JPH02174263A - Semiconductor protective element - Google Patents
Semiconductor protective elementInfo
- Publication number
- JPH02174263A JPH02174263A JP63330875A JP33087588A JPH02174263A JP H02174263 A JPH02174263 A JP H02174263A JP 63330875 A JP63330875 A JP 63330875A JP 33087588 A JP33087588 A JP 33087588A JP H02174263 A JPH02174263 A JP H02174263A
- Authority
- JP
- Japan
- Prior art keywords
- semiconductor region
- semiconductor
- voltage
- junction
- region
- 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.)
- Pending
Links
Landscapes
- Thyristors (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は半導体保護素子に関し、特に通信機器分暗にお
いて通信ケーブルを通って侵入してくる異常電圧から有
線通信機器を守るための半導体保護素子に関する。[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a semiconductor protection device, and particularly to a semiconductor protection device for protecting wired communication equipment from abnormal voltages that enter through communication cables when the communication equipment is in the dark. Regarding.
従来、この種の半導体保護素子は、第4図の断面図に示
されるように、P型半導体材料からなる第二半導体領域
2及び第三半導体領域3と、N型半導体材料からなる第
一半導体領域l及び第四半導体領域4とのPNPNの四
層と、これに素子の順阻止電圧上昇率dv/dtを大き
くするため第三半導体領域3と第四半導体領域4を短絡
するよう、に設けられたカソード電極7及び第二半導体
領域2とオーミック接触を持つアノード電極6とからな
り、画電極はSiO□膜8に設けられた開口部に形成さ
れている。Conventionally, this type of semiconductor protection element has a second semiconductor region 2 and a third semiconductor region 3 made of a P-type semiconductor material, and a first semiconductor made of an N-type semiconductor material, as shown in the cross-sectional view of FIG. A four-layer PNPN layer including the region 1 and the fourth semiconductor region 4 is provided to short-circuit the third semiconductor region 3 and the fourth semiconductor region 4 in order to increase the forward blocking voltage increase rate dv/dt of the element. The image electrode is formed in an opening provided in the SiO □ film 8 .
このようなデバイス構造を持つ従来の半導体保護素子は
、アノード電極6とカソード電極7との間に第一半導体
領域1と第三半導体領域3からなるPN接合の逆耐圧を
越える異常電圧が印加されると、第二半導体領域2と第
一半導体領域1と第三半導体領域3とからなるPNPの
三層に電流が流れるなだれ降伏状態を経た後、第二半導
体領域2と第一半導体領域1と第三半導体領域3と第四
半導体領域4とのPNPN四層からなるサイリスタがオ
ン状態に入って異常電圧を吸収するようになっていた。In a conventional semiconductor protection element having such a device structure, an abnormal voltage exceeding the reverse withstand voltage of the PN junction consisting of the first semiconductor region 1 and the third semiconductor region 3 is applied between the anode electrode 6 and the cathode electrode 7. Then, after passing through an avalanche breakdown state in which current flows in the three layers of PNP consisting of the second semiconductor region 2, first semiconductor region 1, and third semiconductor region 3, the second semiconductor region 2 and the first semiconductor region 1 The thyristor, which is made up of four PNPN layers including the third semiconductor region 3 and the fourth semiconductor region 4, enters the on state and absorbs the abnormal voltage.
上述した従来の半導体保護素子では、そのブレークダウ
ン電圧VBRは第一半導体領域1と第三半導体領域3に
より形成されるPN接合の降伏電圧により定まると考え
られていた。In the conventional semiconductor protection element described above, the breakdown voltage VBR was thought to be determined by the breakdown voltage of the PN junction formed by the first semiconductor region 1 and the third semiconductor region 3.
しかしながら実際には、第4図に示したデバイス構造か
らもわかるように、アノード電極6とカソード電8i!
7間に印加される電圧は第一半導体領域1と第三半導体
領域3とからなるPN接合だけでなく、第二半導体領域
2をも含んだPNP三層に対して加わることになる。However, in reality, as can be seen from the device structure shown in FIG. 4, the anode electrode 6 and the cathode electrode 8i!
The voltage applied across 7 is applied not only to the PN junction consisting of the first semiconductor region 1 and the third semiconductor region 3 but also to the PNP three layers including the second semiconductor region 2.
このため、今第−半導体領域1と第三半導体領域3とか
らなるPN接合の降伏電圧をV2Cとすると、この半導
体保護素子のブレークダウン電圧V8Rは一般に V
BR= V zo ”!ゴー]1 と表わされる値とな
る。ここでnは定数で、Stでは通常3である。又、α
FはPNP三層をトランジスタとみなした時の順方向電
流伝達率である。Therefore, if the breakdown voltage of the PN junction consisting of the first semiconductor region 1 and the third semiconductor region 3 is V2C, then the breakdown voltage V8R of this semiconductor protection element is generally V8R.
The value is expressed as BR = V zo "! Go] 1. Here, n is a constant, which is usually 3 in St. Also, α
F is the forward current transfer rate when the three PNP layers are considered as a transistor.
すなわち、従来構造の半導体保護素子においては、その
ブレークダウン電圧は第一半導体領域1と第三半導体領
域3によるPN接合の降伏電圧だけでなく、第二半導体
領域2をも含んだPNP三層のトランジスタ特性の影響
も受けてしまうことになる。In other words, in the semiconductor protection element with the conventional structure, the breakdown voltage is not only the breakdown voltage of the PN junction between the first semiconductor region 1 and the third semiconductor region 3, but also the breakdown voltage of the PNP three layer including the second semiconductor region 2. It will also be affected by transistor characteristics.
しかも、従来のなだれ降伏状態での電圧−電流特性は、
第5図のグラフに示すような負抵抗特性となるため、立
ち上がり速度の遅い異常電圧に対してはブレークダウン
電圧VBRで制限される電圧でオン状態に入るが、立ち
上がり速度の速い異常電圧に対してはブレークダウン電
圧VBRが保持できず、ブレークオーバ電圧■Boで制
限される電圧でオン状態に入ってしまい、すなわち印加
電圧の立ち上がり速度によりオン電圧に入る制限電圧が
2分極化してしまうという欠点もある。Moreover, the voltage-current characteristics in the conventional avalanche breakdown state are
Since it has a negative resistance characteristic as shown in the graph of Figure 5, it enters the ON state at a voltage limited by the breakdown voltage VBR in response to an abnormal voltage with a slow rise speed, but it enters the ON state at a voltage limited by the breakdown voltage VBR, but in response to an abnormal voltage with a fast rise speed. The disadvantage is that the breakdown voltage VBR cannot be maintained and the ON state is entered at a voltage limited by the breakover voltage Bo, which means that the limiting voltage that enters the ON voltage becomes bipolarized depending on the rising speed of the applied voltage. There is also.
本発明は、N型半導体材料で形成された第一半導体領域
と、前記第一半導体領域の両表面のうちの一方の面とP
N接合を形成するP型半導体材料で形成された第二半導
体領域と、前記第一半導体領域の両表面のうちの他方の
面とPN接合を形成するP型半導体材料で形成された第
三半導体領域と、前記第三半導体領域の表面の一部分と
PN接合を形成するN型半導体材料で形成された第四半
導体領域と、前記第二半導体領域とオーミック接触を持
つアノード電極と、前記第三半導体領域と第四半導体領
域の両領域とオーミック接触を持つカソード電極とから
なる半導体保護素子において、前記第二半導体領域を突
き抜けて前記アノード電極と前記第一半導体領域とを短
絡するN型半導体材料で形成された第五半導体領域を設
けた半導体保護素子である。The present invention includes a first semiconductor region formed of an N-type semiconductor material, one surface of both surfaces of the first semiconductor region, and a P
a second semiconductor region formed of a P-type semiconductor material forming an N-junction; and a third semiconductor formed of a P-type semiconductor material forming a PN-junction with the other of both surfaces of the first semiconductor region. a fourth semiconductor region formed of an N-type semiconductor material forming a PN junction with a portion of the surface of the third semiconductor region, an anode electrode having ohmic contact with the second semiconductor region, and the third semiconductor region. and a cathode electrode having ohmic contact with both the fourth semiconductor region and the fourth semiconductor region, the N-type semiconductor material penetrating the second semiconductor region and short-circuiting the anode electrode and the first semiconductor region. It is a semiconductor protection element provided with a formed fifth semiconductor region.
次に本発明について図面を参照して説明する。 Next, the present invention will be explained with reference to the drawings.
第1図は本発明の一実施例を示す半導体保護素子の断面
図である。第二半導体領域2の一部分に表面からN型不
純物を第一半導体領域1に達するまで押し込んだ第五半
導体領域5を形成し、この第五半導体領域5と第二半導
体領域2の両方にオーミック接触を持つようにアノード
電極6を作っである。FIG. 1 is a sectional view of a semiconductor protection element showing an embodiment of the present invention. A fifth semiconductor region 5 is formed in a part of the second semiconductor region 2 by pushing N-type impurities from the surface until it reaches the first semiconductor region 1, and ohmic contact is made with both the fifth semiconductor region 5 and the second semiconductor region 2. The anode electrode 6 is made so as to have the following properties.
すなわち、本発明の半導体保護素子では、アノード電f
i6は第二半導体領域2だけでなく第−半導体領域1と
もオーミック接触を持っている。この構造においては、
オン状態においてアノード電極6とカソード電極7に印
加される電圧は、直接第一半導体領域1と第三半導体領
域3で形成されるPN接合に逆方向に加わることになる
。That is, in the semiconductor protection device of the present invention, the anode voltage f
i6 has ohmic contact not only with the second semiconductor region 2 but also with the -th semiconductor region 1. In this structure,
The voltage applied to the anode electrode 6 and the cathode electrode 7 in the on state is directly applied to the PN junction formed by the first semiconductor region 1 and the third semiconductor region 3 in the opposite direction.
このため、このPN接合の逆耐圧がそのまま半導体保護
素子のブレークダウン電圧VBRとなり、第二半導体領
域2とは無関係に定めることができる。第2図は本発明
の半導体保護素子の電圧−電流特性を示すグラフである
。第2図に示すように、そのなだれ降伏状態もPN接合
の逆方向電圧電流特性となるため負抵抗特性とはならず
、よって半導体保護素子がオン状態に入る制限電圧はブ
レークオーバ電圧VBOのみで決まり2分極化すること
もない。Therefore, the reverse breakdown voltage of this PN junction directly becomes the breakdown voltage VBR of the semiconductor protection element, and can be determined independently of the second semiconductor region 2. FIG. 2 is a graph showing the voltage-current characteristics of the semiconductor protection device of the present invention. As shown in Figure 2, the avalanche breakdown state also has the reverse voltage-current characteristics of a PN junction, so it does not have a negative resistance characteristic, so the limiting voltage at which the semiconductor protection device turns on is only the breakover voltage VBO. There is no obvious polarization.
又、本発明の半導体保護素子は逆電圧に対してはダイオ
ード特性になるため、保護素子として必要な双方向特性
を得たい時は、単にこのデバイスを逆向きに直列につな
ぐだけで双方向特性を得ることもできる。In addition, since the semiconductor protection device of the present invention has diode characteristics with respect to reverse voltage, if you want to obtain the bidirectional characteristics necessary for a protection device, simply connect this device in series in the opposite direction to obtain the bidirectional characteristics. You can also get
第3図は本発明の応用例を示す断面図である。FIG. 3 is a sectional view showing an example of application of the present invention.
この応用例では、第一半導体領域1と第三半導体領域3
で形成されるPN接合の表面部分に、N型の不純物を押
し込んだ第六半導体領域9を形成し、この部分の不純物
濃度により第一半導体領域1と第三半導体領域3で形成
されるPN接合の逆耐圧、すなわち半導体保護素子のブ
レークダウン電圧を制御できるようにしたものである。In this application example, first semiconductor region 1 and third semiconductor region 3
A sixth semiconductor region 9 in which N-type impurities are pushed is formed in the surface part of the PN junction formed by the PN junction formed by the first semiconductor region 1 and the third semiconductor region 3 due to the impurity concentration in this part. This makes it possible to control the reverse breakdown voltage of the semiconductor protection element, that is, the breakdown voltage of the semiconductor protection element.
以上説明したように本発明は、第一〜第四半導体領域か
らなる半導体保護素子に第五半導体領域を作ることによ
り1.半導体保護素子のブレークダウン電圧が第一半導
体領域と第三半導体領域により形成されるPN接合の逆
耐圧のみで決まり、しかも立ち上がり速度の速い印加電
圧に対しても一定の制限電圧でオン状態に入ることがで
きるようになるという効果がある。As explained above, the present invention provides 1. a. The breakdown voltage of the semiconductor protection element is determined only by the reverse withstand voltage of the PN junction formed by the first semiconductor region and the third semiconductor region, and it enters the ON state at a certain limited voltage even for applied voltages that rise quickly. This has the effect of making it possible to
第1図は本発明の一実施例を示す断面図、第2図は本発
明の半導体保護素子の電圧−電流特性を示すグラフ、第
3図は本発明の応用例を示す断面図、第4図は従来の半
導体保護素子の断面図、第5図は従来の半導体保護素子
の電圧−電流特性を示すグラフである。
1・・・第一半導体領域、2・・・第二半導体領域、3
・・・第三半導体領域、4・・・第四半導体領域、5・
・・第五半導体領域、6・・・アノード電極、7・・・
カソード電極、8・・・5i02膜、9・・・第六半導
体°領域。FIG. 1 is a sectional view showing an embodiment of the present invention, FIG. 2 is a graph showing voltage-current characteristics of a semiconductor protection element of the present invention, FIG. The figure is a cross-sectional view of a conventional semiconductor protection element, and FIG. 5 is a graph showing voltage-current characteristics of the conventional semiconductor protection element. 1... First semiconductor region, 2... Second semiconductor region, 3
... third semiconductor region, 4... fourth semiconductor region, 5.
...Fifth semiconductor region, 6... Anode electrode, 7...
Cathode electrode, 8...5i02 film, 9...6th semiconductor region.
Claims (1)
一半導体領域の両表面のうちの一方の面とPN接合を形
成するP型半導体材料で形成された第二半導体領域と、
前記第一半導体領域の両表面のうちの他方の面とPN接
合を形成するP型半導体材料で形成された第三半導体領
域と、前記第三半導体領域の表面の一部分とPN接合を
形成するN型半導体材料で形成された第四半導体領域と
、前記第二半導体領域とオーミック接触を持つアノード
電極と、前記第三半導体領域と第四半導体領域の両領域
とオーミック接触を持つカソード電極とからなる半導体
保護素子において、前記第二半導体領域を突き抜けて前
記アノード電極と前記第一半導体領域とを短絡するN型
半導体材料で形成された第五半導体領域を設けたことを
特徴とする半導体保護素子。a first semiconductor region formed of an N-type semiconductor material; a second semiconductor region formed of a P-type semiconductor material forming a PN junction with one of both surfaces of the first semiconductor region;
a third semiconductor region formed of a P-type semiconductor material forming a PN junction with the other of both surfaces of the first semiconductor region; and an N-type semiconductor region forming a PN junction with a portion of the surface of the third semiconductor region. a fourth semiconductor region formed of a type semiconductor material, an anode electrode having ohmic contact with the second semiconductor region, and a cathode electrode having ohmic contact with both the third semiconductor region and the fourth semiconductor region. 1. A semiconductor protection element, further comprising a fifth semiconductor region made of an N-type semiconductor material that penetrates through the second semiconductor region and short-circuits the anode electrode and the first semiconductor region.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63330875A JPH02174263A (en) | 1988-12-27 | 1988-12-27 | Semiconductor protective element |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63330875A JPH02174263A (en) | 1988-12-27 | 1988-12-27 | Semiconductor protective element |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH02174263A true JPH02174263A (en) | 1990-07-05 |
Family
ID=18237491
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP63330875A Pending JPH02174263A (en) | 1988-12-27 | 1988-12-27 | Semiconductor protective element |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH02174263A (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH04320067A (en) * | 1991-04-18 | 1992-11-10 | Agency Of Ind Science & Technol | Surge protective device |
| JP2011249601A (en) * | 2010-05-27 | 2011-12-08 | Shindengen Electric Mfg Co Ltd | Short circuit thyristor |
-
1988
- 1988-12-27 JP JP63330875A patent/JPH02174263A/en active Pending
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH04320067A (en) * | 1991-04-18 | 1992-11-10 | Agency Of Ind Science & Technol | Surge protective device |
| JP2011249601A (en) * | 2010-05-27 | 2011-12-08 | Shindengen Electric Mfg Co Ltd | Short circuit thyristor |
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