JPS61147570A - Schottky barrier semiconductor device - Google Patents
Schottky barrier semiconductor deviceInfo
- Publication number
- JPS61147570A JPS61147570A JP26985584A JP26985584A JPS61147570A JP S61147570 A JPS61147570 A JP S61147570A JP 26985584 A JP26985584 A JP 26985584A JP 26985584 A JP26985584 A JP 26985584A JP S61147570 A JPS61147570 A JP S61147570A
- Authority
- JP
- Japan
- Prior art keywords
- voltage
- type silicon
- surge
- schottky barrier
- 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.)
- Granted
Links
- 230000004888 barrier function Effects 0.000 title claims abstract description 34
- 239000004065 semiconductor Substances 0.000 title claims abstract description 34
- 230000015556 catabolic process Effects 0.000 claims abstract description 20
- 229910052751 metal Inorganic materials 0.000 claims description 16
- 239000002184 metal Substances 0.000 claims description 16
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical group [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 abstract description 55
- 229910052710 silicon Inorganic materials 0.000 abstract description 55
- 239000010703 silicon Substances 0.000 abstract description 55
- 238000000034 method Methods 0.000 abstract description 3
- QHGVXILFMXYDRS-UHFFFAOYSA-N pyraclofos Chemical compound C1=C(OP(=O)(OCC)SCCC)C=NN1C1=CC=C(Cl)C=C1 QHGVXILFMXYDRS-UHFFFAOYSA-N 0.000 abstract 1
- 239000000758 substrate Substances 0.000 description 5
- 230000006872 improvement Effects 0.000 description 3
- VYZAMTAEIAYCRO-UHFFFAOYSA-N Chromium Chemical compound [Cr] VYZAMTAEIAYCRO-UHFFFAOYSA-N 0.000 description 2
- 150000004678 hydrides Chemical class 0.000 description 2
- ZOKXTWBITQBERF-UHFFFAOYSA-N Molybdenum Chemical compound [Mo] ZOKXTWBITQBERF-UHFFFAOYSA-N 0.000 description 1
- 230000008901 benefit Effects 0.000 description 1
- 239000003795 chemical substances by application Substances 0.000 description 1
- 229910052804 chromium Inorganic materials 0.000 description 1
- 239000011651 chromium Substances 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000010438 heat treatment Methods 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 229910052750 molybdenum Inorganic materials 0.000 description 1
- 239000011733 molybdenum Substances 0.000 description 1
- 230000002093 peripheral effect Effects 0.000 description 1
- 230000009467 reduction Effects 0.000 description 1
- 238000007740 vapor deposition Methods 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L29/00—Semiconductor devices adapted for rectifying, amplifying, oscillating or switching, or capacitors or resistors with at least one potential-jump barrier or surface barrier, e.g. PN junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof ; Multistep manufacturing processes therefor
- H01L29/66—Types of semiconductor device ; Multistep manufacturing processes therefor
- H01L29/86—Types of semiconductor device ; Multistep manufacturing processes therefor controllable only by variation of the electric current supplied, or only the electric potential applied, to one or more of the electrodes carrying the current to be rectified, amplified, oscillated or switched
- H01L29/861—Diodes
- H01L29/872—Schottky diodes
Abstract
Description
【発明の詳細な説明】
(イ)産業上の利用分野
本発明は改良されたサージ耐圧特性を有するショットキ
)<’I)7半導体装置に関するものである。DETAILED DESCRIPTION OF THE INVENTION (A) Field of Industrial Application The present invention relates to a Schottky)<'I)7 semiconductor device having improved surge withstand voltage characteristics.
(ロ)従来の技術
ショットキバリア半導体装置は順方向電圧が低く、順方
向の電力損失が小さいという特徴を有し、スイッチング
電源回路の出力整流ダイオード等への応用が?r入引、
でいる一駈ムスイッチング璽源回路の出力整流ダイオー
ドに適用する罠は、逆方向降伏電圧が高いこと及び破壊
耐量(サージ耐圧)が犬ぎいことが要求される。(b) Conventional technology Schottky barrier semiconductor devices have the characteristics of low forward voltage and low forward power loss, and can they be applied to output rectifier diodes of switching power supply circuits, etc.? r input,
The trap applied to the output rectifier diode of the single-speed switching power source circuit is required to have a high reverse breakdown voltage and a high breakdown withstand voltage (surge withstand voltage).
従来のショットキバリア半導体装置では特公昭59−3
5183号公報(HOIL29/48)に示す如く、逆
方向降伏電圧を高くする改良が採られている。即ちガー
ドリング構造又はフィールドプレート構造である。しか
しガードリング構造は金属−半導体接触の周辺部の逆電
流を小さくするのみであり、金属−半導体接触の中央部
の逆電流を小さくすることができない。またフィールド
プレート構造も金属−半導体接触の周辺部の特性改善に
他ならない。従っていずれの構造でもショットキバリア
半導体装置の降伏電圧を大幅に上昇させることはできな
かった。In the conventional Schottky barrier semiconductor device, the
As shown in Publication No. 5183 (HOIL29/48), improvements have been made to increase the reverse breakdown voltage. That is, it is a guard ring structure or a field plate structure. However, the guard ring structure only reduces the reverse current at the periphery of the metal-semiconductor contact, but cannot reduce the reverse current at the center of the metal-semiconductor contact. The field plate structure also improves the characteristics of the peripheral area of the metal-semiconductor contact. Therefore, in either structure, it was not possible to significantly increase the breakdown voltage of the Schottky barrier semiconductor device.
特公昭59−35183号公報に開示されたショットキ
バリア半導体装置は逆電流を低減させ且つ逆方向降伏電
圧を高めることを可能にしている。The Schottky barrier semiconductor device disclosed in Japanese Patent Publication No. 59-35183 makes it possible to reduce reverse current and increase reverse breakdown voltage.
第3図及び第4図を参照して詳述すると、N 型シリコ
ン層Qllの上にエピタキシャル成長したN型シリコン
領域a2を有するシリコン基板03を用意し、ここに複
数のP 型シリコン領域Iを形成し、酸化膜住ツの開口
四を利用してクロムからなる金属層aηを設けている。To explain in detail with reference to FIGS. 3 and 4, a silicon substrate 03 having an N-type silicon region a2 epitaxially grown on an N-type silicon layer Qll is prepared, and a plurality of P-type silicon regions I are formed here. A metal layer aη made of chromium is provided using the opening 4 of the oxide film.
クロム金属層αDは蒸着後350℃〜500℃の範囲で
6分間〜9000分間の熱処理を施して形成することが
望ましく、これにより0.65±0.015eVの安定
したバリアハイドを得ることができる。シリコン基板(
1310表面状態を示す第4図から明らかなようにP
型シリコン領域(14は4本の帯状部分(14a)と上
下の結合部(14b)、(14c) とから成る。従
りて平面的にはP+型シリコン領域Iの中に複数の短冊
形N型シリコン領域α3が配置され、P 型シリコン領
域IとN型シリコン領域α4とが交互に表面に露呈して
いる。It is desirable to form the chromium metal layer αD by performing heat treatment for 6 minutes to 9000 minutes at a temperature of 350° C. to 500° C. after vapor deposition, whereby a stable barrier hydride of 0.65 ± 0.015 eV can be obtained. . Silicon substrate (
As is clear from Figure 4 showing the 1310 surface condition, P
The type silicon region (14) consists of four strip-shaped portions (14a) and upper and lower connecting portions (14b) and (14c).Therefore, in plan view, there are a plurality of rectangular shapes N in the P+ type silicon region I. A type silicon region α3 is arranged, and P type silicon regions I and N type silicon regions α4 are alternately exposed on the surface.
+
P 型シリコン領域a4の相互間の距離は、金属層αη
に負、下部の金属電極αのに正の電圧を印加したとぎに
生じる空間電荷領域によってP 型シリコン領域α滲の
相互に結ばれる大きさとする。この場合更にN型シリコ
ン領域α2と金属層αηとで形成されるシl ットキバ
リアの逆方向降伏電圧よりも低い電圧で上述の如くP
型シリコン領域−の相互間が結ばれるようにする2゜
斯上の構造のショットキバリア半導体装置では高い逆方
向電圧が印加されると、P 型シリコン領域IとN型シ
リコン領域aaとから成るPN接合により形成される空
間電荷領域が広がってP 型シリコン領域(141の相
互間が空間電荷領域によって結ばれた状態となり、シリ
コン基板αJに接触する金属層(17)の下部全領域に
空間電荷領域が分布する。+ The distance between the P-type silicon regions a4 is the metal layer αη
The size is such that the P type silicon regions α are connected to each other by a space charge region generated when a negative voltage is applied to the lower metal electrode α and a positive voltage is applied to the lower metal electrode α. In this case, the voltage lower than the reverse breakdown voltage of the Schittky barrier formed by the N-type silicon region α2 and the metal layer αη is
In a Schottky barrier semiconductor device having the above structure, when a high reverse voltage is applied, a PN consisting of a P-type silicon region I and an N-type silicon region aa is connected to each other. The space charge region formed by the bonding expands, and the P-type silicon regions (141) are connected by the space charge region, and a space charge region is formed in the entire lower region of the metal layer (17) in contact with the silicon substrate αJ. is distributed.
この結果空間電荷領域によって逆方向電流が遮断され、
高い逆方向降伏電圧を実現できる。As a result, the space charge region blocks the reverse current,
High reverse breakdown voltage can be achieved.
el 発明が解決しようとする問題点斯る従来のショ
ットキバリア半導体装置では逆方向降伏電圧の向上を実
現できるが、スイッチング電源回路等で要求される破壊
耐量の向上は得られない欠点があった。el Problems to be Solved by the Invention Although the conventional Schottky barrier semiconductor device can achieve an improvement in reverse breakdown voltage, it has the drawback that it cannot achieve an improvement in breakdown strength required for switching power supply circuits and the like.
即ち従来のショットキバリア半導体装置ではN盤シリコ
ン領域鰺な約11μm厚とするとP 裂シリコン領域I
は高々約3μmの深さに形成していたので、第2図に示
す如く逆方向降伏電圧の最も高い範囲で作動させていた
。しかしこの範囲ではサージ耐量は第2図から明らかな
様に最も低い範囲で使用することになり、従来のショッ
トキバリア半導体装置はサージ耐量が極め℃弱い欠点を
有していた。That is, in a conventional Schottky barrier semiconductor device, if the N-cavity silicon region is approximately 11 μm thick, the P-cavity silicon region I is approximately 11 μm thick.
was formed to a depth of about 3 μm at the most, so it was operated in the range where the reverse breakdown voltage was highest, as shown in FIG. However, within this range, the surge withstand capability is used at its lowest range, as is clear from FIG. 2, and the conventional Schottky barrier semiconductor device has the disadvantage that the surge withstand capability is extremely weak in degrees centigrade.
に)問題点を解決するための手段
本発明は斯点に鑑み℃なされ、ショットキバリア半導体
装置のP 型シリコン領域を床く拡散して逆方向降伏電
圧を犠牲にする反面サージ耐量を大巾に改善したショッ
トキバリア半導体装置を実現するものである。In view of the above, the present invention was devised by diffusing the P-type silicon region of the Schottky barrier semiconductor device, thereby sacrificing the reverse breakdown voltage, while greatly increasing the surge resistance. An improved Schottky barrier semiconductor device is realized.
(ホ)作用
本発明に依るショットキバリア半導体装置はP+型シリ
コン領域(4)を従来より深く拡散し℃、ショットキバ
リアのサージ耐量よりP 型シリコン領域(4)とN型
シリコン領域(2)により形成されるPN接合下のパン
チスルー電圧を小さく設定してスイッチング電源等で要
求されるサージ耐量を向上させている。(E) Function The Schottky barrier semiconductor device according to the present invention has a P+ type silicon region (4) diffused deeper than the conventional one. The punch-through voltage under the formed PN junction is set low to improve the surge resistance required for switching power supplies and the like.
(へ)実施例
本発明に依るショットキバリア半導体装置を第1図及び
第2図を参照して詳述する。(F) Embodiment A Schottky barrier semiconductor device according to the present invention will be described in detail with reference to FIGS. 1 and 2.
本発明に依るショットキバリア半導体装置はN+型シリ
コン層(11の上にエピタキシャル成長した第10半導
体領域となるN型シリコン領域(2)を有するシリコン
基板(3)を準備し、ここに第2の半導体領域となる複
数のP 型シリコン領域(4)を形成し、酸化膜(5)
の開口(6)を利用してモリブデンからなるショットキ
バリアを形成する金属層(7)を設けている。この金属
層(力は蒸着後350℃〜500℃で熱処理をして0.
65±0.015eVのバリアハイドな形成する。P
型シリコン領域(4)は第4図に示す従来のものと同様
に4本の帯状部分(14a)と上下の結合部(14b)
、(14C)から成り、平面的に+
はP 型シリコン領域(4)の中に複数の短冊形N型シ
リコン領域(2)が配置され、P 屋シリコン領域(4
)とN型シリコン領域(2)とが交互に表面に配列され
ている。金属層(力はP 型シリコン領域(4)とそれ
に囲まれたN型シリコ/領域(2)と接触し、N凰シリ
コン領域(2)間でショットキバリアを形成している。In the Schottky barrier semiconductor device according to the present invention, a silicon substrate (3) having an N-type silicon region (2) which is epitaxially grown on an N+-type silicon layer (11 and serving as a tenth semiconductor region) is prepared, and a second semiconductor layer (3) is prepared. A plurality of P-type silicon regions (4) are formed, and an oxide film (5) is formed.
A metal layer (7) that forms a Schottky barrier made of molybdenum is provided using the opening (6). This metal layer (with a strength of 0.00000.
A barrier hydride of 65±0.015 eV is formed. P
The mold silicon region (4) has four strip-shaped parts (14a) and upper and lower joint parts (14b) as in the conventional one shown in FIG.
, (14C), in which a plurality of rectangular N-type silicon regions (2) are arranged in a P-type silicon region (4), and a P-type silicon region (4) is formed in a plane.
) and N-type silicon regions (2) are alternately arranged on the surface. The metal layer (force) contacts the P-type silicon region (4) and the surrounded N-type silicon region (2), forming a Schottky barrier between the N-type silicon regions (2).
本発明の特徴はP 型シリコン領域(4)にある。The feature of the present invention lies in the P type silicon region (4).
+
P 型シリコン領域(4)を従来のものより深く拡散す
る。具体的にはN型シリコン領域(2)を約11μm厚
に設計した場合、従来のP 型シリコン領域(4)を高
々3μm以下に拡散していたものを本発明+
のPiシリコン領域(4)を3.5μmから4.5μm
の深さに拡散している。P 型シリコン領域(4)の深
さは第2図から明らかな様に逆方向降伏電圧が低下する
が、サージ耐量が増加する範囲を設定している。具体的
には逆方向降伏電圧が最高約130■得られるものを本
発明では約110Vで使用している。+ The P-type silicon region (4) is diffused deeper than the conventional one. Specifically, when the N-type silicon region (2) is designed to have a thickness of approximately 11 μm, the conventional P-type silicon region (4), which is diffused to a thickness of at most 3 μm or less, becomes the Pi silicon region (4) of the present invention+. from 3.5μm to 4.5μm
is diffused to a depth of As is clear from FIG. 2, the depth of the P-type silicon region (4) is set within a range where the reverse breakdown voltage decreases but the surge resistance increases. Specifically, in the present invention, a material with a maximum reverse breakdown voltage of about 130V is used at about 110V.
斯上の構造に依ればP 型シリコン領域(4)を深く形
成するのでP 型シリコン領域(4)直下のパンチスル
ー電圧を従来のものに比べて大巾に低下できる。−万金
属層(7)とN型シリコン領域(2)とで形成されるバ
リアハイドの低い部分での従来のサージ耐量は第2図よ
り約80v程度である。そこで本発明はP 型シリコン
領域(4)直下のパンチスルー電圧を80v以下に設定
できる様にP 型シリコン領域(4)を深く拡散してい
る。この結果金属層(力と裏面の金属電極(8)間にシ
ョットキバリアのサージ破壊電圧を超えるサージ電圧が
印加されても+
P 型シリコン領域(4)下でパンチスルーを発生して
サージ電圧はN 型シリコン層(2)および金属電極(
8)を介して逃げる。このためショットキバリアでのサ
ージ破壊は未然に防止でき、サージ電圧はすべてP 型
シリコン領域(4)下の空乏層により吸収できるのであ
る。従ってサージ耐量は第2図から明らかな様に、従来
の80vから大巾に向上してIKVまで上昇できる。According to the above structure, since the P type silicon region (4) is formed deeply, the punch-through voltage directly under the P type silicon region (4) can be greatly reduced compared to the conventional structure. - The conventional surge resistance at the low part of the barrier hide formed by the metal layer (7) and the N-type silicon region (2) is about 80V as shown in FIG. Therefore, in the present invention, the P type silicon region (4) is deeply diffused so that the punch-through voltage directly under the P type silicon region (4) can be set to 80 V or less. As a result, even if a surge voltage exceeding the surge breakdown voltage of the Schottky barrier is applied between the metal layer (force) and the metal electrode (8) on the back surface, punch-through occurs under the +P type silicon region (4) and the surge voltage N-type silicon layer (2) and metal electrode (
8) Escape via. Therefore, surge breakdown in the Schottky barrier can be prevented, and all the surge voltage can be absorbed by the depletion layer under the P-type silicon region (4). Therefore, as is clear from FIG. 2, the surge resistance can be greatly improved from the conventional 80V to IKV.
(ト)発明の効果
本発明に依ればP 型シリコン領域(4)を従来より深
く形成することにより、逆方向降伏電圧を若干犠牲にす
るがサージ耐量を従来より10倍以上に向上できる利点
を有する。この結果スイッチング電源回路等に最適のシ
1ットキパリアダイオードを得られ、電源回路の小型化
軽量化に寄与できるのである。(G) Effects of the Invention According to the present invention, by forming the P-type silicon region (4) deeper than before, the surge resistance can be improved by more than 10 times than before, although the reverse breakdown voltage is slightly sacrificed. has. As a result, it is possible to obtain a shut-chip parrier diode that is most suitable for switching power supply circuits, etc., and contributes to the reduction in size and weight of power supply circuits.
また本発明は従来のショットキバリア半導体装置のP
型シリコン領域(4)を深く拡散するのみで実現でき、
何ら工程を増加することなく導入できる利点を有する。Further, the present invention provides P of the conventional Schottky barrier semiconductor device.
This can be achieved simply by deeply diffusing the mold silicon region (4).
It has the advantage that it can be introduced without any increase in process steps.
第1図は本発明のショットキバリア半導体装置を説明す
る断面図、第2図は本発明および従来のショットキバリ
ア半導体装置の逆方向降伏電圧特性およびサージ耐量を
説明する特性図、第3図および第4図は従来のショット
キバリア半導体装置を説明する断面図および上面図であ
る。
(1)はNuシリコン層、 (2)はN型シリコン層+
域、 ■は半導体基板、 (4)はP 型シリコン領域
、 (5)は酸化膜、 (6)は開口、 (7)は金属
層、(8)は金属電極である。
出願人 三洋電機株式会社 外1名
代理人 弁理士 佐 野 靜゛夫
第1図FIG. 1 is a sectional view illustrating the Schottky barrier semiconductor device of the present invention, FIG. 2 is a characteristic diagram illustrating the reverse breakdown voltage characteristics and surge withstand capacity of the Schottky barrier semiconductor device of the present invention and the conventional Schottky barrier semiconductor device, and FIGS. FIG. 4 is a cross-sectional view and a top view illustrating a conventional Schottky barrier semiconductor device. (1) is Nu silicon layer, (2) is N-type silicon layer + region, (2) is semiconductor substrate, (4) is P-type silicon region, (5) is oxide film, (6) is opening, (7) is The metal layer (8) is a metal electrode. Applicant Sanyo Electric Co., Ltd. and one other agent Patent attorney Seiji Sano Figure 1
Claims (1)
域表面に設けた逆導電型の第2の半導体領域とショット
キバリア用金属層とを具備するショットキバリア半導体
装置に於いて、前記第2の半導体領域を深く形成してシ
ョットキバリアのサージ耐圧より前記第2の半導体領域
直下のパンチスルー電圧を小さく設定することを特徴と
するショットキバリア半導体装置。(1) In a Schottky barrier semiconductor device comprising a first semiconductor region of one conductivity type, a second semiconductor region of the opposite conductivity type provided on the surface of the first semiconductor region, and a Schottky barrier metal layer, A Schottky barrier semiconductor device, characterized in that the second semiconductor region is formed deeply and a punch-through voltage directly under the second semiconductor region is set to be lower than a surge breakdown voltage of the Schottky barrier.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP26985584A JPS61147570A (en) | 1984-12-20 | 1984-12-20 | Schottky barrier semiconductor device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP26985584A JPS61147570A (en) | 1984-12-20 | 1984-12-20 | Schottky barrier semiconductor device |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS61147570A true JPS61147570A (en) | 1986-07-05 |
JPH0476218B2 JPH0476218B2 (en) | 1992-12-03 |
Family
ID=17478134
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP26985584A Granted JPS61147570A (en) | 1984-12-20 | 1984-12-20 | Schottky barrier semiconductor device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS61147570A (en) |
Cited By (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5148241A (en) * | 1989-12-15 | 1992-09-15 | Kabushiki Kaisha Toshiba | Method of manufacturing a schottky diode device |
JPH06121513A (en) * | 1992-10-06 | 1994-04-28 | Sumitomo Metal Mining Co Ltd | Magnetic actuator |
JP2002076371A (en) * | 2000-06-12 | 2002-03-15 | Fuji Electric Co Ltd | Semiconductor device |
JP2006210690A (en) * | 2005-01-28 | 2006-08-10 | Matsushita Electric Ind Co Ltd | Semiconductor device for surge protection |
JP2008519448A (en) * | 2004-11-08 | 2008-06-05 | ローベルト ボツシユ ゲゼルシヤフト ミツト ベシユレンクテル ハフツング | Semiconductor device and manufacturing method of semiconductor device |
KR20140099879A (en) * | 2011-12-01 | 2014-08-13 | 로베르트 보쉬 게엠베하 | High-voltage trench junction barrier schottky diode |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5168183A (en) * | 1974-12-10 | 1976-06-12 | Nippon Electric Co | SHOTSUTOKI SEIRYUSOSHI |
JPS5224465A (en) * | 1975-08-20 | 1977-02-23 | Sanken Electric Co Ltd | Schottky barrier semiconductor device |
-
1984
- 1984-12-20 JP JP26985584A patent/JPS61147570A/en active Granted
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5168183A (en) * | 1974-12-10 | 1976-06-12 | Nippon Electric Co | SHOTSUTOKI SEIRYUSOSHI |
JPS5224465A (en) * | 1975-08-20 | 1977-02-23 | Sanken Electric Co Ltd | Schottky barrier semiconductor device |
Cited By (8)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5148241A (en) * | 1989-12-15 | 1992-09-15 | Kabushiki Kaisha Toshiba | Method of manufacturing a schottky diode device |
JPH06121513A (en) * | 1992-10-06 | 1994-04-28 | Sumitomo Metal Mining Co Ltd | Magnetic actuator |
JP2002076371A (en) * | 2000-06-12 | 2002-03-15 | Fuji Electric Co Ltd | Semiconductor device |
JP2008519448A (en) * | 2004-11-08 | 2008-06-05 | ローベルト ボツシユ ゲゼルシヤフト ミツト ベシユレンクテル ハフツング | Semiconductor device and manufacturing method of semiconductor device |
US8816467B2 (en) | 2004-11-08 | 2014-08-26 | Robert Bosch Gmbh | Semiconductor device and method for manufacturing same |
JP2006210690A (en) * | 2005-01-28 | 2006-08-10 | Matsushita Electric Ind Co Ltd | Semiconductor device for surge protection |
KR20140099879A (en) * | 2011-12-01 | 2014-08-13 | 로베르트 보쉬 게엠베하 | High-voltage trench junction barrier schottky diode |
JP2015504610A (en) * | 2011-12-01 | 2015-02-12 | ローベルト ボツシユ ゲゼルシヤフト ミツト ベシユレンクテル ハフツングRobert Bosch Gmbh | High voltage trench junction Schottky barrier diode |
Also Published As
Publication number | Publication date |
---|---|
JPH0476218B2 (en) | 1992-12-03 |
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