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JPH0217939B2 - - Google Patents
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JPH0217939B2 - - Google Patents

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Publication number
JPH0217939B2
JPH0217939B2 JP59121800A JP12180084A JPH0217939B2 JP H0217939 B2 JPH0217939 B2 JP H0217939B2 JP 59121800 A JP59121800 A JP 59121800A JP 12180084 A JP12180084 A JP 12180084A JP H0217939 B2 JPH0217939 B2 JP H0217939B2
Authority
JP
Japan
Prior art keywords
layer
junction
main surface
gto
diffusion
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
JP59121800A
Other languages
Japanese (ja)
Other versions
JPS612364A (en
Inventor
Yoshio Terasawa
Saburo Oikawa
Tsutomu Yao
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.)
Hitachi Ltd
Original Assignee
Hitachi 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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP59121800A priority Critical patent/JPS612364A/en
Publication of JPS612364A publication Critical patent/JPS612364A/en
Publication of JPH0217939B2 publication Critical patent/JPH0217939B2/ja
Granted legal-status Critical Current

Links

Classifications

    • 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
    • H10D62/17Semiconductor regions connected to electrodes not carrying current to be rectified, amplified or switched, e.g. channel regions
    • H10D62/192Base regions of thyristors
    • H10D62/206Cathode base regions of thyristors

Landscapes

  • Bipolar Transistors (AREA)
  • Thyristors (AREA)

Description

【発明の詳細な説明】 〔発明の利用分野〕 本発明は半導体装置に係り、特に、トランジス
タ、ゲートターンオフサイリスタ等の自己消弧型
スイツチング半導体装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Application of the Invention] The present invention relates to semiconductor devices, and particularly to self-extinguishing switching semiconductor devices such as transistors and gate turn-off thyristors.

この種の半導体装置では半導体基体におけるキ
ヤリアをゲート電極(トランジスタではベース電
極)から引抜いてターンオフ動作を行つている。
そこで、ゲートターンオフサイリスタ(以下
GTOと略記)を例にとつて詳細に説明する。第
1図はGTOを構成する半導体基体1の部分的断
面図で隣接相互で導電型が順次異なる4個の半導
体層、即ち、pE層2、nB層3、pB層4、nE層5を
有し、pB層4とnE層5が作るpn接合Jは半導体基
体1の上主表面に露出したプレーナ接合構造とな
つている。通常nE層5は短冊状に分割されるか、
櫛歯状になつている。第1図では短冊状のnE層5
を幅方向で切断して示している。半導体基体1の
下主表面のpE層2にはアノード電極6、上主表面
のpB層4にはnE層5を取囲むようにゲート電極
7、そしてnE層5にはカソード電極8がそれぞれ
低抵抗接触されている。ゲート、カソード電極
7,8以外の上主表面には表面安定化膜が設けら
れているのが第1図では省略されている。
In this type of semiconductor device, a turn-off operation is performed by extracting carriers in a semiconductor substrate from a gate electrode (base electrode in a transistor).
Therefore, gate turn-off thyristor (hereinafter referred to as
This is explained in detail using GTO (abbreviated as GTO) as an example. FIG. 1 is a partial cross-sectional view of a semiconductor substrate 1 constituting a GTO, and shows four adjacent semiconductor layers having sequentially different conductivity types: p E layer 2, n B layer 3, p B layer 4, n E The pn junction J formed by the pB layer 4 and the nE layer 5 has a planar junction structure exposed on the upper main surface of the semiconductor substrate 1. Usually the nE layer 5 is divided into strips or
It has a comb-like shape. In Figure 1, the strip-shaped n E layer 5
is shown cut in the width direction. The pE layer 2 on the lower main surface of the semiconductor substrate 1 has an anode electrode 6, the pB layer 4 on the upper main surface has a gate electrode 7 surrounding the nE layer 5, and the nE layer 5 has a cathode electrode. 8 are connected to each other with low resistance. A surface stabilizing film provided on the upper main surface other than the gate and cathode electrodes 7 and 8 is omitted in FIG.

ターンオフ時にはpn接合Jに逆バイアス電圧
を印加し、アノード電極6からカソード電極8に
向つて流れている電流iAを点線で示すようにゲー
ト電極7から引抜く。この場合、nE層5直下にお
けるpB層4の横方向抵抗RPBが大きいとpB層4に
おける電圧降下iA×RPBが大きくなり、ターンオ
フ時に電流が集中するnE層5中央部のpn接合J
が順バイアス状態となり、この部分でGTOはタ
ーンオンしてしまい、ターンオフ失敗に至る。タ
ーンオフ失敗を避けるために、横方向抵抗RPB
減少すべく、pB層4の不純物濃度を高くしてい
る。特にpB層4は不純物拡散で作られることが多
く、そのため、pB層4の表面不純物濃度は約5×
1017〜2×1018atoms/c.c.とかなり高くなつてい
る。この結果、pn接合Jの耐圧は低く、市販さ
れているGTOでゲート耐圧は約10〜20V程度で
ある。このようなゲート耐圧では大きな電流を速
くターンオフすることが困難である。ゲート耐圧
を高くする方法としてpB層4あるいはnE層5をエ
ピタキシヤル技術を用いて形成する方法があるが
この方法によれば製作コストが高いものとなる。
At turn-off, a reverse bias voltage is applied to the pn junction J, and the current i A flowing from the anode electrode 6 toward the cathode electrode 8 is drawn out from the gate electrode 7 as shown by the dotted line. In this case, if the lateral resistance R PB of the p B layer 4 directly under the n E layer 5 is large, the voltage drop i A ×R PB in the p B layer 4 will increase, and the current will concentrate at the center of the n E layer 5 at turn-off. p-n junction J
becomes a forward bias state, and the GTO turns on in this part, leading to turn-off failure. In order to avoid turn-off failure, the impurity concentration of the pB layer 4 is increased to reduce the lateral resistance RPB . In particular, the p B layer 4 is often created by impurity diffusion, so the surface impurity concentration of the p B layer 4 is approximately 5×
It is quite high at 10 17 to 2×10 18 atoms/cc. As a result, the pn junction J has a low breakdown voltage, and the gate breakdown voltage of commercially available GTOs is about 10 to 20V. With such a gate breakdown voltage, it is difficult to quickly turn off a large current. One method of increasing the gate breakdown voltage is to form the p B layer 4 or the n E layer 5 using epitaxial technology, but this method results in high manufacturing costs.

〔発明の目的〕[Purpose of the invention]

本発明の目的は低い製作コストで高いゲート耐
圧を持つ自己消弧型スイツチング半導体装置を提
供するにある。
SUMMARY OF THE INVENTION An object of the present invention is to provide a self-extinguishing switching semiconductor device that has a high gate breakdown voltage at a low manufacturing cost.

〔発明の概要〕[Summary of the invention]

上記目的を達成する本発明の特徴とするところ
は拡散マスクを用いてpB層が形成され、この時で
きる拡散マスク下の不純物濃度の低い横方向拡散
領域内にnE層とpB層が作るpn接合の端部が形成さ
れ、半導体基体の主表面に露出されていることに
ある。
A feature of the present invention that achieves the above object is that a p B layer is formed using a diffusion mask, and an n E layer and a p B layer are formed in a lateral diffusion region with a low impurity concentration under the diffusion mask. The end of the pn junction is formed and exposed on the main surface of the semiconductor body.

〔発明の実施例〕[Embodiments of the invention]

以下、本発明を図面に示した一実施例に従つて
説明する。
Hereinafter, the present invention will be explained according to an embodiment shown in the drawings.

第2図は第1図と同様GTOの一部の半導体基
体11を示している。半導体基体11はpE層1
2、nB層13、pB層14そしてnE層15を有し、
pE層12にアノード電極16、pB層14にゲート
電極17、nE層15にカソード電極18が低抵抗
接触している。この半導体基体11は次のように
して作られる。即ち、n型導電性の半導体基体1
1が用意され、下主表面には拡散マスクを設け
ず、上主表面には図中L記号で示す幅の拡散マス
ク(図示せず)を設ける。次にp型不純物を上下
両主表面から拡散する。p型不純物としてボロン
を用いる場合、拡散マスクとしてシリコン酸化膜
を用いる。pE層12は平坦に形成され、pB層14
は図示の如く拡散マスクの両側から不純物が横方
向に拡散して連続したものとなつている。図に点
線で示す領域内は横方向拡散により連続した部分
である。次に、横方向拡散で形成されたpB層部分
でpn接合Jの端部即ちpn接合の主表面と平行を
なす部分と主表面とを連結する部分が位置するよ
うにn型不純物を拡散しnE層15を形成する。そ
して、最後に、各電極16〜18となる金属を設
ける。
Similar to FIG. 1, FIG. 2 shows a part of the semiconductor substrate 11 of the GTO. The semiconductor substrate 11 has a pE layer 1
2, having an n B layer 13, a p B layer 14 and an n E layer 15,
An anode electrode 16 is in low resistance contact with the pE layer 12, a gate electrode 17 is in contact with the pB layer 14, and a cathode electrode 18 is in low resistance contact with the nE layer 15. This semiconductor substrate 11 is manufactured as follows. That is, the semiconductor substrate 1 with n-type conductivity
1 is prepared, no diffusion mask is provided on the lower main surface, and a diffusion mask (not shown) having a width indicated by the symbol L in the figure is provided on the upper main surface. Next, p-type impurities are diffused from both the upper and lower main surfaces. When boron is used as the p-type impurity, a silicon oxide film is used as a diffusion mask. The p E layer 12 is formed flat, and the p B layer 14
As shown in the figure, impurities are diffused in the lateral direction from both sides of the diffusion mask and are continuous. The area indicated by the dotted line in the figure is a continuous portion due to lateral diffusion. Next, in the p B layer portion formed by lateral diffusion, an n-type impurity is diffused so that the end of the pn junction J, that is, the part that connects the main surface with the part parallel to the main surface of the pn junction, is located. Then, an E layer 15 is formed. Finally, a metal serving as each electrode 16 to 18 is provided.

以上の構成のGTOでは、nE層15直下におけ
るpB層14の横方向抵抗RPBは第1図に示すもの
と同程度に低い。さらに上主表面に露出している
pn接合近傍では横方向拡散のためpB層の不純物
濃度が低いので、pn接合の耐圧を高くできる。
第3図は拡散マスク端から拡散マスク内側への横
方向距離y(第2図参照)と表面不純物濃度の関
係の一例を示しており、拡散マスクで覆われなか
つた部分の表面不純物濃度を2×1018atoms/
c.c.、P型不純物の拡散深さXJ(第2図参照)が
60μmの場合である。pn接合Jの露出端を拡散マ
スク端(第3図においてy=0)から25μm内側
の位置(第3図においてy=25μm)に設定した
場合、ここでのpB層14の表面不純物濃度は1×
1016atoms/c.c.となる。一方第4図は階段接合に
おける不純物濃度とブレークダウン電圧VB、即
ち耐圧の関係を示しているが、1×1016atoms/
c.c.の場合、耐圧は約60Vとなる。pB層の拡散条件
が第3図の場合と同じである第1図のGTOでは
上主表面に露出しているpn接合JにおけるpB
の不純物濃度は2×1018atoms/c.c.であり、この
pn接合の耐圧は約3V程度(第3図参照)である。
In the GTO having the above configuration, the lateral resistance RPB of the pB layer 14 directly below the nE layer 15 is as low as that shown in FIG. Furthermore, it is exposed on the upper main surface.
Near the pn junction, the impurity concentration of the pB layer is low due to lateral diffusion, so the withstand voltage of the pn junction can be increased.
Figure 3 shows an example of the relationship between the lateral distance y from the edge of the diffusion mask to the inside of the diffusion mask (see Figure 2) and the surface impurity concentration. ×10 18 atoms/
cc, the diffusion depth of P-type impurity X J (see Figure 2) is
This is the case of 60 μm. When the exposed end of the pn junction J is set at a position 25 μm inside (y=25 μm in FIG. 3) from the diffusion mask end (y=0 in FIG. 3), the surface impurity concentration of the p B layer 14 here is 1×
10 16 atoms/cc. On the other hand, Figure 4 shows the relationship between the impurity concentration and the breakdown voltage VB , that is, the breakdown voltage, in a stepped junction, which is 1×10 16 atoms/
In the case of cc, the withstand voltage is approximately 60V. In the GTO shown in Figure 1, where the diffusion conditions for the p B layer are the same as those in Figure 3, the impurity concentration of the p B layer at the pn junction J exposed on the upper main surface is 2 x 10 18 atoms/cc. ,this
The withstand voltage of a pn junction is approximately 3V (see Figure 3).

第5図及び第6図は本発明の他の実施例を示し
ており、第5図は部分的断面図、第6図は第5図
におけるpB層拡散マスク19(斜視部)とnE層1
5(点部)の位置関係を示す平面図である。この
実施例ではnE層15の幅が狭い場合、nE層15全
体をpB層14の横方向拡散領域内に設けることが
できることを示している。nE層15全体がpB層の
低不純物濃度領域にあるので、nE層15を薄くし
てもpn接合Jの耐圧は第2図の実施例に比較し
て高くできる。
5 and 6 show other embodiments of the present invention, FIG. 5 is a partial cross-sectional view, and FIG. layer 1
FIG. 5 is a plan view showing the positional relationship of 5 (point portions). This example shows that if the width of the nE layer 15 is narrow, the entire nE layer 15 can be provided within the lateral diffusion region of the pB layer 14. Since the entire nE layer 15 is in the low impurity concentration region of the pB layer, the withstand voltage of the pn junction J can be made higher than in the embodiment shown in FIG. 2 even if the nE layer 15 is made thinner.

第5,6図の実施例において、L=0μm、50μ
m及び60μmにして、ボロンを表面不純物濃度を
5×1017atoms/c.c.でXJ=60μmまで拡散し、n
エミツタ層の幅WoE=10μm及び拡散深さ11μmに
した場合、ゲート耐圧はそれぞれ20V、33V及び
38Vであつた。このように本発明(L=50μm及
び60μmの場合)では、従来GTO(L=0μmの場
合)に比較して、ゲート耐圧を1.5〜2倍以上に
増大できる。その結果、本発明ではターンオフ用
ゲート電源電圧EGを高くできるのでターンオフ
時間を短かくできる。その一例として、耐圧
1200VGTO(チツプサイズ7.5mm×2mm)におい
て、本発明(L=50μmの場合)ではアノード電
流10A、EG=−30Vでターンオフ時間1μsであつ
たのに対して、従来のGTO(L=0μmの場合)で
はアノード電流10A、EG=−17Vでターンオフ時
間2μSであつた。
In the embodiments shown in Figures 5 and 6, L = 0μm, 50μ
m and 60 μm, boron is diffused at a surface impurity concentration of 5 × 10 17 atoms/cc until X J = 60 μm, and n
When the width of the emitter layer W oE = 10 μm and the diffusion depth is 11 μm, the gate breakdown voltage is 20 V, 33 V, and
It was 38V. As described above, in the present invention (when L=50 μm and 60 μm), the gate breakdown voltage can be increased by 1.5 to 2 times or more compared to the conventional GTO (when L=0 μm). As a result, in the present invention, the turn-off gate power supply voltage EG can be increased, so the turn-off time can be shortened. As an example, pressure resistance
In a 1200VGTO (chip size 7.5mm x 2mm), the present invention (when L = 50μm) had an anode current of 10A, E G = -30V and a turn-off time of 1μs, whereas the conventional GTO (when L = 0μm) had a turn-off time of 1μs. ), the anode current was 10 A, E G = -17 V, and the turn-off time was 2 μS.

以上、本発明をGTOに適用した場合について
説明したが、GTOの場合と同様にエミツタ
(GTOのカソードに対応)とベース(GTOのゲ
ートに対応)間に逆電圧を印加してターンオフ時
間を短かくするトランジスタの場合にも、本発明
を適用できる。
Above, we have explained the case where the present invention is applied to a GTO, but as in the case of a GTO, a reverse voltage is applied between the emitter (corresponding to the GTO cathode) and the base (corresponding to the GTO gate) to shorten the turn-off time. The present invention can also be applied to such a transistor.

両実施例では特殊な拡散技術によりpB層やnE
を作つている訳ではないので、製作コストが高く
なることはない。
In both embodiments, the p B layer and the n E layer are not created using a special diffusion technique, so the manufacturing cost does not increase.

〔発明の効果〕〔Effect of the invention〕

以上説明したように本発明によれば、製作コス
トを高めることなくゲート耐圧を高めた自己消弧
型スイツチング半導体装置を得ることができる。
As described above, according to the present invention, a self-extinguishing switching semiconductor device with increased gate breakdown voltage can be obtained without increasing manufacturing costs.

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

第1図は従来のGTOの半導体基体の部分的断
面図、第2図は本発明の一実施例になるGTOの
半導体基体の部分的断面図、第3図は横方向拡散
における横方向距離と不純物濃度の関係を示す
図、第4図は階段接合における不純物濃度とブレ
ークダウン電圧の関係を示す図、第5図、第6図
は本発明の他の実施例を示すGTOの半導体基体
の部分的断面図と平面図である。 11……半導体基体、12……pE層、13……
nB層、14……pB層、15……nE層、16……ア
ノード電極、17……ゲート電極、18……カソ
ード電極。
FIG. 1 is a partial cross-sectional view of the semiconductor substrate of a conventional GTO, FIG. 2 is a partial cross-sectional view of the semiconductor substrate of a GTO according to an embodiment of the present invention, and FIG. 3 is a diagram showing the lateral distance in lateral diffusion. Figure 4 is a diagram showing the relationship between impurity concentration and breakdown voltage in a stepped junction. Figures 5 and 6 are parts of a semiconductor substrate of a GTO showing other embodiments of the present invention. FIG. 2 is a cross-sectional view and a plan view. 11...Semiconductor substrate, 12...p E layer, 13...
n B layer, 14...p B layer, 15...n E layer, 16... anode electrode, 17... gate electrode, 18... cathode electrode.

Claims (1)

【特許請求の範囲】 1 半導体基体が一対の主表面間に隣接相互で順
次導電型が互に異なる少なくとも3個の半導体層
を有し、一方の主表面に第一の主電極が設けられ
る最外層と制御電極が設けられる最外層に隣接し
た層が露出し、他方の主表面に第二の主電極が設
けられる半導体装置において、上記隣接層がその
下全体が横方向拡散領域となるような大きさの拡
散マスクを用いて形成された拡散層であり、上記
最外層と上記隣接層が作るpn接合の少なくとも
上記一方の主表面と平行をなす部分と上記一方の
主表面とを連結する部分が上記横方向拡散領域に
位置していることを特徴とする半導体装置。 2 特許請求の範囲第1項において、前記pn接
合全体が前記隣接層の前記横方向拡散領域に位置
していることを特徴とする半導体装置。
[Claims] 1. A semiconductor substrate has at least three adjacent semiconductor layers having different conductivity types between a pair of main surfaces, and a first main electrode is provided on one of the main surfaces. In a semiconductor device in which a layer adjacent to the outermost layer in which an outer layer and a control electrode are provided is exposed and a second main electrode is provided on the other main surface, the adjacent layer is such that the entire bottom thereof becomes a lateral diffusion region. a diffusion layer formed using a diffusion mask of a certain size, and a portion connecting at least a portion parallel to the one main surface of the p-n junction formed by the outermost layer and the adjacent layer and the one main surface; is located in the lateral diffusion region. 2. The semiconductor device according to claim 1, wherein the entire pn junction is located in the lateral diffusion region of the adjacent layer.
JP59121800A 1984-06-15 1984-06-15 semiconductor equipment Granted JPS612364A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59121800A JPS612364A (en) 1984-06-15 1984-06-15 semiconductor equipment

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59121800A JPS612364A (en) 1984-06-15 1984-06-15 semiconductor equipment

Publications (2)

Publication Number Publication Date
JPS612364A JPS612364A (en) 1986-01-08
JPH0217939B2 true JPH0217939B2 (en) 1990-04-24

Family

ID=14820231

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59121800A Granted JPS612364A (en) 1984-06-15 1984-06-15 semiconductor equipment

Country Status (1)

Country Link
JP (1) JPS612364A (en)

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS507424A (en) * 1973-05-18 1975-01-25

Also Published As

Publication number Publication date
JPS612364A (en) 1986-01-08

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