JPS604871A - Method for measuring saturated current of semiconductor apparatus - Google Patents
Method for measuring saturated current of semiconductor apparatusInfo
- Publication number
- JPS604871A JPS604871A JP11313583A JP11313583A JPS604871A JP S604871 A JPS604871 A JP S604871A JP 11313583 A JP11313583 A JP 11313583A JP 11313583 A JP11313583 A JP 11313583A JP S604871 A JPS604871 A JP S604871A
- Authority
- JP
- Japan
- Prior art keywords
- current
- voltage
- gradient
- point
- saturated current
- 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 13
- 238000000034 method Methods 0.000 title claims abstract description 8
- 229920006395 saturated elastomer Polymers 0.000 title abstract 5
- 229910001218 Gallium arsenide Inorganic materials 0.000 abstract description 3
- 238000005259 measurement Methods 0.000 abstract 1
- 238000010586 diagram Methods 0.000 description 5
- 238000000691 measurement method Methods 0.000 description 2
- 230000010355 oscillation Effects 0.000 description 2
- 230000007423 decrease Effects 0.000 description 1
Landscapes
- Testing Of Individual Semiconductor Devices (AREA)
Abstract
Description
【発明の詳細な説明】 本発明は半導体装置の飽和電流測定方法に関する。[Detailed description of the invention] The present invention relates to a method for measuring saturation current of a semiconductor device.
半導体装置の飽和電流自動測定方法の原理は、第1図の
電流−電圧特性曲線図に示すように、飽和点より十分高
い電圧Aの電圧パルスを供試半導体装置に印加し、その
時の電流Bを表示することによってめられる。しかし、
第2図の電流−電圧特性曲線図に示すように、ガンダイ
オード、あるいはGaAs FETのように、飽和電流
領域において発振Voscの起る半導体装置の場合には
、第1図に示す方法では飽和電流は測定できない。The principle of the method for automatically measuring the saturation current of a semiconductor device is that, as shown in the current-voltage characteristic curve diagram in Figure 1, a voltage pulse of voltage A that is sufficiently higher than the saturation point is applied to the semiconductor device under test, and the current B at that time is It can be recognized by displaying . but,
As shown in the current-voltage characteristic curve diagram in Figure 2, in the case of semiconductor devices such as Gunn diodes or GaAs FETs where oscillation Vosc occurs in the saturation current region, the method shown in Figure 1 cannot be measured.
本発明の目的は、飽和電流領域において発振を起す半導
体装置においても適用可能な半導体装置の飽和電流測定
方法を提供することにある。An object of the present invention is to provide a method for measuring the saturation current of a semiconductor device, which is applicable even to semiconductor devices that cause oscillation in the saturation current region.
第2図は本発明の詳細な説明するための電流−電圧特性
曲線図である。図において、横軸のAI。FIG. 2 is a current-voltage characteristic curve diagram for explaining the present invention in detail. In the figure, the horizontal axis is AI.
A、、A、、・・・・・・に対応する電圧パルスを供試
半導体装置に印加し、順次その勾配、ΔB/△Ai測定
してゆく。勾配は、電圧の低い場合には比較的大きいが
゛、電圧が大きくなるにしたがって勾配はしだいに低下
してゆく。この勾配の大きさに一定の規格をもうけてお
き、勾配が規格値以下になった点の電流値を飽和電流と
するものである。Voltage pulses corresponding to A, , A, . . . are applied to the semiconductor device under test, and their slopes, ΔB/ΔAi, are sequentially measured. The slope is relatively large at low voltages, but gradually decreases as the voltage increases. A certain standard is established for the magnitude of this slope, and the current value at the point where the slope becomes less than the standard value is defined as the saturation current.
第2図の例ではB6が飽和電流になる。In the example of FIG. 2, B6 becomes the saturation current.
本発明の測定方法を用いれば、ガンダイオードGaAs
FBT等の飽和電流を容易に測定することができる。If the measurement method of the present invention is used, the Gunn diode GaAs
The saturation current of FBT etc. can be easily measured.
第1図は従来の飽和電流測定方法を説明するための供試
半導体装置の電流−電圧特性曲線図、第2図は本発明の
一実施例を説明するための供試半導体装置の電流−電圧
特性曲線図である。
AI A11 A2.・・・、・・・・・・印加パルス
電圧、 B、B、。
B2.・・・、・・・・・・印加パルス電圧によるパル
ス電流。
C万−
箭 1図
:ぎ圧−
第 Z 図FIG. 1 is a current-voltage characteristic curve diagram of a semiconductor device under test for explaining a conventional saturation current measurement method, and FIG. 2 is a current-voltage characteristic curve of a semiconductor device under test for explaining an embodiment of the present invention. It is a characteristic curve diagram. AI A11 A2. ..., ...applied pulse voltage, B, B,. B2. ..., ...Pulse current due to applied pulse voltage. C 10,000 - Yasushi Figure 1: Pressure - Figure Z
Claims (1)
い点より順次測定してゆき、その勾配の大ききが一定値
以下になった点の電流値を飽和電流とすることを特徴と
する半導体装置の飽和電流測定方法。The method is characterized in that the slope of the current-voltage characteristic of the semiconductor device under test is sequentially measured starting from the point with the lowest voltage, and the current value at the point where the magnitude of the slope becomes less than a certain value is taken as the saturation current. Method for measuring saturation current of semiconductor devices.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP11313583A JPS604871A (en) | 1983-06-23 | 1983-06-23 | Method for measuring saturated current of semiconductor apparatus |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP11313583A JPS604871A (en) | 1983-06-23 | 1983-06-23 | Method for measuring saturated current of semiconductor apparatus |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS604871A true JPS604871A (en) | 1985-01-11 |
Family
ID=14604434
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP11313583A Pending JPS604871A (en) | 1983-06-23 | 1983-06-23 | Method for measuring saturated current of semiconductor apparatus |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS604871A (en) |
-
1983
- 1983-06-23 JP JP11313583A patent/JPS604871A/en active Pending
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