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JPS62589B2 - - Google Patents
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JPS62589B2 - - Google Patents

Info

Publication number
JPS62589B2
JPS62589B2 JP53002104A JP210478A JPS62589B2 JP S62589 B2 JPS62589 B2 JP S62589B2 JP 53002104 A JP53002104 A JP 53002104A JP 210478 A JP210478 A JP 210478A JP S62589 B2 JPS62589 B2 JP S62589B2
Authority
JP
Japan
Prior art keywords
region
layer
voltage
drain
resistance layer
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired
Application number
JP53002104A
Other languages
Japanese (ja)
Other versions
JPS5494886A (en
Inventor
Toshiaki Yamano
Katsumasa Fujii
Tetsuo Biwa
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.)
Sharp Corp
Original Assignee
Sharp Corp
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 Sharp Corp filed Critical Sharp Corp
Priority to JP210478A priority Critical patent/JPS5494886A/en
Publication of JPS5494886A publication Critical patent/JPS5494886A/en
Publication of JPS62589B2 publication Critical patent/JPS62589B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D84/00Integrated devices formed in or on semiconductor substrates that comprise only semiconducting layers, e.g. on Si wafers or on GaAs-on-Si wafers
    • H10D84/80Integrated devices formed in or on semiconductor substrates that comprise only semiconducting layers, e.g. on Si wafers or on GaAs-on-Si wafers characterised by the integration of at least one component covered by groups H10D12/00 or H10D30/00, e.g. integration of IGFETs
    • H10D84/811Combinations of field-effect devices and one or more diodes, capacitors or resistors
    • H10D84/817Combinations of field-effect devices and resistors only

Landscapes

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

Description

【発明の詳細な説明】 <梗概> 本発明は高耐圧の電界効果半導体装置の改良に
係る。
DETAILED DESCRIPTION OF THE INVENTION <Summary> The present invention relates to improvement of a high voltage field effect semiconductor device.

更に詳細には二重拡散型絶縁ゲート電界効果ト
ランジスタ(以下DSA MOS FETと称す)にお
いて、ピンチ抵抗を形成するN-層とベース領域
を形成するP層とを離して一定の間隔を置き、さ
らにN-層の濃度を適当に選んだ時に素子のゲー
トに正電圧を印加しても素子のオン状態における
耐圧が高いドレイン・ソース間電圧VDSに至らし
める事ができる。いいかえれば素子のオン状態に
おける電流飽和領域が高いVDSにおいても安定に
動作する特徴を持つ半導体装置を提供するもので
ある。
More specifically, in a double diffused insulated gate field effect transistor (hereinafter referred to as DSA MOS FET), the N - layer that forms the pinch resistance and the P layer that forms the base region are separated by a certain distance, and When the concentration of the N - layer is appropriately selected, even if a positive voltage is applied to the gate of the device, it is possible to reach a drain-source voltage V DS with a high withstand voltage in the on-state of the device. In other words, the present invention provides a semiconductor device that operates stably even at V DS where the current saturation region in the on-state of the element is high.

<先行技術> 従来より高い電圧でスイツチする必要のある容
量性素子等を駆動できる素子が要求されているが
容量性素子を駆動する場合、第1図に電圧電流特
性を示すように駆動素子のオン状態においてもオ
フ状態においても同じ電位が必要である。つまり
第2図に示すように、DSA MOS FET50に容
量負荷60が並列接続され、この並列回路に例え
ば抵抗のような電圧供給回路70を介して数100
ボルトの高電圧80を印加する回路にあつては、
DSA MOS FET50はオフ状態(VG=0)に
おいて、負荷60が高電圧80充電され、第1図
のa点に至り、次にDSA MOS FET50のオ
ン状態(VG>0)において、負荷に充電された
電荷が第1図のb点を通つて放電され、c点に至
るスイツチ動作をする。
<Prior art> There is a demand for an element that can drive capacitive elements that need to be switched at a higher voltage than conventional ones, but when driving a capacitive element, the voltage-current characteristics of the driving element are shown in Figure 1. The same potential is required in both the on and off states. In other words, as shown in FIG. 2, a capacitive load 60 is connected in parallel to the DSA MOS FET 50, and several 100 capacitive loads are connected to this parallel circuit via a voltage supply circuit 70 such as a resistor.
For a circuit that applies a high voltage of 80 volts,
When the DSA MOS FET 50 is in the off state (V G =0), the load 60 is charged to a high voltage 80, reaching point a in FIG. 1, and then when the DSA MOS FET 50 is in the on state (V G >0), the load The charged charge is discharged through point b in FIG. 1, and a switch operation is performed to reach point c.

以下図面を用いて従来装置の問題点を明らかに
する。
The problems of the conventional device will be explained below using the drawings.

従来の高耐圧DSA MOS FETは、第3図a〜
dに製造工程を示すように半導体基板1にはたと
えば低不純物濃度のP型基板を用い、その表面に
薄い絶縁物(たとえばSiO2)12を介して31P+
イオンをイオン注入技術を用いてN-ピンチ抵抗
層2を全表面に形成する(第3図a)。次に厚い
SiO23を基板1の表面に形成し、写真食刻技術
を用いて窓開けし、さらに薄いSiO2膜6を形成
した上でレジスト4で覆い部分的に窓開けしてイ
オン注入技術を用い、P型の実効チヤンネル領
域、すなわちベース領域5を形成する(第3図
b)。レジスト4及び薄いSiO2膜6を除去したの
ち、始めに開けた窓から拡散等によりN+型の不
純物層7,8を形成する。N+型領域の一部はド
レイン領域7になり他部はソース領域8になる
(第3図c)。最後にゲート領域を形成したあと
Al等の金属を蒸着等で形成し、不要な部分を除
去してドレイン電極9、ゲート電極10、ソース
電極11を形成する(第3図d)。素子はP−
P′を中心とした円環形状を形成している。
Conventional high-voltage DSA MOS FETs are shown in Figure 3a~
As shown in FIG. d, the semiconductor substrate 1 is, for example, a P-type substrate with a low impurity concentration, and 31 P + ions are implanted onto its surface through a thin insulator (for example, SiO 2 ) 12 using ion implantation technology. Then, an N -pinch resistance layer 2 is formed on the entire surface (FIG. 3a). the next thickest
SiO 2 3 is formed on the surface of the substrate 1, a window is opened using photolithography technology, a thin SiO 2 film 6 is further formed, and then a resist 4 is covered and a window is opened partially using ion implantation technology. , forming a P-type effective channel region, that is, a base region 5 (FIG. 3b). After removing the resist 4 and the thin SiO 2 film 6, N + type impurity layers 7 and 8 are formed by diffusion or the like through the first opened window. A part of the N + type region becomes the drain region 7 and the other part becomes the source region 8 (FIG. 3c). After finally forming the gate region
A metal such as Al is formed by vapor deposition or the like, and unnecessary portions are removed to form a drain electrode 9, a gate electrode 10, and a source electrode 11 (FIG. 3d). The element is P-
It forms an annular shape centered at P′.

この様にして形成されたNチヤンネル高耐圧−
DSA MOS FET−はドリフト領域全面に31P+
イオンが注入されてN-層2を形成しているた
め、ゲートに実効的なチヤンネルが形成される程
度に十分な電圧が印加された状態でドレインに正
の電圧が印加された時ベース領域P層5への空乏
層の伸びが著るしく、比較的低いドレイン電圧で
パンチスルーを起こしてしまう。これはベース領
域5の端部でN-ピンチ抵抗層2とP−N接合を
形成している上に互いに相殺してチヤンネル領域
で濃度勾配を形成していることによる。またN-
ピンチ抵抗層2を形成する際、比較的低濃度のイ
オン注入を行なうと、ドレインに電圧が印加され
るとすぐにN-ピンチ抵抗層2は空乏化され、一
度空乏化されてしまうと電荷の中性条件を満たさ
なければならない。すなわちドレイン領域7の
N+を空乏化しなければならなく、ドレイン領域
7が高濃度であるためベース領域5のP層が急激
に空乏化され、比較的低電圧でパンチスルーを起
こしてしまう。またN-ピンチ抵抗層2に高濃度
のイオン注入を行なうと、N-ピンチ抵抗層2は
空乏化されにくく、そのためドレイン電圧を吸収
しきれなく、ベース領域5のP層でのポテンシヤ
ルが高くなり、P層5への空乏化が促進され、そ
の結果、比較的低いドレイン電圧でパンチスルー
現象を起こすと考えられる。
N-channel high voltage withstand voltage formed in this way
In the DSA MOS FET-, 31 P + ions are implanted all over the drift region to form the N - layer 2, so a sufficient voltage is applied to the gate to form an effective channel. When a positive voltage is applied to the drain, the depletion layer extends significantly into the base region P layer 5, and punch-through occurs at a relatively low drain voltage. This is because a PN junction is formed with the N - pinch resistance layer 2 at the end of the base region 5, and a concentration gradient is formed in the channel region by canceling each other. Also N -
When forming the pinch resistance layer 2, if ion implantation is performed at a relatively low concentration, the N -pinch resistance layer 2 will be depleted as soon as a voltage is applied to the drain, and once depleted, the charge will be reduced. Neutrality conditions must be met. That is, the drain region 7
It is necessary to deplete N + , and since the drain region 7 has a high concentration, the P layer in the base region 5 is rapidly depleted, causing punch-through at a relatively low voltage. Furthermore, when a high concentration of ions is implanted into the N -pinch resistance layer 2, the N -pinch resistance layer 2 is difficult to be depleted and therefore cannot absorb the drain voltage completely, increasing the potential in the P layer of the base region 5. , depletion into the P layer 5 is promoted, and as a result, it is thought that a punch-through phenomenon occurs at a relatively low drain voltage.

<本発明の趣旨> 本発明は以上の考案に基づいて発明されたもの
であり、本発明はピンチ抵抗を形成するN-層と
ベース領域を形成するP層とを一定の間隔だけ離
すことを特徴とし、またN-層の濃度を適当に選
び、オン状態の耐圧を高めることを特徴とするも
のである。
<Purpose of the present invention> The present invention was invented based on the above idea, and the present invention is based on the above idea, and the present invention is to separate the N - layer forming the pinch resistance and the P layer forming the base region by a certain distance. Another feature is that the concentration of the N - layer is appropriately selected to increase the withstand voltage in the on state.

<発明の構成> 本発明はガラスマスクを一枚加えるだけで複雑
化させることなくかかる欠点を除去した高耐圧
MOS FETを提供するものである。以下に本発明
による一実施例の高耐圧MOS FETについて説明
する。
<Structure of the Invention> The present invention provides a high voltage withstand voltage that eliminates such drawbacks by simply adding a single glass mask without complicating the process.
It provides MOS FET. A high voltage MOS FET according to an embodiment of the present invention will be described below.

本発明の第1の要点はゲート絶縁層下の実効的
なチヤンネル部分P層5端部とN-ピンチ抵抗層
との間に間隔を設けること、第2の要点はN-
ンチ抵抗層への31P+のドーズ量を適切な値にする
ことである。
The first point of the present invention is to provide a space between the end of the effective channel portion P layer 5 under the gate insulating layer and the N - pinch resistance layer, and the second point is to provide a space between the end of the effective channel portion P layer 5 under the gate insulating layer and the N - pinch resistance layer. The goal is to set the dose of 31 P + to an appropriate value.

本発明による高耐圧MOS FETのプロセスを第
4図a〜dに示してあり従来例との違いを述べ
る。N-ピンチ抵抗層2を形成する31P+イオンを
半導体基板1に注入する際、予め薄いSiO212
を基板1の表面に形成しレジスト4を塗布し部分
的に開口する(第4図a)。この開口部よりSiO2
膜12を介して31P+イオンをイオン注入技術によ
つて注入し、N-ピンチ抵抗層2を形成する。イ
オン注入を行なう際にドーズ量を適当に選ばなけ
ればならない。
The process of the high voltage MOS FET according to the present invention is shown in FIGS. 4a to 4d, and the differences from the conventional example will be described. When implanting 31P + ions to form the N - pinch resistance layer 2 into the semiconductor substrate 1, a thin SiO 2 12
is formed on the surface of the substrate 1, a resist 4 is applied, and a portion is opened (FIG. 4a). SiO 2 from this opening
31 P + ions are implanted through the membrane 12 by ion implantation technique to form the N - pinch resistance layer 2 . When performing ion implantation, the dose must be appropriately selected.

次にレジスト4を除いて厚いSiO2膜3を基板
1の表面に形成し、写真食刻技術を用いて窓開け
する。窓開けする部分は、次に不純物をイオン注
入及び拡散して形成されるチヤンネル領域5と
N-ピンチ抵抗層2の端部とが間隔dを形成する
ようにする箇所である。上記SiO2膜3の上をレ
ジスト4で覆い、ベース領域5を形成する部分だ
け窓開けする。そしてイオン注入技術を用いて不
純物を注入し、P型の実効チヤンネル領域、すな
わち、ベース領域5を形成する(第4図b)。
Next, a thick SiO 2 film 3 is formed on the surface of the substrate 1 excluding the resist 4, and a window is opened using photolithography. The part to be opened is a channel region 5 formed by implanting and diffusing impurity ions.
This is a location where the end portion of the N -pinch resistance layer 2 forms a distance d. The SiO 2 film 3 is covered with a resist 4, and a window is opened only in the portion where the base region 5 is to be formed. Then, impurities are implanted using ion implantation technology to form a P-type effective channel region, that is, a base region 5 (FIG. 4b).

以下第4図c,dのプロセスは第3図c,dと
同じプロセスと同じになされる。
Hereinafter, the processes shown in FIGS. 4c and d are performed in the same manner as those shown in FIGS. 3c and d.

<発明の効果> 本発明による高耐圧DSA MOS FETはN-ピン
チ抵抗層2とベース領域P層5の間に間隔を取
り、基板1のπ層をこの間隔に設ける事により、
P層5方向への空乏層の拡がりを制限し、パンチ
スルー現象を生じにくくできる。第1図に示した
従来構造の場合、一定のゲート電圧、たとえばV
G=5Vを印加した状態での耐圧は375v程度である
が、本発明による素子では500v程度の耐圧を得
ることができる。さらにN-ピンチ抵抗層2とゲ
ート電極10との間に容量が内在しているがこの
容量を低減している。つまり入力容量が小さくな
る。しかしながら第4図bに示したdの値を大き
く取り過ぎるとイオン抵抗が増大する上に、ゲー
トに実効的なチヤンネルを形成するに必要な電圧
が印加された上でドレイン電圧を印加しても電流
が流れない状態、言い換えればオフセツト電圧を
生じてしまう。この事を考慮に入れると自ずから
dの範囲に制限が加えられ、本素子においてはド
レイン領域7、端部よりベース領域5までのドリ
フト領域の距離を30〜100μmとした場合、d=
5〜15μmとなる。ベース領域P層5とN-ピン
チ抵抗層2とが互いに相殺する事なくそれぞれ独
立に濃度が決定できる。さらに31P+イオンのドー
ズ量は7×1011/cm2〜2×1012/cm2が適切であ
る。
<Effects of the Invention> The high voltage DSA MOS FET according to the present invention has a space between the N -pinch resistance layer 2 and the base region P layer 5, and by providing the π layer of the substrate 1 at this space,
The spread of the depletion layer in the direction of the P layer 5 is restricted, making it difficult to cause punch-through phenomenon. In the conventional structure shown in FIG. 1, a constant gate voltage, e.g.
The breakdown voltage when G = 5V is applied is about 375V, but the element according to the present invention can obtain a breakdown voltage of about 500V. Furthermore, although there is a capacitance between the N - pinch resistance layer 2 and the gate electrode 10, this capacitance is reduced. In other words, the input capacity becomes smaller. However, if the value of d shown in Figure 4b is too large, the ionic resistance will increase, and even if the drain voltage is applied after the voltage necessary to form an effective channel is applied to the gate. A state in which no current flows, in other words, an offset voltage occurs. Taking this into consideration, a restriction is naturally placed on the range of d, and in this device, when the distance of the drift region from the drain region 7 and the end to the base region 5 is 30 to 100 μm, d=
It becomes 5 to 15 μm. The concentrations of the base region P layer 5 and the N - pinch resistance layer 2 can be determined independently without canceling each other out. Further, the appropriate dose of 31 P + ions is 7×10 11 /cm 2 to 2×10 12 /cm 2 .

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

第1図はMOS FETの出力静特性図の一例、第
2図はMOS FETの駆動回路図、第3図は従来プ
ロセスにおけるDSA・MOS・FETの一例を示す
断面図、第4図は本発明による高耐圧DSA・
MOS・FETの一実施例を示す断面図である。 1:サブストレイト領域、2:N-ピンチ抵抗
層、3:フイールド酸化膜、4:レジスト、5:
ベース領域、6:薄い酸化膜、7:ドレイン領
域、8:ソース領域、9:ドレイン電極、10:
ゲート電極、11:ソース電極。
Figure 1 is an example of an output static characteristic diagram of a MOS FET, Figure 2 is a drive circuit diagram of a MOS FET, Figure 3 is a cross-sectional view showing an example of a DSA/MOS/FET in a conventional process, and Figure 4 is a diagram of the present invention. High voltage DSA・
1 is a cross-sectional view showing an example of a MOS/FET. 1: Substrate region, 2: N - pinch resistance layer, 3: Field oxide film, 4: Resist, 5:
base region, 6: thin oxide film, 7: drain region, 8: source region, 9: drain electrode, 10:
Gate electrode, 11: source electrode.

Claims (1)

【特許請求の範囲】 1 1つの電導型を有するソース領域と、ドレイ
ン領域と、該ドレイン領域に連続し且つドレイン
領域より低い不純物濃度を有するピンチ抵抗層
と、他の電導型をもつ基板より高い不純物濃度を
有し且つドレインと対向するソース領域に接して
形成したチヤンネル領域とを備えてなる二重拡散
型絶縁ゲート電界効果トランジスタに於いて、 上記チヤンネル領域とピンチ抵抗層との間に間
隔を設けてなることを特徴とする高耐圧電界効果
半導体装置。
[Claims] 1. A source region and a drain region having one conductivity type, a pinch resistance layer continuous with the drain region and having an impurity concentration lower than that of the drain region, and a substrate having an impurity concentration higher than that of the other conductivity type. In a double diffused insulated gate field effect transistor comprising a channel region having an impurity concentration and formed in contact with a source region opposite to a drain, an interval is provided between the channel region and the pinch resistance layer. A high voltage field effect semiconductor device comprising:
JP210478A 1978-01-11 1978-01-11 High dielectric strength field effect semiconductor device Granted JPS5494886A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP210478A JPS5494886A (en) 1978-01-11 1978-01-11 High dielectric strength field effect semiconductor device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP210478A JPS5494886A (en) 1978-01-11 1978-01-11 High dielectric strength field effect semiconductor device

Publications (2)

Publication Number Publication Date
JPS5494886A JPS5494886A (en) 1979-07-26
JPS62589B2 true JPS62589B2 (en) 1987-01-08

Family

ID=11520028

Family Applications (1)

Application Number Title Priority Date Filing Date
JP210478A Granted JPS5494886A (en) 1978-01-11 1978-01-11 High dielectric strength field effect semiconductor device

Country Status (1)

Country Link
JP (1) JPS5494886A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4280855A (en) * 1980-01-23 1981-07-28 Ibm Corporation Method of making a dual DMOS device by ion implantation and diffusion

Also Published As

Publication number Publication date
JPS5494886A (en) 1979-07-26

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