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JPH0793431B2 - Method for manufacturing substrate of vertical conductivity modulation type MOSFET - Google Patents
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JPH0793431B2 - Method for manufacturing substrate of vertical conductivity modulation type MOSFET - Google Patents

Method for manufacturing substrate of vertical conductivity modulation type MOSFET

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Publication number
JPH0793431B2
JPH0793431B2 JP63080932A JP8093288A JPH0793431B2 JP H0793431 B2 JPH0793431 B2 JP H0793431B2 JP 63080932 A JP63080932 A JP 63080932A JP 8093288 A JP8093288 A JP 8093288A JP H0793431 B2 JPH0793431 B2 JP H0793431B2
Authority
JP
Japan
Prior art keywords
region
igbt
substrate
conductivity type
wafer
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
JP63080932A
Other languages
Japanese (ja)
Other versions
JPH01253279A (en
Inventor
勝典 上野
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.)
Fuji Electric Co Ltd
Original Assignee
Fuji Electric Co Ltd
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Filing date
Publication date
Application filed by Fuji Electric Co Ltd filed Critical Fuji Electric Co Ltd
Priority to JP63080932A priority Critical patent/JPH0793431B2/en
Publication of JPH01253279A publication Critical patent/JPH01253279A/en
Publication of JPH0793431B2 publication Critical patent/JPH0793431B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明はたて型の伝導度変調型MOSFET(以下これをIGBT
と略称する)に用いられるシリコン基板の製造する方法
に関する。
DETAILED DESCRIPTION OF THE INVENTION [Industrial application] The present invention relates to a vertical conductivity modulation type MOSFET (hereinafter referred to as an IGBT).
(Hereinafter abbreviated as ").

〔従来の技術〕[Conventional technology]

従来パワースイッチング素子としてたて型MOSFETやドレ
イン側にソースと逆導電型の領域を付加したIGBTが知ら
れており、IGBTはたて型MOSFETの高速スイッチング性と
バイポーラトランジスタの低インピーダンスを兼ね備え
た素子として注目されているものである。
Conventionally, as a power switching element, a vertical MOSFET and an IGBT in which a region of a conductivity type opposite to that of the source is added to the drain side are known. The IGBT is an element that combines the high-speed switching characteristics of the vertical MOSFET and the low impedance of a bipolar transistor. Has been attracting attention.

第6図はNチャネルのIGBTの部分断面図を示したもので
あり、IGBTの主要な構成部はコレクタのP+領域1、バッ
ファ層のN+領域2,ベース層のN-領域3,チャネルを形成す
るPベース領域4,P+エミッタ領域5,N+ソース領域6,チャ
ネル形成領域上にゲート酸化膜を介して形成されるポリ
シリコンゲート7,絶縁膜8およびソース電極9である。
このIGBTはP+コレクタ領域1,N-ベース領域3,Pベース領
域4からなるPNPトランジスタのベースにNチャネルMOS
FETから電流を供給して動作させるものである。
Fig. 6 shows a partial cross-sectional view of an N-channel IGBT. The main components of the IGBT are the P + region 1 of the collector, the N + region 2 of the buffer layer, the N - region 3 of the base layer, and the channel. A P base region 4, a P + emitter region 5, an N + source region 6, a polysilicon gate 7 formed on the channel forming region via a gate oxide film, an insulating film 8 and a source electrode 9.
This IGBT has an N channel MOS at the base of a PNP transistor composed of P + collector region 1, N base region 3 and P base region 4.
It is operated by supplying current from the FET.

第7図はIGBTのシリコン基板の部分のみを抽出して示し
た部分断面図であり、第6図と共通部分を同一符号で表
わしてある。すなわち、第7図のようにIGBTのシリコン
基板10はP+領域1(コレクタ),N+領域2(バッファ
層),N-領域3(ベース層)からなり、この基板10を製
造するには従来エピタキシャル成長法により行なわれて
いる。まずコレクタ領域となるP+領域1は低抵抗のP型
CZシリコンウエハを用い、この上にバッファ層となるN+
領域2,さらにベース層となるN-領域3を順次エピタキシ
ャル成長により堆積し形成する。基板10の主な部分の厚
さは例えば第1表のごとくである。
FIG. 7 is a partial cross-sectional view showing only the portion of the silicon substrate of the IGBT, and common portions with FIG. 6 are represented by the same symbols. That is, as shown in FIG. 7, the silicon substrate 10 of the IGBT is composed of P + region 1 (collector), N + region 2 (buffer layer), and N region 3 (base layer). Conventionally, it is performed by the epitaxial growth method. First, the P + region 1 which is the collector region is a low resistance P type
A CZ silicon wafer is used, and a buffer layer N + is formed on top of this.
Region 2 and N region 3 to be a base layer are sequentially deposited by epitaxial growth to form. The thickness of the main part of the substrate 10 is, for example, as shown in Table 1.

また比抵抗はN+領域2は0.1〜0.2Ωcm、N-領域3が数10
〜100Ωcmである。エピタキシャル成長法は厚さの制御
性が良好で濃度勾配の急激な接合を得ることができる。
エピタキシャル成長法で製造されるシリコン基板の不純
物濃度分布は接合部で階段状に変化するという特徴をも
っている。
The specific resistance of N + region 2 is 0.1 to 0.2 Ωcm, and that of N region 3 is several tens.
~ 100 Ωcm. The epitaxial growth method has good thickness controllability and can obtain a junction with a sharp concentration gradient.
The impurity concentration distribution of the silicon substrate manufactured by the epitaxial growth method is characterized in that it changes stepwise at the junction.

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

以上のごとく、IGBTに用いるシリコン基板はエピタキシ
ャル成長法により製造されている。しかしながらエピタ
キシャル成長法は高度な技術を要し、とくに厚いエピタ
キシャル層を積むときは結晶の欠陥を生じやすく歩留り
を著しく低下させる上に、エピタキシャル成長装置自体
が甚だ高価であって、大量処理を行なうのが容易でな
く、したがってシリコン基板のコストも高価なものとな
り、最終的に得られるIGBTは価格が高くなるのを避ける
ことができない。
As described above, the silicon substrate used for the IGBT is manufactured by the epitaxial growth method. However, the epitaxial growth method requires a high level of technology, crystal defects are liable to occur, especially when a thick epitaxial layer is stacked, and the yield is significantly reduced, and the epitaxial growth apparatus itself is extremely expensive, making it easy to perform large-scale processing. Therefore, the cost of the silicon substrate is also high, and the price of the finally obtained IGBT cannot be avoided.

本発明は上述の点に鑑みてなされたものであり、その目
的はIGBT用のシリコン基板をエピタキシャル成長法に代
って安価で容易な基板の製造方法を提供することにあ
る。
The present invention has been made in view of the above points, and an object thereof is to provide an inexpensive and easy substrate manufacturing method in place of an epitaxial growth method for a silicon substrate for an IGBT.

〔課題を解決するための手段〕[Means for Solving the Problems]

本発明はシリコン基板中に必要な各導電型の領域を全て
不純物拡散工程により形成するものであり、次のように
して行なう。
The present invention forms all required conductivity type regions in a silicon substrate by an impurity diffusion process, and is performed as follows.

まず所定の厚さを有するN型シリコン板の両面からN型
不純物を拡散し、次いでP型不純物を拡散して両表面か
ら所の深さまでをP型領域、さらにこのP型領域から60
〜90μmの深さまでをN型シリコン板よりN型不純物濃
度の高い領域とする5層からなるシリコン板として形成
した後、このシリコン板を一方の表面から所定の厚さと
なるまで研削除去することにより、残余のP型領域,高
不純物濃度N型領域およびN型領域からなるシリコン板
を作製し、これをIGBTの基板とするものである。
First, N-type impurities are diffused from both sides of an N-type silicon plate having a predetermined thickness, and then P-type impurities are diffused to form a P-type region from both surfaces to a certain depth.
By forming a silicon plate consisting of 5 layers up to a depth of up to 90 μm as a region where the N-type impurity concentration is higher than that of the N-type silicon plate, the silicon plate is ground and removed from one surface to a predetermined thickness. , A remaining P-type region, a high-impurity concentration N-type region, and an N-type region are produced, and this is used as the substrate of the IGBT.

〔作用〕[Action]

本発明の方法により得られるIGBT用シリコン基板は拡散
法を用いているために、エピタキシャル成長法によるシ
リコン基板とは不純物濃度分布の形が異なり、IGBTの特
性上は同じターンオフ時間で電圧降下は本発明による基
板を用いたものの方が従来素子よりやや高く、そのため
拡散法の基板に対してはN+領域すなわちバッファ層をか
なり厚くし、N-領域すなわちベース層の厚さを減らすこ
とによりエピタキシャル基板とほぼ同等の特性を与える
ことができる。
Since the silicon substrate for the IGBT obtained by the method of the present invention uses the diffusion method, the shape of the impurity concentration distribution is different from that of the silicon substrate by the epitaxial growth method, and the voltage drop of the present invention is the same at the same turn-off time due to the characteristics of the IGBT. The substrate using the substrate according to (1) is slightly higher than the conventional device, so that for the substrate of the diffusion method, the N + region, that is, the buffer layer is made considerably thicker, and the thickness of the N region, that is, the base layer is reduced to form an epitaxial substrate. It is possible to give almost the same characteristics.

〔実施例〕〔Example〕

第1図は本発明の方法によるシリコン基板の製造工程を
示したものであり、第1図では製造工程順とそれに対応
してシリコンウエハ内に形成される各導電型の領域をウ
エハの断面図として並列に記してある。
FIG. 1 shows a manufacturing process of a silicon substrate according to the method of the present invention. FIG. 1 is a cross-sectional view of the manufacturing process sequence and regions of each conductivity type formed in the silicon wafer corresponding to the manufacturing process order. Are written in parallel as.

第1図においてまずIGBTの耐圧から決まる抵抗を有する
N-シリコンの結晶の引き上げを行いN-領域3(第7図)
となるシリコン板を得る(a)。結晶引き上げは高抵抗
が得やすく抵抗の制御性のよいFZ法により行なう。次に
このシリコン板の両面からPOCl3等を用いてバッファ層
となるN+領域2(第7図)を形成する拡散を行なう
(b)。次いで両面からコレクタとなるP+領域1(第7
図)を形成する拡散を行なう(c)。このようにして第
1図のようにN-領域3を中心に厚さ方向に対称的なN+,P
+領域をもつ5層からなるシリコン板を得ることができ
る。最後にこれを一方の表面から厚さ方向にN-領域3が
所定の厚さとなるまで研削除去することにより、第7図
と同様のシリコン基板10が完成する(d)。
In Fig. 1, first, it has a resistance determined by the breakdown voltage of the IGBT.
N - silicon crystal is pulled up and N - region 3 (Fig. 7)
A silicon plate is obtained (a). Crystal pulling is performed by the FZ method, which easily obtains high resistance and has good controllability of resistance. Next, diffusion is performed from both sides of this silicon plate using POCl 3 or the like to form an N + region 2 (FIG. 7) to be a buffer layer (b). Next, P + region 1 (7th
(D) is performed to form (c). Thus, as shown in FIG. 1, N + , P symmetrical about the N region 3 in the thickness direction is formed.
It is possible to obtain a silicon plate composed of 5 layers having + regions. Finally, this is ground and removed from one surface in the thickness direction until the N region 3 has a predetermined thickness, whereby a silicon substrate 10 similar to that shown in FIG. 7 is completed (d).

以上のようにして、熱拡散と研削で製造したIGBT用基板
の模式的な不純物濃度分布を第2図に示す。第2図のご
とく熱拡散により得られら基板の不純物濃度分布はN+
域2(バッファ層)およびP+領域1(コレクタ領域)が
ガウス分布を呈しており、この点接合部が階段状となっ
ているエピタキシャル成長法による基板とは不純物の分
布状態が異なる。
FIG. 2 shows a schematic impurity concentration distribution of the IGBT substrate manufactured by thermal diffusion and grinding as described above. As shown in FIG. 2, the impurity concentration distribution of the substrate obtained by thermal diffusion shows a Gaussian distribution in the N + region 2 (buffer layer) and P + region 1 (collector region), and this point junction has a stepwise shape. The state of impurity distribution is different from that of the substrate obtained by the epitaxial growth method.

そのために拡散ウエハを用いたIGBTはエピタキシャルウ
エハを用いたIGBTとは特性上の違いを生ずる。それはIG
BTの主要な特性である一定の電流を流したときの電圧降
下(Von)とターンオフ時のスイッチングスピート(t
off)との関係(以下これをトレードオフと称する)で
ある。第3図はこのトレードオフを拡散ウエハとエピタ
キシャルウエハとの比較で示した模式的な線図である。
第3図において、曲線(イ)は拡散法,曲線(ロ)はエ
ピタキシャル法によるウエハの場合であり、拡散法では
バッファ層となるN+領域2の厚さを30μmとしてIGBTを
試作したものである。IGBTはVonが低くtoffが短いもの
が要求されるから、第3図のトレードオフ曲線から、拡
散ウエハの方がエピタキシャルウエハより全体的にトレ
ードオフガ劣ることがわかる。すなわち、同じターンオ
フ時間に対して拡散ウエハの方がオン電圧が高くなる。
第3図の曲線(ハ)については後述する。
Therefore, the IGBT using the diffusion wafer has a characteristic difference from the IGBT using the epitaxial wafer. It is IG
The main characteristics of BT are the voltage drop (V on ) when a constant current is applied and the switching speed (t
off ) (hereinafter referred to as a trade-off). FIG. 3 is a schematic diagram showing this trade-off in comparison between a diffusion wafer and an epitaxial wafer.
In FIG. 3, the curve (a) is for the wafer by the diffusion method and the curve (b) is for the wafer by the epitaxial method. In the diffusion method, the thickness of the N + region 2 to be the buffer layer is 30 μm is there. Since the IGBT is required to have a low V on and a short t off, it can be seen from the trade-off curve in FIG. 3 that the diffusion wafer is generally inferior to the epitaxial wafer in trade-off. That is, the on-voltage is higher in the diffusion wafer for the same turn-off time.
The curve (c) in FIG. 3 will be described later.

拡散ウエハの方がエピタキシャルウエハよりVonが高く
なる原因としてこの試作IGBTに用いたシリコン基板の第
2図におけるN+領域2のピーク濃度NbがN+領域2の厚さ
dN=30μmのときに十分に大きくないことが挙げられ
る。エピタキシャルウエハはバッファ層となるN+領域2
の不純物濃度と厚さは別のパラメータとして結晶成長時
に個別に設定することができる。ところが拡散ウエハで
はこれらをそれぞれ単独に設定することができず、不純
物濃度と厚さに一定の関係をもっている。第4図は拡散
の実験によるNbはdNの関係を示した線図である。第4図
のように拡散法ではNbはdNの増加ととも急激に増大す
る。そこで本発明者はバッファ層の厚さをパラメータと
しIGBT用の拡散ウエハを作製し、これを用いて素子を試
作した結果、バッファ層が厚くなるとトレードオフの関
係は第3図の点線の曲線(ハ)のようになり、曲線
(ロ)すなわちエピタキシャルウエハを用いた場合に近
づくことがわかった。
Peak concentration N b N + region 2 in Figure 2 the thickness of the N + region 2 of the silicon substrate used in this trial IGBT causes for better diffusion wafer becomes higher V on than the epitaxial wafer
The reason is that it is not sufficiently large when d N = 30 μm. Epitaxial wafer is N + region 2 which becomes the buffer layer
The impurity concentration and the thickness of can be set individually as separate parameters during crystal growth. However, in the diffusion wafer, these cannot be set independently, and there is a fixed relationship between the impurity concentration and the thickness. FIG. 4 is a diagram showing the relationship between N b and d N in the diffusion experiment. As shown in Fig. 4, in the diffusion method, N b increases rapidly with the increase of d N. Therefore, the present inventor produced a diffusion wafer for IGBT using the thickness of the buffer layer as a parameter and prototyped an element using this, and as a result, as the buffer layer becomes thicker, the trade-off relationship is shown by the dotted line curve ( It was found that the result becomes as shown in (c) and approaches the curve (b), that is, the case of using an epitaxial wafer.

一定のtoffをもつ素子について、dNとVonの関係を求め
ると第5図の線図が得られる。第5図の点線はエピタキ
シャルウエハを基板としたIGBTを表わし、一部点線の実
線曲線が本発明による拡散ウエハを基板としたIGBTを表
わしている。第5図からわかるように拡散ウエハはdN
60〜90μmの範囲でVonが低下するようになり、Vonの改
善が見られる。しかし、この程度ではまだオン電圧はエ
ピタキシャルウエハより拡散ウエハの方が高く、トレー
ドオフがやや劣る。
When the relationship between d N and V on is obtained for a device having a constant t off , the diagram of FIG. 5 is obtained. The dotted line in FIG. 5 represents an IGBT using an epitaxial wafer as a substrate, and a partially dotted solid curve represents an IGBT using a diffusion wafer according to the present invention as a substrate. As can be seen from FIG. 5, d N of the diffusion wafer is
In the range of 60 to 90 μm, V on starts to decrease, and V on is improved. However, at this level, the on-voltage is still higher in the diffusion wafer than in the epitaxial wafer, and the trade-off is slightly inferior.

これに対しては次のようにすることができる。エピタキ
シャルウエハは前述のように接合部で階段状に変化する
不純物濃度分布曲線をもっているので、耐圧は純粋にベ
ース層となるN-領域の厚さで決まるが、拡散ウエハは第
2図のような不純物濃度分布曲線となっているから、そ
の耐圧はN-領域のほかに、バッファ層となるN+領域のN-
領域側の不純物濃度の低い所も寄与している。したがっ
て拡散ウエハのN-領域はエピタキシャルウエハより約1
割厚さを減らすことができる。N-領域の厚さを約1割少
なくすると、エピタキシャルウエハを基板に用いたとき
もIGBTのトレードオフの関係はさらに改善され、第5図
の曲線を全体的に下方に移動することができ、最適な位
置がエピタキシャルウエハの場合とほぼ同等になる。
This can be done as follows. Since the epitaxial wafer has the impurity concentration distribution curve that changes stepwise at the junction as described above, the breakdown voltage is purely determined by the thickness of the N region that serves as the base layer, but the diffusion wafer is as shown in FIG. because it becomes impurity concentration distribution curve, the breakdown voltage the N - well region, the N + region serving as a buffer layer N -
The low impurity concentration on the region side also contributes. Therefore, the N - region of the diffusion wafer is about 1
The thickness can be reduced. When the thickness of the N region is reduced by about 10%, the IGBT trade-off relationship is further improved even when an epitaxial wafer is used as a substrate, and the curve in FIG. 5 can be moved downward as a whole. The optimum position is almost the same as that of the epitaxial wafer.

以上本発明をNチャネルIGBTについて説明してきたが、
本発明の方法は各半導体領域の導電型を逆にしたPチャ
ネル素子に対しても原理的に適用し得るものである。
Although the present invention has been described with respect to the N-channel IGBT,
The method of the present invention can be applied in principle to a P-channel device in which the conductivity type of each semiconductor region is reversed.

〔発明の効果〕〔The invention's effect〕

NチャネルIGBTに用いるシリコン基板としてエピタキシ
ャル成長法により堆積したシリコンウエハの代りに、本
発明では実施例で述べた如く、まずN-シリコンウエハを
用意してその両面からN型不純物を熱拡散してN+領域を
形成し、さらに両面からP型不純物を熱拡散してP+領域
を形成した後、一方の両面から厚さ方向の所定に厚さと
なるまで研削除去した残部のシリコンウエハを基板とし
て用いるようにしたため、エピタキシャルウエハでは高
度な技術を要する上に、設備費などの点からも得られる
IGBT素子が高価なものとなるのに対して、安価で製造の
容易な基板を実現することができる。また拡散ウエハと
エピタキシャルウエハとの不純物濃度分布の相違による
素子のトレードオフ特性の低下についてもバッファ層と
なるN+領域の拡散深さをエピタキシャルウエハの場合よ
り大きくし60〜90μmとすることや、ベース層となるN-
領域の厚さを減らすことにより解決される。
Instead of a silicon wafer deposited by an epitaxial growth method as a silicon substrate used for an N-channel IGBT, in the present invention, as described in the embodiment, first, an N - silicon wafer is prepared and N-type impurities are thermally diffused from both surfaces thereof to form an N-type impurity. A + region is formed, P-type impurities are thermally diffused from both sides to form a P + region, and then the remaining silicon wafer is ground and removed from one side to a predetermined thickness in the thickness direction and is used as a substrate. As a result, the epitaxial wafer requires advanced technology and can be obtained from the viewpoint of equipment cost.
While the IGBT element is expensive, it is possible to realize a substrate that is inexpensive and easy to manufacture. Regarding the deterioration of the element trade-off characteristics due to the difference in impurity concentration distribution between the diffusion wafer and the epitaxial wafer, the diffusion depth of the N + region serving as the buffer layer should be made larger than that of the epitaxial wafer to be 60 to 90 μm. N serving as a base layer -
The solution is to reduce the thickness of the area.

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

第1図は本発明の方法によるシリコン基板の製造工程
図、第2図は本発明の方法により得られるシリコン基板
の不純物濃度分布を模式的に示した線図、第3図は本発
明の方法により得られるシリコン基板を用いたIGBTと従
来のエピタキシャルウエハのシリコン基板を用いたIGBT
との比較で示した模式的なトレードオフ特性線図、第4
図は拡散実験におけるN+領域の不純物ピーク濃度(Nb
と厚さ(dN)との関係を表わす線図、第5図は一定のタ
ーンオフ時間をもつIGBT素子について基板のN+領域の厚
さ(dN)とオン電圧(Von)との関係を表わす線図、第
6図はIGBTの要部構成断面図、第7図は同じく基板のみ
の部分断面図である。 1:P+領域、2:N+領域、3:N-領域。
FIG. 1 is a manufacturing process diagram of a silicon substrate by the method of the present invention, FIG. 2 is a diagram schematically showing an impurity concentration distribution of a silicon substrate obtained by the method of the present invention, and FIG. 3 is a method of the present invention. IGBT using the silicon substrate obtained by the method and the conventional IGBT using the silicon substrate of the epitaxial wafer
Schematic trade-off characteristic diagram shown in comparison with
The figure shows the impurity peak concentration (N b ) in the N + region in the diffusion experiment.
Preparative thick (d N) and a line diagram showing the relationship, FIG. 5 is the relationship between the thickness of the substrate of the N + region for the IGBT element having a constant turn-off time (d N) and on-voltage (V on) FIG. 6 is a cross-sectional view of the essential parts of the IGBT, and FIG. 7 is a partial cross-sectional view of the substrate only. 1: P + region, 2: N + region, 3: N region.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】たて型の伝導度変調型MOSFETのシリコン基
板を製造する方法であって、まず所定の厚さを有する第
1導電型シリコン板の両面から第1導電型不純物を拡散
し、次いで第2導電型不純物を拡散して、両表面から所
定の深さまでを第2導電型領域、さらにこの第2導電型
領域から60〜90μmの深さまでを前記第1導電型シリコ
ン板より第1導電型不純物濃度の高い領域とする5層か
らなるシリコン板として形成した後、このシリコン板を
一方の表面から所定の厚さとなるまで研削除去すること
により、残余の第2導電型領域,高不純物濃度第1導電
型領域および第1導電型領域からなるシリコン板を基板
とすることを特徴とするたて型伝導度変調型MOSFETの基
板の製造方法。
1. A method of manufacturing a silicon substrate of a vertical conductivity modulation type MOSFET, which comprises first diffusing first conductivity type impurities from both sides of a first conductivity type silicon plate having a predetermined thickness, Then, impurities of the second conductivity type are diffused to form a second conductivity type region from both surfaces to a predetermined depth, and a first conductivity type silicon plate to a depth of 60 to 90 μm from the second conductivity type region. After forming a silicon plate composed of five layers to be a region having a high conductivity type impurity concentration, the silicon plate is ground and removed from one surface to a predetermined thickness to remove the remaining second conductivity type region and high impurities. A method of manufacturing a substrate of a vertical conductivity modulation type MOSFET, characterized in that a silicon plate composed of a concentration first conductivity type region and a first conductivity type region is used as a substrate.
JP63080932A 1988-04-01 1988-04-01 Method for manufacturing substrate of vertical conductivity modulation type MOSFET Expired - Lifetime JPH0793431B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63080932A JPH0793431B2 (en) 1988-04-01 1988-04-01 Method for manufacturing substrate of vertical conductivity modulation type MOSFET

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63080932A JPH0793431B2 (en) 1988-04-01 1988-04-01 Method for manufacturing substrate of vertical conductivity modulation type MOSFET

Publications (2)

Publication Number Publication Date
JPH01253279A JPH01253279A (en) 1989-10-09
JPH0793431B2 true JPH0793431B2 (en) 1995-10-09

Family

ID=13732218

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Application Number Title Priority Date Filing Date
JP63080932A Expired - Lifetime JPH0793431B2 (en) 1988-04-01 1988-04-01 Method for manufacturing substrate of vertical conductivity modulation type MOSFET

Country Status (1)

Country Link
JP (1) JPH0793431B2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH08288503A (en) * 1995-04-11 1996-11-01 Rohm Co Ltd Semiconductor device having planar type high breakdown voltage vertical element and manufacturing method thereof
DE19860581A1 (en) * 1998-12-29 2000-07-06 Asea Brown Boveri Semiconductor device and manufacturing method

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS57194583A (en) * 1981-05-27 1982-11-30 Hitachi Ltd Mos semiconductor device and manufacture thereof

Also Published As

Publication number Publication date
JPH01253279A (en) 1989-10-09

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