JPS6022379A - Semiconductor device - Google Patents
Semiconductor deviceInfo
- Publication number
- JPS6022379A JPS6022379A JP13141383A JP13141383A JPS6022379A JP S6022379 A JPS6022379 A JP S6022379A JP 13141383 A JP13141383 A JP 13141383A JP 13141383 A JP13141383 A JP 13141383A JP S6022379 A JPS6022379 A JP S6022379A
- Authority
- JP
- Japan
- Prior art keywords
- type layer
- type
- oscillation
- single crystal
- avalanche
- 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
- 239000004065 semiconductor Substances 0.000 title claims abstract description 14
- 239000013078 crystal Substances 0.000 claims abstract description 9
- 230000010355 oscillation Effects 0.000 claims abstract description 9
- 239000012535 impurity Substances 0.000 claims abstract description 8
- 238000009751 slip forming Methods 0.000 claims abstract description 4
- 230000000694 effects Effects 0.000 claims description 5
- 238000000034 method Methods 0.000 abstract description 5
- 230000002194 synthesizing effect Effects 0.000 abstract 2
- 230000001960 triggered effect Effects 0.000 abstract 2
- 238000007796 conventional method Methods 0.000 abstract 1
- 230000001419 dependent effect Effects 0.000 abstract 1
- 230000015572 biosynthetic process Effects 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 238000003786 synthesis reaction Methods 0.000 description 2
- 230000007423 decrease Effects 0.000 description 1
- PCHJSUWPFVWCPO-UHFFFAOYSA-N gold Chemical compound [Au] PCHJSUWPFVWCPO-UHFFFAOYSA-N 0.000 description 1
- 239000010931 gold Substances 0.000 description 1
- 229910052737 gold Inorganic materials 0.000 description 1
- 239000007791 liquid phase Substances 0.000 description 1
- 239000000758 substrate Substances 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L29/00—Semiconductor devices specially adapted for rectifying, amplifying, oscillating or switching and having potential barriers; Capacitors or resistors having potential barriers, e.g. a 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
- H01L29/864—Transit-time diodes, e.g. IMPATT, TRAPATT diodes
Landscapes
- Engineering & Computer Science (AREA)
- Microelectronics & Electronic Packaging (AREA)
- Power Engineering (AREA)
- Physics & Mathematics (AREA)
- Ceramic Engineering (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- General Physics & Mathematics (AREA)
- Computer Hardware Design (AREA)
- Semiconductor Lasers (AREA)
Abstract
Description
【発明の詳細な説明】
〔発明の属する技術分野〕
本発明は半導体装置に関し、特にアバ2ンシエ効果を利
用する高周波、晶出力の半導体装置1C関する。DETAILED DESCRIPTION OF THE INVENTION [Technical Field to which the Invention Pertains] The present invention relates to a semiconductor device, and particularly to a high frequency, crystal output semiconductor device 1C that utilizes the abancié effect.
PN接合あるいはショットキー接合部に2けるアバラン
シェ効果を利用したインパソトダイメードはマイクロ波
同体発振源として非常に重要な素子である。他の素子と
同様高周波化、高出力化が望まれて29、例えば高出力
化の為にチップを並列aるいは直列に接続するという試
みがなされている。しかしながら、並列接続はlチップ
の電極面積を大きくする事とほぼ同じで、接続個数ヶ増
せばそれだけ素子のインピーダンスが下がり外部回路と
の整合が困難になる。これに対し、直列接続は、逆に接
続個数を増すほどインピーダンスが上が9外部回路との
整合が容易になる。このように、外部回路との整合とい
う点では町らかに直列接続の方が有利なのであるが、一
方組立ての容易さという点では直列にチップを接続す/
)事は並列接続に比べてはるかに困難である。また、チ
ップを接続するリード線の浮遊インダクタンスの為に出
力甘酸がうまく行なわれないなどの欠点がめった。The Impasso Dimade, which utilizes the avalanche effect in the PN junction or Schottky junction, is a very important element as a microwave homogeneous oscillation source. As with other devices, higher frequencies and higher outputs are desired29. For example, attempts have been made to connect chips in parallel or in series in order to increase output. However, parallel connection is almost the same as increasing the electrode area of the l-chip, and as the number of connected elements increases, the impedance of the element decreases and matching with an external circuit becomes difficult. On the other hand, in series connection, as the number of connected devices increases, impedance increases and matching with an external circuit becomes easier. In this way, serial connection is more advantageous in terms of matching with external circuits, but on the other hand, in terms of ease of assembly, it is better to connect chips in series.
) is much more difficult than parallel connection. In addition, there were many shortcomings, such as poor output control due to the stray inductance of the lead wires connecting the chips.
本発明の目的は、上記欠点を除去し、組立が容易で、出
力合成を改良した高周波高出力の半導体装置全提供する
ことlC6る。SUMMARY OF THE INVENTION An object of the present invention is to provide a high-frequency, high-output semiconductor device that eliminates the above-mentioned drawbacks, is easy to assemble, and has improved output synthesis.
本ビ明の半導体装置は、PN接合を有しアバランシェ効
果を利用する半導体装置において、アバランシェ発振が
可能な不純物濃度分布を持つP凰とN型との2層からな
る1組の半導体単結晶層が2組以上繰返し連続的に形成
され、前記単結晶層が発振素子として直列に接続されて
構成される。The semiconductor device of the present invention is a semiconductor device having a PN junction and utilizing an avalanche effect, which includes a pair of semiconductor single crystal layers consisting of two layers of P-type and N-type, each having an impurity concentration distribution capable of avalanche oscillation. Two or more sets of single crystal layers are repeatedly and continuously formed, and the single crystal layers are connected in series as an oscillation element.
次に、本発明の実施例について、図面を参照して説明す
る。Next, embodiments of the present invention will be described with reference to the drawings.
第1図は本発明の一実施例の不純物濃度分布を示す図で
るる。図において、縦軸は不純物濃度の絶対筒、横軸は
表面からの距離である。N+は低抵抗N型半導体基板で
、この上のN−の高抵抗N型層がエピタキシャル成長に
工9形成され、高抵抗N型層に重ねて、P+である低抵
抗P型層が同じくエピタキシャル成長に工9形gされて
いる。FIG. 1 is a diagram showing an impurity concentration distribution in one embodiment of the present invention. In the figure, the vertical axis is the absolute cylinder of impurity concentration, and the horizontal axis is the distance from the surface. N+ is a low-resistance N-type semiconductor substrate, on which a high-resistance N-type layer is epitaxially grown, and a low-resistance P-type layer, P+, is also epitaxially grown over the high-resistance N-type layer. It has a type 9 g.
前記Nm層及びPm層は更に繰返し成長され、都合3回
連続的に成長されている。各々のN型層とP型層とから
成る組は発振領域會形成し、本災施例ではSDR(Si
ngle DrifO型インバツインバットダイオード
濃度分布と同じで、例えば発振周波数が10GHzの場
合は、N型層の厚さ、fA度及びP型層の厚さ、濃度は
各々5〜6μm、 8 X 10”5cInシ及び2〜
3μm、 10 tyn に選べばよい。The Nm layer and Pm layer are further grown repeatedly, three times in total. Each set consisting of an N-type layer and a P-type layer forms an oscillation region, and in this disaster example, an SDR (Si
Same as the concentration distribution of DrifO type inva-in-butt diode, for example, when the oscillation frequency is 10 GHz, the thickness of the N-type layer, fA degree, and the thickness and concentration of the P-type layer are each 5 to 6 μm, 8 x 10" 5cInshi and 2~
It is sufficient to select 3 μm and 10 tyn.
この場合、従来の81)R型インパッドダイオードが3
個直列に接続されたものが1チツプでできることになる
。結晶の成長はスライディングボート法による液相成長
やMBE(molecular BeatnEp 1t
axy)等で行えばよい。In this case, the conventional 81) R type in-pad diode is
This means that devices connected in series can be made with one chip. Crystal growth is carried out by liquid phase growth using the sliding boat method or MBE (molecular beatnEp 1t).
axy) etc.
なお、N型及びP型層の不純物濃度分布を変えることに
エリDDR(Double pri ft)型インバッ
トダイオード、リード型インバットダイオードの1チツ
プ内での直列接続化ができることは以上の説明から明ら
かである。It is clear from the above explanation that by changing the impurity concentration distribution of the N-type and P-type layers, it is possible to connect a DDR (Double pre ft) type invat diode and a lead type invat diode in series within one chip. It is.
以上説明したように、本発明に工れば、従来のチップで
の直列接続に見られた組立の困難性、接続リード線の浮
遊インダクタンスによる出力合成の困難性等の欠点が除
去され、出力合成がうまく行われる高周波高出力の半導
体装置が得られる。As explained above, the present invention eliminates the drawbacks of conventional serial connection of chips, such as difficulty in assembly and difficulty in output synthesis due to stray inductance of connection lead wires, and A high-frequency, high-output semiconductor device in which this process is successfully performed can be obtained.
第1図は本発明の一実施例の不純物@度分布金示す図で
ある。
\−1
¥1ヅFIG. 1 is a diagram showing the impurity @degree distribution of gold according to an embodiment of the present invention. \−1 ¥1ヅ
Claims (1)
において、アバランシェ発振が可能な不純物濃度分布t
もつP型とN型との2層からなる1組の半導体単結晶層
が2組以上繰返し連続的に形成され、前記単結晶層が発
振素子として直列に接続されていること?!−特徴とす
る半導体装置。In a semiconductor device that has a PN junction and utilizes the avalanche effect, impurity concentration distribution t that allows avalanche oscillation
Two or more sets of semiconductor single crystal layers consisting of two layers, P type and N type, are repeatedly and continuously formed, and the single crystal layers are connected in series as an oscillation element? ! -Featured semiconductor device.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP13141383A JPS6022379A (en) | 1983-07-19 | 1983-07-19 | Semiconductor device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP13141383A JPS6022379A (en) | 1983-07-19 | 1983-07-19 | Semiconductor device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS6022379A true JPS6022379A (en) | 1985-02-04 |
Family
ID=15057385
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP13141383A Pending JPS6022379A (en) | 1983-07-19 | 1983-07-19 | Semiconductor device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS6022379A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPWO2018225855A1 (en) * | 2017-06-09 | 2020-04-09 | 株式会社Uacj | Semiconductor layer, oscillation element, and method of manufacturing semiconductor layer |
-
1983
- 1983-07-19 JP JP13141383A patent/JPS6022379A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPWO2018225855A1 (en) * | 2017-06-09 | 2020-04-09 | 株式会社Uacj | Semiconductor layer, oscillation element, and method of manufacturing semiconductor layer |
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