JPH028059U - - Google Patents

Info

Publication number
JPH028059U
JPH028059U JP7016589U JP7016589U JPH028059U JP H028059 U JPH028059 U JP H028059U JP 7016589 U JP7016589 U JP 7016589U JP 7016589 U JP7016589 U JP 7016589U JP H028059 U JPH028059 U JP H028059U
Authority
JP
Japan
Prior art keywords
layer
resistance
electric field
substrate
resistance layer
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
Application number
JP7016589U
Other languages
Japanese (ja)
Other versions
JPH051085Y2 (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
Application filed filed Critical
Priority to JP1989070165U priority Critical patent/JPH051085Y2/ja
Publication of JPH028059U publication Critical patent/JPH028059U/ja
Application granted granted Critical
Publication of JPH051085Y2 publication Critical patent/JPH051085Y2/ja
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Bipolar Transistors (AREA)

Description

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

第1図イは従来の半導体装置、ロは動作時の直
流的な電界強度分布の様子をいろいろな場合につ
いて示したもの、第2図は本考案の半導体装置の
実施例でイはその構造、ロはマイクロ波以上のダ
イオード構造、ハは本考案の半導体装置を発振器
として応用した実施例、第3図は本考案の半導体
装置の動作を説明するもので、イは直流バイアス
での電界強度分布、ロはトンネル注入されたキヤ
リアの空乏層端での電界強度分布の変化を示して
いるものであり、第4図は本考案の別の実施例、
第5図イは本考案の実施例で合金拡散法によるも
のであり、ロは不純物密度分布であり、第6図は
本考案の実施例でトンネル注入部を禁制帯幅の小
さな半導体で構成し、走行層はガン効果を示す半
導体で形成されたヘテロ接合型のものである。
Figure 1A shows a conventional semiconductor device; B shows a diode structure for microwaves or higher, C shows an example in which the semiconductor device of the present invention is applied as an oscillator, Figure 3 explains the operation of the semiconductor device of the present invention, and A shows electric field intensity distribution under DC bias. , b show changes in the electric field intensity distribution at the edge of the depletion layer of tunnel-injected carriers, and Fig. 4 shows another embodiment of the present invention.
Figure 5A shows an embodiment of the present invention using the alloy diffusion method, B shows the impurity density distribution, and Figure 6 shows an embodiment of the invention in which the tunnel injection part is constructed of a semiconductor with a small forbidden band width. , the running layer is of a heterojunction type made of a semiconductor exhibiting the Gunn effect.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 基板上に電子遷移効果を有する半導体で比
較的高抵抗な層を設け、その上に前記高抵抗な層
よりも低抵抗なn層を1層以上設け、さらにその
上にn層とp層を設けた構造を有し、p
接合に逆方向バイアス電圧を印加したとき生
ずるトンネル注入効果により電子群が前記n層に
注入され、前記n層及び高抵抗層に生ずる電界に
より、電子群は走行し、前記n基板近傍の高抵
抗層内で電界が小さくなることにより電子群の走
行速度が飽和速度以下になる点とn基板との間
の距離よりも、前記高抵抗層が厚く、高抵抗層中
でトンネル注入された電子の一部が、負微分移動
度の電界領域となることを特徴とする超高周波半
導体装置。
A relatively high-resistance semiconductor layer having an electronic transition effect is provided on an n + substrate, one or more n-layers having a lower resistance than the high-resistance layer are provided on the layer, and an n + layer is further provided on top of the n-layer. It has a structure with a p + layer, and a p +
A group of electrons is injected into the n layer due to the tunnel injection effect that occurs when a reverse bias voltage is applied to the n + junction, and the electron group travels due to the electric field generated in the n layer and the high resistance layer, and near the n + substrate. The high-resistance layer is thicker than the distance between the n + substrate and the point where the traveling speed of the electron group becomes below the saturation speed due to the electric field becoming smaller in the high-resistance layer. An ultra-high frequency semiconductor device characterized in that a part of the electrons generated becomes an electric field region with negative differential mobility.
JP1989070165U 1989-06-15 1989-06-15 Expired - Lifetime JPH051085Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1989070165U JPH051085Y2 (en) 1989-06-15 1989-06-15

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1989070165U JPH051085Y2 (en) 1989-06-15 1989-06-15

Publications (2)

Publication Number Publication Date
JPH028059U true JPH028059U (en) 1990-01-18
JPH051085Y2 JPH051085Y2 (en) 1993-01-12

Family

ID=31295424

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1989070165U Expired - Lifetime JPH051085Y2 (en) 1989-06-15 1989-06-15

Country Status (1)

Country Link
JP (1) JPH051085Y2 (en)

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS4929777A (en) * 1972-07-18 1974-03-16
JPS5458379A (en) * 1977-10-18 1979-05-11 Matsushita Electronics Corp Avalanche diode

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS4929777A (en) * 1972-07-18 1974-03-16
JPS5458379A (en) * 1977-10-18 1979-05-11 Matsushita Electronics Corp Avalanche diode

Also Published As

Publication number Publication date
JPH051085Y2 (en) 1993-01-12

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