JPH0229729Y2 - - Google Patents

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Publication number
JPH0229729Y2
JPH0229729Y2 JP1982113716U JP11371682U JPH0229729Y2 JP H0229729 Y2 JPH0229729 Y2 JP H0229729Y2 JP 1982113716 U JP1982113716 U JP 1982113716U JP 11371682 U JP11371682 U JP 11371682U JP H0229729 Y2 JPH0229729 Y2 JP H0229729Y2
Authority
JP
Japan
Prior art keywords
semiconductor layer
semiconductor
layer
type
impurity concentration
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
JP1982113716U
Other languages
Japanese (ja)
Other versions
JPS5936264U (en
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
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Priority to JP1982113716U priority Critical patent/JPS5936264U/en
Publication of JPS5936264U publication Critical patent/JPS5936264U/en
Application granted granted Critical
Publication of JPH0229729Y2 publication Critical patent/JPH0229729Y2/ja
Granted legal-status Critical Current

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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
    • H10D62/102Constructional design considerations for preventing surface leakage or controlling electric field concentration
    • H10D62/103Constructional design considerations for preventing surface leakage or controlling electric field concentration for increasing or controlling the breakdown voltage of reverse-biased devices
    • H10D62/105Constructional design considerations for preventing surface leakage or controlling electric field concentration for increasing or controlling the breakdown voltage of reverse-biased devices by having particular doping profiles, shapes or arrangements of PN junctions; by having supplementary regions, e.g. junction termination extension [JTE] 
    • H10D62/106Constructional design considerations for preventing surface leakage or controlling electric field concentration for increasing or controlling the breakdown voltage of reverse-biased devices by having particular doping profiles, shapes or arrangements of PN junctions; by having supplementary regions, e.g. junction termination extension [JTE]  having supplementary regions doped oppositely to or in rectifying contact with regions of the semiconductor bodies, e.g. guard rings with PN or Schottky junctions
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D8/00Diodes
    • H10D8/60Schottky-barrier diodes 

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  • Electrodes Of Semiconductors (AREA)

Description

【考案の詳細な説明】 本考案は、高耐圧化及び高信頼性化されたシヨ
ツトキバリア半導体装置に関するものである。
[Detailed Description of the Invention] The present invention relates to a shot barrier semiconductor device with high breakdown voltage and high reliability.

シヨツトキバリア半導体装置は順電圧が低く、
順方向の電力損失が小さいという特徴を有する反
面、逆方向降伏電圧が低いという欠点があつた。
そこで、従来ガードリング構造、又はフイールド
プレート構造等にすることによつて降伏電圧を高
める試みがなされている。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出来ない。又、フイー
ルドプレート構造も金属−半導体接触の周辺部の
特性改善にほかならない。従つて、いずれの構造
でもシヨツ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出来なかつた。
Schottky barrier semiconductor devices have low forward voltage;
Although it had the feature of low power loss in the forward direction, it had the drawback of low breakdown voltage in the reverse direction.
Therefore, attempts have been made to increase the breakdown voltage by creating a guard ring structure, a field plate structure, or the like. 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 periphery of the metal-semiconductor contact. Therefore, in either structure, it was not possible to significantly increase the breakdown voltage of the shot barrier semiconductor device.

上述の如き欠点を解決するために、本件出願人
は特願昭50−100896号(特開昭52−24465号)に
てpn接合の逆バイアスに基づく空間電荷領域に
よつて逆方向電流を減少させ、高耐圧化を図つた
シヨツトキバリア半導体装置を提案した。しか
し、更に高耐圧化及び高信頼性化する方法は開示
されていない。
In order to solve the above-mentioned drawbacks, the applicant of the present application proposed in Japanese Patent Application No. 50-100896 (Japanese Unexamined Patent Publication No. 52-24465) that the reverse current is reduced by a space charge region based on the reverse bias of the pn junction. We proposed a shot barrier semiconductor device with high voltage resistance. However, a method for further increasing the voltage resistance and reliability is not disclosed.

そこで、本考案の目的は、特願昭50−100896号
の発明を利用して、逆方向耐圧、信頼性、及び順
方向特性を更に良くすることが可能なシヨツトキ
バリア半導体装置を提供することにある。
Therefore, an object of the present invention is to provide a shot barrier semiconductor device that can further improve reverse breakdown voltage, reliability, and forward characteristics by utilizing the invention of Japanese Patent Application No. 100896/1982. .

上記目的を達成するための本考案は、n型又は
p型の第1の導電型を有すると共に高不純物濃度
を有する第1の半導体層と、前記第1の導電型を
有すると共に前記第1の半導体層の不純物濃度よ
りも低い不純物濃度を有して前記第1の半導体層
の上に形成された第2の半導体層と、前記第1の
導電型を有すると共に前記第2の半導体層の不純
物濃度よりも低い不純物濃度を有して前記第2の
半導体層の上に形成され且つその上面が半導体基
板の表面に露呈している第3の半導体層と、その
上面が前記半導体基板の表面に露呈し、その下面
が前記第2の半導体層に隣接し、その側面に前記
第3の半導体層が隣接するように配設され、且つ
前記第3の半導体層よりも深く形成され、且つ前
記第1の導電型と反対の第2の導電型を有してい
る第4の半導体層と、前記第3の半導体層に対し
てシヨツトキバリアを形成するように接触し且つ
前記第4の半導体層に対してオーミツクコンタク
トを形成するように接触している金属層とを具備
し、前記半導体基板の表面の特定方向の直線上に
おいて前記シヨツトキバリアと前記オーミツクコ
ンタクトが交互に配置されるように前記第3及び
第4の半導体層が配置されていることを特徴とす
るシヨツトキバリア半導体装置に係わるものであ
る。
The present invention for achieving the above object includes: a first semiconductor layer having a first conductivity type of n-type or p-type and having a high impurity concentration; a second semiconductor layer formed on the first semiconductor layer having an impurity concentration lower than that of the semiconductor layer; and an impurity of the second semiconductor layer having the first conductivity type. a third semiconductor layer having an impurity concentration lower than that of the second semiconductor layer and having an upper surface exposed to the surface of the semiconductor substrate; The semiconductor layer is exposed, a lower surface thereof is adjacent to the second semiconductor layer, a side surface thereof is adjacent to the third semiconductor layer, and the semiconductor layer is formed deeper than the third semiconductor layer; a fourth semiconductor layer having a second conductivity type opposite to the first conductivity type and in contact with the third semiconductor layer to form a shot barrier and with respect to the fourth semiconductor layer; and a metal layer in contact with the semiconductor substrate so as to form an ohmic contact, and the shot barrier and the ohmic contact are arranged alternately on a straight line in a specific direction on the surface of the semiconductor substrate. The present invention relates to a shot barrier semiconductor device characterized in that a fourth semiconductor layer is arranged.

上記考案によれば、第3の半導体層を設けてシ
ヨツトキバリア直下の不純物濃度を低くしたの
で、第4の半導体層から広がる空間電荷領域がシ
ヨツトキバリアの下部に広がり易くなり、第4の
半導体層を設けることによる逆方向特性向上の効
果(逆方向電流の減少、高耐圧化)が一層顕著に
なる。特に、第3の半導体層が第4の半導体層よ
り浅く形成されているので、第4の半導体層から
広がる空間電荷領域は、シヨツトキバリアの下部
には広がり易くても、第4の半導体層の下部には
これより広がり難い。このため、第4の半導体層
から広がる空間電荷領域が第1の半導体層に到達
してリーチスルー降伏を起こす逆電圧値が、第3
の半導体層を設けたことにより低下することはな
い。すなわち、リーチスルー降伏を起こす逆電圧
値の低下に伴う耐圧低下を防止するために第2の
半導体層を厚くする必要はなく、第2の半導体層
を厚くしたことにより直列抵抗が増大して順電圧
が増大するという欠点は生じない。しかも、最も
高抵抗の領域である第3の半導体層を相対的に浅
く形成することになるので、この面でも順電圧の
増大を抑える合理的な構造となつている。
According to the above idea, since the third semiconductor layer is provided to lower the impurity concentration directly under the shottock barrier, the space charge region spreading from the fourth semiconductor layer can easily spread to the bottom of the shottock barrier, and the fourth semiconductor layer is provided. As a result, the effect of improving reverse characteristics (reduction in reverse current, higher breakdown voltage) becomes even more remarkable. In particular, since the third semiconductor layer is formed shallower than the fourth semiconductor layer, the space charge region spreading from the fourth semiconductor layer tends to spread to the bottom of the shot barrier, but the space charge region spreads from the fourth semiconductor layer to the bottom of the fourth semiconductor layer. It is more difficult to spread than this. Therefore, the reverse voltage value at which the space charge region spreading from the fourth semiconductor layer reaches the first semiconductor layer and causes reach-through breakdown is lower than the third semiconductor layer.
This does not occur due to the provision of the semiconductor layer. In other words, it is not necessary to make the second semiconductor layer thicker in order to prevent a decrease in breakdown voltage due to a decrease in reverse voltage value that causes reach-through breakdown, and by making the second semiconductor layer thicker, the series resistance increases and the The disadvantage of increased voltage does not occur. Moreover, since the third semiconductor layer, which is the region with the highest resistance, is formed to be relatively shallow, the structure is reasonable in this respect as well to suppress an increase in forward voltage.

次に、第1図及び第2図を参照して本考案の実
施例に係わるシヨツトキバリア半導体装置につい
て述べる。
Next, a shot barrier semiconductor device according to an embodiment of the present invention will be described with reference to FIGS. 1 and 2.

第1図に示すシヨツトキバリア半導体装置は、
n+型(第1の導電型)のシリコン基板からなる
第1の半導体層1の上に、n型のシリコンエピタ
キシヤル層から成る第2の半導体層2を形成し、
更に、第2の半導体層2の表面からB+イオンを
3×1011/cm2注入することによつて不純物補償で
n-型の第3の半導体層3を形成し、しかる後、
縞状にp+型(第2の導電型)の第4の半導体層
4を形成し、シヨツトキバリアを得るためにCr
を厚さ約2000Åに蒸着し更にAg及びNiを連続的
に蒸着することによつて金属層5を設け、又下部
電極金属層6を設けたものである。尚、7は約
7000ÅのSiO2層、8はp+型のガードリング半導
体層である。
The shot barrier semiconductor device shown in FIG.
A second semiconductor layer 2 made of an n - type silicon epitaxial layer is formed on a first semiconductor layer 1 made of an n + type (first conductivity type) silicon substrate,
Furthermore, impurity compensation can be achieved by implanting B + ions at 3×10 11 /cm 2 from the surface of the second semiconductor layer 2.
Forming an n - type third semiconductor layer 3, and then
A p + type (second conductivity type) fourth semiconductor layer 4 is formed in a striped pattern, and Cr is used to obtain a shot barrier.
The metal layer 5 was formed by vapor-depositing the metal to a thickness of about 2000 Å, and then the metal layer 5 was formed by successively vapor-depositing Ag and Ni, and the lower electrode metal layer 6 was also formed. In addition, 7 is approximately
7000 Å SiO 2 layer, 8 is a p + type guard ring semiconductor layer.

各層の不純物濃度を示すと、第1の半導体層1
が約5×1019/cm3、第2の半導体層2が約4×
1015/cm3、第3の半導体層3が1×1015/cm3(補
償後)、第4の半導体層4が約6×1018/cm3の不
純物濃度を夫々有する。また、半導体上面(電極
面)から第2の半導体層2の下端までの深さが約
10μ、p+型の第4の半導体層4の深さが約2μであ
り、第3の半導体層3の深さは第4の半導体層4
よりも更に浅く形成されている。また、p+型の
第4の半導体層4の幅は約6μ、第4の半導体層
4の相互間のn-型の第3の半導体層3の幅は約
10μである。
Showing the impurity concentration of each layer, the first semiconductor layer 1
is approximately 5×10 19 /cm 3 , and the second semiconductor layer 2 is approximately 4×
10 15 /cm 3 , the third semiconductor layer 3 has an impurity concentration of 1×10 15 /cm 3 (after compensation), and the fourth semiconductor layer 4 has an impurity concentration of about 6×10 18 /cm 3 . Also, the depth from the top surface of the semiconductor (electrode surface) to the bottom end of the second semiconductor layer 2 is approximately
10μ, the depth of the p + type fourth semiconductor layer 4 is approximately 2μ, and the depth of the third semiconductor layer 3 is approximately 2μ.
It is formed even more shallowly than the Further, the width of the p + type fourth semiconductor layer 4 is approximately 6μ, and the width of the n type third semiconductor layer 3 between the fourth semiconductor layers 4 is approximately
It is 10μ.

第1図に示す如く構成されたシヨツトキバリア
半導体装置の上側電極金属層5に正の電圧を印加
して順バイアス状態とすれば、金属層5、第3の
半導体層3、第2の半導体層2、第1の半導体層
1、下側金属層6の経路で順方向電流が流れる。
一方、上側の金属層5に例えばマイナス30Vを印
加して逆バイアス状態とすれば、p+型の第4の
半導体層4とn-型の第3の半導体層3との間が
逆バイアス状態となり、p+型の第4の半導体層
4から約5.1μの幅で空間電荷領域即ち空乏層がn-
型の第3の半導体層3に広がる。n-型の第3の
半導体層3には両側から空乏層が延びてくるの
で、結局−30Vの逆電圧によつてn-型の第3の半
導体層3の表面が空乏層によつて埋まる。これに
より、金属層5とn-型の第3の半導体層3とを
通つて流れる逆方向電流は大幅に制限される。
p+型の第4の半導体層4の直下のn型の第2の
半導体層2に延びる空乏層は、不純物濃度の違い
から第3の半導体層3の広がり幅より小さく、リ
ーチスルー降伏を起こすにはまだ十分の余裕があ
る。今、−30Vの逆バイアスでn-型の第3の半導
体層3を空乏層で埋めた場合について述べたが、
低い逆方向電圧の場合には、第3の半導体層3が
空乏層で埋められない。しかし、空乏層が形成さ
れている領域は逆方向電流が流れにくいので、空
乏層の分だけ逆方向電流が抑えられる。また、空
乏層が広がつた分だけ逆方向でシヨツトキバリア
の面積が小さくなるので、結晶欠陥等で逆方向特
性が悪化する要因の存在確率が低くなり、信頼性
が向上する。尚、n-型の第3の半導体層3の表
面に於ける空乏層の面積の割合は50%以上である
ことが好ましく、80%以上であれば一層好まし
い。
When a positive voltage is applied to the upper electrode metal layer 5 of the shot barrier semiconductor device configured as shown in FIG. 1 to create a forward bias state, the metal layer 5, the third semiconductor layer 3, and the second semiconductor layer 2 , a forward current flows through the path between the first semiconductor layer 1 and the lower metal layer 6.
On the other hand, if, for example, -30V is applied to the upper metal layer 5 to create a reverse bias state, the state between the p + type fourth semiconductor layer 4 and the n - type third semiconductor layer 3 is reverse biased. Therefore, the space charge region, that is, the depletion layer is n - with a width of about 5.1 μ from the p + type fourth semiconductor layer 4.
spreads into the third semiconductor layer 3 of the mold. Since depletion layers extend from both sides of the n - type third semiconductor layer 3, the surface of the n - type third semiconductor layer 3 is eventually filled with the depletion layer due to the -30V reverse voltage. . As a result, the reverse current flowing through the metal layer 5 and the n - type third semiconductor layer 3 is significantly restricted.
The depletion layer extending to the n-type second semiconductor layer 2 directly under the p + -type fourth semiconductor layer 4 is smaller than the spread width of the third semiconductor layer 3 due to the difference in impurity concentration, causing reach-through breakdown. There is still plenty of room left. We have just described the case where the n - type third semiconductor layer 3 is filled with a depletion layer with a reverse bias of -30V.
In the case of a low reverse voltage, the third semiconductor layer 3 is not filled with a depletion layer. However, since it is difficult for reverse current to flow in the region where the depletion layer is formed, the reverse current is suppressed by the amount of the depletion layer. Furthermore, since the area of the shot barrier in the reverse direction is reduced by the extent to which the depletion layer is expanded, the probability of the existence of factors such as crystal defects that deteriorate the reverse direction characteristics is lowered, and reliability is improved. The area ratio of the depletion layer on the surface of the n - type third semiconductor layer 3 is preferably 50% or more, and more preferably 80% or more.

上述から明らかなように、本実施例によれば、
n-型の第3の半導体層3を設けたので、空乏層
の横方向への拡がりが大きくなる。従つて、p+
型の第4の半導体層4の相互間隔即ちn-型の第
3の半導体層3の幅を大きくすることが可能にな
り、この種のシヨツトキバリア半導体装置として
はシヨツトキバリア部分の面積が大きくなつて電
流容量を大きく取れる。換言すれば小さな半導体
チツプで所望の電流容量を得ることが出来る。こ
のため、逆方向及び順方向の両方の特性のよいシ
ヨツトキバリア半導体装置を提供することが出来
る。
As is clear from the above, according to this example,
Since the n - type third semiconductor layer 3 is provided, the depletion layer expands in the lateral direction. Therefore, p +
It becomes possible to increase the mutual spacing between the n - type fourth semiconductor layers 4, that is, the width of the n-type third semiconductor layer 3, and as a result of this type of shot barrier semiconductor device, the area of the shot barrier portion becomes larger and the current flow increases. Large capacity can be obtained. In other words, a desired current capacity can be obtained with a small semiconductor chip. Therefore, it is possible to provide a shot barrier semiconductor device with good characteristics in both the reverse direction and the forward direction.

またイオン注入によつて第3の半導体層3を形
成するので、これを極めて浅く形成することが可
能になる。従つて、順方向特性を良好に保つた状
態で順方向電流を減少させることが出来る。
Furthermore, since the third semiconductor layer 3 is formed by ion implantation, it is possible to form it extremely shallowly. Therefore, the forward current can be reduced while maintaining good forward characteristics.

以上、本考案の実施例について述べたが、本考
案はこれに限定されるものでなく更に変形可能な
ものである。例えば、第3の半導体層3をn-
エピタキシヤル成長層で形成してもよい。また、
第3及び第4の半導体層3,4の平面形状を第3
図又は第4図のように変形してもよい。
Although the embodiments of the present invention have been described above, the present invention is not limited thereto and can be further modified. For example, the third semiconductor layer 3 may be formed of an n - type epitaxial growth layer. Also,
The planar shapes of the third and fourth semiconductor layers 3 and 4 are
It may be modified as shown in the figure or FIG.

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

第1図は本考案の実施例に係わるシヨツトキバ
リア半導体装置の一部を示す断面図、第2図は第
1図の装置の半導体部分の表面を示す平面図であ
る。第3図及び第4図は本考案の変形例に係わる
シヨツトキバリア半導体装置を示す平面図であ
る。 尚図面に用いられている符号に於いて、1は第
1の半導体層、2は第2の半導体層、3は第3の
半導体層、4は第4の半導体層、5は金属層であ
る。
FIG. 1 is a sectional view showing a part of a shot barrier semiconductor device according to an embodiment of the present invention, and FIG. 2 is a plan view showing the surface of the semiconductor portion of the device shown in FIG. 3 and 4 are plan views showing a shot barrier semiconductor device according to a modified example of the present invention. In the symbols used in the drawings, 1 is the first semiconductor layer, 2 is the second semiconductor layer, 3 is the third semiconductor layer, 4 is the fourth semiconductor layer, and 5 is the metal layer. .

Claims (1)

【実用新案登録請求の範囲】 n型又はp型の第1の導電型を有すると共に高
不純物濃度を有する第1の半導体層と、 前記第1の導電型を有すると共に前記第1の半
導体層の不純物濃度よりも低い不純物濃度を有し
て前記第1の半導体層の上に形成された第2の半
導体層と、 前記第1の導電型を有すると共に前記第2の半
導体層の不純物濃度よりも低い不純物濃度を有し
て前記第2の半導体層の上に形成され且つその上
面が半導体基板の表面に露呈している第3の半導
体層と、 その上面が前記半導体基板の表面に露呈し、そ
の下面が前記第2の半導体層に隣接し、その側面
に前記第3の半導体層が隣接するように配設さ
れ、且つ前記第3の半導体層よりも深く形成さ
れ、且つ前記第1の導電型と反対の第2の導電型
を有している第4の半導体層と、 前記第3の半導体層に対してシヨツトキバリア
を形成するように接触し且つ前記第4の半導体層
に対してオーミツクコンタクトを形成するように
接触している金属層と を具備し、前記半導体基板の表面の特定方向の直
線上において前記シヨツトキバリアと前記オーミ
ツクコンタクトが交互に配置されるように前記第
3及び第4の半導体層が配置されていることを特
徴とするシヨツトキバリア半導体装置。
[Claims for Utility Model Registration] A first semiconductor layer having a first conductivity type of n-type or p-type and having a high impurity concentration; a second semiconductor layer formed on the first semiconductor layer having an impurity concentration lower than the impurity concentration; and a second semiconductor layer having the first conductivity type and having an impurity concentration lower than the impurity concentration of the second semiconductor layer. a third semiconductor layer having a low impurity concentration and formed on the second semiconductor layer, the upper surface of which is exposed to the surface of the semiconductor substrate; the upper surface of which is exposed to the surface of the semiconductor substrate; The lower surface is adjacent to the second semiconductor layer, the third semiconductor layer is adjacent to the side surface thereof, and is formed deeper than the third semiconductor layer, and the first conductive layer is formed deeper than the third semiconductor layer. a fourth semiconductor layer having a second conductivity type opposite to that of the semiconductor layer; and a fourth semiconductor layer in contact with the third semiconductor layer to form a shot barrier and in ohmic contact with the fourth semiconductor layer. and a metal layer in contact to form a contact, and the third and fourth contacts are arranged such that the shot barrier and the ohmic contact are alternately arranged on a straight line in a specific direction on the surface of the semiconductor substrate. A shot barrier semiconductor device characterized in that a semiconductor layer is arranged.
JP1982113716U 1982-07-27 1982-07-27 Shock barrier semiconductor device Granted JPS5936264U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1982113716U JPS5936264U (en) 1982-07-27 1982-07-27 Shock barrier semiconductor device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1982113716U JPS5936264U (en) 1982-07-27 1982-07-27 Shock barrier semiconductor device

Publications (2)

Publication Number Publication Date
JPS5936264U JPS5936264U (en) 1984-03-07
JPH0229729Y2 true JPH0229729Y2 (en) 1990-08-09

Family

ID=30263134

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1982113716U Granted JPS5936264U (en) 1982-07-27 1982-07-27 Shock barrier semiconductor device

Country Status (1)

Country Link
JP (1) JPS5936264U (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0750791B2 (en) * 1989-09-20 1995-05-31 株式会社日立製作所 Semiconductor rectifier diode, power supply device using the same, and electronic computer
US7355260B2 (en) * 2004-06-30 2008-04-08 Freescale Semiconductor, Inc. Schottky device and method of forming
US7436022B2 (en) * 2005-02-11 2008-10-14 Alpha & Omega Semiconductors, Ltd. Enhancing Schottky breakdown voltage (BV) without affecting an integrated MOSFET-Schottky device layout
JPWO2012157679A1 (en) * 2011-05-18 2014-07-31 ローム株式会社 Semiconductor device and manufacturing method thereof

Family Cites Families (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS522446A (en) * 1975-06-24 1977-01-10 Ushio Inc Information reading apparatus
JPS528781A (en) * 1975-07-10 1977-01-22 Mitsubishi Electric Corp Schottky barrier diode
JPS5935183B2 (en) * 1975-08-20 1984-08-27 サンケイ電気 (株) Shock barrier semiconductor device
JPS5737886A (en) * 1980-08-20 1982-03-02 Hitachi Ltd Semiconductor device

Also Published As

Publication number Publication date
JPS5936264U (en) 1984-03-07

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