つてオフ状態が得られる
為、負荷51に上述せる電流が供給されないとい
う、第1図にて上述せる絶縁ゲート電界効果トラ
ンジスタの場合と同様の絶縁ゲート電界効果トラ
ンジスタとしての機能が得られるものである。 Therefore, according to the structure of the insulated gate field effect transistor according to the present invention described above in FIG. 2, the conductive layer MS as the source electrode, the conductive layer MB as the back gate electrode, the conductive layer MQ as the drain electrode, A conductive layer between the conductive layer MD
The required operating power source 50 with the MD side as positive is connected to the load 51
Connected through and also conductive layers MS, MB and MQ
When the control voltage source 53 is connected between the control voltage source 53 and the conductive layer MG as a gate electrode, if the value of the control voltage obtained from the control voltage source 53 becomes a predetermined value (threshold value) or more, a channel is formed. A channel by an N-type inversion layer is formed on the surface side of the region B1 of the third semiconductor region Q3 as a storage region, and therefore an on state is obtained.
Conductive layer MD, region B of the first semiconductor region Q1 and second semiconductor region Q2 as a drain region
2. A current having a value corresponding to the value of the control voltage in this case is supplied through the channel formed in the region B1 as the channel forming region, the fourth semiconductor region Q4 as the source region, and the conductive layer MS; In addition, if the value of the control voltage obtained from the control voltage source 53 takes a value lower than the threshold value in such a state, the above-mentioned channel is not formed, and therefore an OFF state is obtained, so that the above-mentioned current is supplied to the load 51. In this case, the function as an insulated gate field effect transistor similar to that of the insulated gate field effect transistor described above in FIG. 1 can be obtained.
又第2図にて上述せる本発明による絶縁ゲート
電界効果トランジスタの構成によれば、上述せる
絶縁ゲート電界効果トランジスタとしての機能が
得られるものであるが、第3の半導体領域Q3
と、第2の半導体領域Q2の第3及び第1の半導
体領域Q3及びQ1間の領域B2とに連接せる第
5の半導体領域Q5と、第2の半導体領域Q2の
第3及び第1の半導体領域Q3及びQ1間の領域
B2にその第5の半導体領域Q5の連接せざる側
より第5の半導体領域Q5側にそれに達すること
なしに延長せる溝Hとを有していることにより、
導電性層MS及びMD間に大なる電圧が印加され
た場合、第2及び第5の半導体領域Q2及びQ5
間のPN接合により溝Hに達する空乏層が得ら
れ、而してその空乏層によつて第2の半導体領域
Q2が溝Hの位置を挟んだ第3の半導体領域Q3
側部と第1の半導体領域Q1側部とに分離される
ものである。 Further, according to the structure of the insulated gate field effect transistor according to the present invention as described above in FIG. 2, the function as the insulated gate field effect transistor described above can be obtained.
and a fifth semiconductor region Q5 connected to the third and first semiconductor regions Q3 of the second semiconductor region Q2 and the region B2 between Q1, and the third and first semiconductor regions of the second semiconductor region Q2. By having a groove H in the region B2 between the regions Q3 and Q1 that can extend from the non-contiguous side of the fifth semiconductor region Q5 to the fifth semiconductor region Q5 side without reaching it,
When a large voltage is applied between the conductive layers MS and MD, the second and fifth semiconductor regions Q2 and Q5
A depletion layer reaching the groove H is obtained by the PN junction between the two, and the depletion layer allows the second semiconductor region Q2 to form a third semiconductor region Q3 with the position of the groove H sandwiched therebetween.
It is separated into a side portion and a side portion of the first semiconductor region Q1.
従つて導電性層MS及びMD間の耐圧が、第1
の半導体領域Q1、第2の半導体領域Q2の溝H
よりみて第1の半導体領域Q1側の部、第5の半
導体領域Q5、第3の半導体領域Q3及び第4の
半導体領域Q4中主として第2の半導体領域Q2
の溝Hよりみた第1の半導体領域Q1側の部及び
第5の半導体領域Q5に依在し、而して第5の半
導体領域Q5の比抵抗が第2の半導体領域Q2の
それに比し高いので、導電性層MS及びMD間の
耐圧が高いものである。又その耐圧は、これを第
5の半導体領域Q5の比抵抗を高くすればする
程、より高くし得るものである。 Therefore, the breakdown voltage between the conductive layers MS and MD is the first
groove H in the semiconductor region Q1 and the second semiconductor region Q2.
When viewed from above, the portion on the first semiconductor region Q1 side, the fifth semiconductor region Q5, the third semiconductor region Q3, and the fourth semiconductor region Q4 are mainly the second semiconductor region Q2.
The specific resistance of the fifth semiconductor region Q5 is higher than that of the second semiconductor region Q2. Therefore, the breakdown voltage between the conductive layers MS and MD is high. Further, the breakdown voltage can be increased as the specific resistance of the fifth semiconductor region Q5 is increased.
又第2図にて上述せる絶縁ゲート電界効果トラ
ンジスタの構成によれば、上述せる如く第5の半
導体領域Q5及び溝Hの存在によつて導電性層
MS及びMD間の耐圧を高くし得るものがあるが
上述せるオン状態に於ては第5の半導体領域Q5
及び溝Hは無関係であり、一方そのオン状態が得
られている状態でのオン抵抗は第2の半導体領域
Q2の領域B2の比抵抗に依在するも、その比抵
抗が第5の半導体領域Q5のそれに比し低いの
で、そのオン抵抗が同じ耐圧を得るにつき第1図
にて上述せる従来の絶縁ゲート電界効果トランジ
スタの場合に比し低くなり、依つてオン状態が得
られていて負荷51に電流を供給している状態で
のその電流値を第1図にて上述せる従来の絶縁ゲ
ート電界効果トランジスタの場合に比し大なるも
のとして得ることが出来るものである。 Further, according to the structure of the insulated gate field effect transistor described above in FIG. 2, the conductive layer is
There is a method that can increase the withstand voltage between MS and MD, but in the above-mentioned on state, the fifth semiconductor region Q5
On the other hand, the on-resistance in the state where the on-state is obtained depends on the specific resistance of the region B2 of the second semiconductor region Q2; Since its on-resistance is lower than that of Q5, its on-resistance is lower than that of the conventional insulated gate field effect transistor described above in FIG. The current value when the current is being supplied to the transistor can be obtained to be larger than that of the conventional insulated gate field effect transistor shown in FIG.
依つて第2図にて上述せる本発明による絶縁ゲ
ート電界効果トランジスタによれば、高い耐圧が
得られ、それでいて低いオン抵抗が得られるとい
う大なる特徴を有するものである。 Accordingly, the insulated gate field effect transistor according to the present invention described above with reference to FIG. 2 has the great feature of being able to obtain a high withstand voltage and yet a low on-resistance.
次に第3図を伴なつて本発明による絶縁ゲート
電界効果トランジスタの他の例を述べるに、第2
図との対応部分には同一符号を附し詳細説明はこ
れを省略するも、第2図にて上述せる構成に於
て、その第2の半導体領域Q2が第3の半導体領
域Q3内に第5の半導体領域Q5側に於て延長せ
るものとして形成され、又溝Hが第1及び第3の
半導体領域Q1及びQ3に亘り且第3の半導体領
域Q3を横切つて第2の半導体領域Q2内に終絡
するV字状の溝として形成され、絶縁層Iを介し
て導電性層MGの配される第3の半導体領域Q3
の表面S1が第3の半導体領域Q3の溝Hに臨む
表面となされていることを除いては、第2図の場
合と同様の構成を有する。 Next, referring to FIG. 3, another example of the insulated gate field effect transistor according to the present invention will be described.
Although the same reference numerals are given to corresponding parts in the figure and detailed explanation thereof is omitted, in the configuration described above in FIG. 2, the second semiconductor region Q2 is located within the third semiconductor region Q3. The groove H is formed to be extended on the semiconductor region Q5 side of No. A third semiconductor region Q3 is formed as a V-shaped groove that terminates in
The structure is similar to that of the case shown in FIG. 2, except that the surface S1 is the surface facing the trench H of the third semiconductor region Q3.
以上が本発明による絶縁ゲート電界効果トラン
ジスタの他の例の構成であるが、斯る構成によれ
ば、それが上述せる事項を除いては第2図の場合
と同様の構成を有するので、詳細説明はこれを省
略するも、第2図にて上述せる本発明による絶縁
ゲート電界効果トランジスタの場合と同様の優れ
た特徴を有するものである。 The above is the configuration of another example of the insulated gate field effect transistor according to the present invention. According to this configuration, it has the same configuration as the case of FIG. 2 except for the matters mentioned above, so the details will be explained below. Although the description thereof will be omitted, it has the same excellent characteristics as the insulated gate field effect transistor according to the present invention described above with reference to FIG.
尚上述に於ては本発明の僅かな実施例を示した
に留り、例えば上述せる「P-型」を「N-型」、
「N型」を「P型」、「N+型」を「P+型」、「P+型」
を「N+型」と読み代えた構成とすることも出来、
又導電性層MB及びMSが図示の如く互に接続さ
れ使用されるものとすれば、それ等導電性層MB
及びMSをそれ等の位置間に連続延長せる1つの
導電性層とすることも出来、その他本発明の精神
を脱することなしに種々の変型変更をなし得るで
あろう。 The above description has only shown a few embodiments of the present invention, and for example, the above-mentioned "P - type" may be referred to as "N - type",
"N type" is "P type", "N + type" is "P + type", "P + type"
It is also possible to read it as "N + type",
Also, if the conductive layers MB and MS are used connected to each other as shown, the conductive layers MB
and MS could be a single conductive layer extending continuously between these locations, and various other modifications could be made without departing from the spirit of the invention.
第1図は従来の絶縁ゲート電界効果トランジス
タを示す略線的断面図、第2図は本発明による絶
縁ゲート電界効果トランジスタの一例を示す略線
的断面図、第3図は本発明による絶縁ゲート電界
効果トランジスタの他の例を示す略線的断面図で
ある。
図中、Q1、Q2、Q3、Q4及びQ5は第
1、第2、第3、第4及び第5の半導体領域、I
は絶縁層、MG、MD、MS及びMBは導電性層、
Hは溝を夫々示す。
FIG. 1 is a schematic cross-sectional view showing a conventional insulated gate field effect transistor, FIG. 2 is a schematic cross-sectional view showing an example of an insulated gate field effect transistor according to the present invention, and FIG. 3 is a schematic cross-sectional view showing an insulated gate field effect transistor according to the present invention. FIG. 3 is a schematic cross-sectional view showing another example of a field effect transistor. In the figure, Q1, Q2, Q3, Q4 and Q5 are first, second, third, fourth and fifth semiconductor regions, I
is an insulating layer, MG, MD, MS and MB are conductive layers,
H indicates a groove, respectively.
Claims (1)
該第1の半導体領域に連接せる上記第1の半導体
領域に比し高い比抵抗を有し且第1の導電型を有
する第2の半導体領域と、上記第1の半導体領域
には連接せざるも上記第2の半導体領域に連接す
る第1の導電型とは逆の第2の導電型を有する第
3の半導体領域と、上記第1及び第2の半導体領
域には連接せざるも上記第3の半導体領域に連接
せる第1の導電型を有する第4の半導体領域と、
上記第3の半導体領域の上記第2及び第4の半導
体領域間の領域の表面上に絶縁層を介して配され
た導電性層とを具備し、上記第1及び第2の半導
体領域をドレイン領域、上記第4の半導体領域を
ソース領域、上記第3の半導体領域の上記第2及
び第4の半導体領域間の領域をチヤンネル形成用
領域、上記絶縁層をゲート用絶縁層、上記導電性
層をゲート電極とせる絶縁ゲート電界効果トラン
ジスタに於て、上記第1及び第4の半導体領域に
は連接せざるも上記第2の半導体領域の上記第1
及び第3の半導体領域間の領域及び上記第3の半
導体領域に連接せる上記第2の半導体領域に比し
高い比抵抗を有し且第2の導電型を有する第5の
半導体領域と、上記第2の半導体領域の上記第1
及び第3の半導体領域間の領域にその上記第5の
半導体領域の連接せざる側より上記第5の半導体
領域側にそれに達することなしに延長せる溝とを
有する事を特徴とする絶縁ゲート電界効果トラン
ジスタ。1 a first semiconductor region having a first conductivity type;
a second semiconductor region that is connected to the first semiconductor region and has a higher specific resistance than the first semiconductor region and has a first conductivity type; and a second semiconductor region that is not connected to the first semiconductor region. a third semiconductor region having a second conductivity type opposite to the first conductivity type, which is connected to the second semiconductor region; and a third semiconductor region which is not connected to the first and second semiconductor regions; a fourth semiconductor region having a first conductivity type connected to the third semiconductor region;
a conductive layer disposed on a surface of a region between the second and fourth semiconductor regions of the third semiconductor region with an insulating layer interposed therebetween; The fourth semiconductor region is a source region, the region between the second and fourth semiconductor regions of the third semiconductor region is a channel forming region, the insulating layer is a gate insulating layer, and the conductive layer In an insulated gate field effect transistor having a gate electrode, the first semiconductor region of the second semiconductor region is not connected to the first and fourth semiconductor regions.
and a fifth semiconductor region having a higher specific resistance than the region between the third semiconductor regions and the second semiconductor region connected to the third semiconductor region and having a second conductivity type; the first semiconductor region of the second semiconductor region;
and an insulated gate electric field characterized by having a groove in a region between the third semiconductor regions that can extend from the non-contiguous side of the fifth semiconductor region to the fifth semiconductor region without reaching it. effect transistor.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP9958480A JPS5724564A (en) | 1980-07-21 | 1980-07-21 | Insulated gate field effect transistor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP9958480A JPS5724564A (en) | 1980-07-21 | 1980-07-21 | Insulated gate field effect transistor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5724564A JPS5724564A (en) | 1982-02-09 |
| JPS641943B2 true JPS641943B2 (en) | 1989-01-13 |
Family
ID=14251141
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP9958480A Granted JPS5724564A (en) | 1980-07-21 | 1980-07-21 | Insulated gate field effect transistor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5724564A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4553151A (en) * | 1982-09-23 | 1985-11-12 | Eaton Corporation | Bidirectional power FET with field shaping |
-
1980
- 1980-07-21 JP JP9958480A patent/JPS5724564A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5724564A (en) | 1982-02-09 |
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