JPH0850161A - Measuring method of semiconductor device - Google Patents

Measuring method of semiconductor device

Info

Publication number
JPH0850161A
JPH0850161A JP6184434A JP18443494A JPH0850161A JP H0850161 A JPH0850161 A JP H0850161A JP 6184434 A JP6184434 A JP 6184434A JP 18443494 A JP18443494 A JP 18443494A JP H0850161 A JPH0850161 A JP H0850161A
Authority
JP
Japan
Prior art keywords
frequency
yadj
adj
measuring
gain
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
Application number
JP6184434A
Other languages
Japanese (ja)
Inventor
Koji Okada
浩治 岡田
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electronics Corp
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 by Matsushita Electronics Corp filed Critical Matsushita Electronics Corp
Priority to JP6184434A priority Critical patent/JPH0850161A/en
Publication of JPH0850161A publication Critical patent/JPH0850161A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To provide a measuring method of cut-off frequency in which the number of measuring points can be reduced while keeping the measuring precision, and the measuring time can be shortened. CONSTITUTION:Respective gains yL, yH in two minimum and maximum frequencies xL, xH of a measuring frequency range for conforming a gain to a prescribed value yADJ are measured. The approximate value x'ADJ of frequency for conforming the gain to the prescribed value yADJ is arithmetically determined by linear approximation. When the approximate value x'ADJ of frequency determined by linear approximation is largely different from xADJ which is the actual frequency value, the frequency characteristic is assumed to be a broken line to approximate it. Namely, optional frequencies x1, x2 are taken between xL and xH, and gains yL, y1, y2, yH in the respective frequencies yADJ measured It is then confirmed between which gains yADJ is situated. In this case, since yADJ is between yL and y1, the approximate value x'ADJ in yADJ is arithmetically determined by linear approximation.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】この発明は周波数特性および非直
線特性を有する半導体デバイスの測定方法に関するもの
である。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method for measuring a semiconductor device having frequency characteristics and non-linear characteristics.

【0002】[0002]

【従来の技術】半導体デバイスの出力信号における周波
数特性であるカットオフ周波数の測定をする場合、折れ
点である−3dB点に一致する周波数を見つけ出さなけ
ればならない。
2. Description of the Related Art When measuring a cutoff frequency, which is a frequency characteristic of an output signal of a semiconductor device, it is necessary to find a frequency corresponding to a -3 dB point which is a break point.

【0003】従来の方法としては、図3に示すように、
まず周波数の測定範囲を等間隔にn分割(図3ではn=
10とした)し、それぞれの周波数に対する利得を測定
し、所定の値y0を間に含む利得y4,y5を与える周波
数x4,x5を求める。これにより、周波数の測定範囲の
1/n(図3ではn=10)の分解能で、所定の利得を
与える周波数を求めることができる。
As a conventional method, as shown in FIG.
First, the frequency measurement range is equally divided into n (in FIG. 3, n =
Then, the gain for each frequency is measured, and the frequencies x 4 and x 5 giving the gains y 4 and y 5 including the predetermined value y 0 are obtained. As a result, the frequency that gives a predetermined gain can be obtained with a resolution of 1 / n (n = 10 in FIG. 3) of the frequency measurement range.

【0004】さらに、周波数x4,x5間をn分割し、上
述と同様のことを行うことにより、周波数の測定範囲の
1/n2の分解能で所定の利得を与える周波数を求める
ことができる。
Further, by dividing the frequency x 4 and the frequency x 5 into n and performing the same operation as described above, it is possible to obtain a frequency giving a predetermined gain with a resolution of 1 / n 2 of the frequency measurement range. .

【0005】このように、m回同様のことを繰り返す
と、周波数の測定範囲の1/nmの分解能となる。要求
される測定精度に応じてnおよびmの値を選択すればよ
い。通常は、n=10の場合、mの値は2〜3で十分で
ある。
In this way, when the same operation is repeated m times, the resolution becomes 1 / n m of the frequency measurement range. The values of n and m may be selected according to the required measurement accuracy. Usually, for n = 10, a value of m of 2-3 is sufficient.

【0006】[0006]

【発明が解決しようとする課題】しかし上記従来の方法
では、利得を所定の値y0に一致させる場合、それに必
要とする時間は、測定点数×1回の測定時間で表すこと
ができ、測定点数が20〜30となるため、測定が完了
するまでに時間がかかるという問題があった。
However, in the above-mentioned conventional method, when the gain is made to coincide with the predetermined value y 0 , the time required for the gain can be expressed by the number of measurement points × one measurement time. Since the score is 20 to 30, there is a problem that it takes time to complete the measurement.

【0007】本発明は上記従来の問題点を解決するもの
で、測定精度を保ちながら測定点数を減らし、測定時間
を短縮できる半導体デバイスの測定方法を提供すること
を目的とする。
The present invention solves the above-mentioned conventional problems, and an object of the present invention is to provide a semiconductor device measuring method which can reduce the number of measuring points and shorten the measuring time while maintaining the measuring accuracy.

【0008】[0008]

【課題を解決するための手段】本発明は上記目的を達成
するために半導体デバイスの出力信号における周波数特
性であるカットオフ周波数の測定において、出力信号の
周波数と利得の関係を折れ線近似することで、演算によ
り近似的にカットオフ周波数を求める。
In order to achieve the above object, the present invention provides a broken line approximation of the relationship between the output signal frequency and the gain in the measurement of the cutoff frequency which is the frequency characteristic of the output signal of the semiconductor device. , The cutoff frequency is approximately calculated by calculation.

【0009】[0009]

【作用】この発明の構成によれば、出力信号の周波数と
利得の関係を折れ線近似することによって、近似による
測定精度を上げ、かつ測定点数を大幅に減らすことがで
きるため測定時間の大幅な短縮が可能となる。
According to the structure of the present invention, the relationship between the frequency of the output signal and the gain is approximated by a polygonal line, so that the accuracy of the measurement by the approximation can be improved and the number of measurement points can be greatly reduced. Is possible.

【0010】[0010]

【実施例】以下、本発明の一実施例について図面を参照
しながら説明する。
An embodiment of the present invention will be described below with reference to the drawings.

【0011】図1は本発明における半導体デバイスの試
験回路図である。図1において、信号発生器1は半導体
デバイス2の入力端子4に接続され、半導体デバイス2
の入力信号を発生する。ACレベルメーター3は半導体
デバイス2の出力端子5に接続され、半導体デバイス2
の出力信号を測定する。
FIG. 1 is a test circuit diagram of a semiconductor device according to the present invention. In FIG. 1, a signal generator 1 is connected to an input terminal 4 of a semiconductor device 2, and a semiconductor device 2
Generate the input signal of. The AC level meter 3 is connected to the output terminal 5 of the semiconductor device 2 and
Measure the output signal of.

【0012】図2は、図1に示す回路において測定され
る周波数特性を表し、周波数と利得との関係を示す図で
ある。
FIG. 2 is a diagram showing the frequency characteristic measured in the circuit shown in FIG. 1 and showing the relationship between the frequency and the gain.

【0013】図2(a)に示すように、まず利得を所定
の値yADJに一致させるための測定周波数範囲の最小お
よび最大の2点の周波数xLおよびxHにおけるそれぞれ
の利得yLおよびyHを測定する。この測定値を用いて周
波数xと利得yとの関係を直線(一次関数)と仮定する
と利得xは、 y=yH+(x−xH)(yH−yL)/(xH−xL) ……(1) で表され、yADJ時の周波数の近似値x’ADJは x’ADJ=xH+(yADJ−yH)(xH−xL)/(yH−yL) ……(2) で表される。これにより、直線近似から利得を所定の値
ADJに一致させるための周波数の近似値x’ADJを演算
で求めることができる。しかし、図2(a)に示すよう
に、直線近似によって求められた周波数の近似値x’
ADJが、実際の周波数値であるxADJと大きく異なってい
た場合、この近似は精度に欠けることになる。
[0013] As shown in FIG. 2 (a), each of the gain y L and the first minimum and maximum two-point measurement frequency range to match the gain to a predetermined value y ADJ frequency x L and x H Measure y H. Assuming that the relationship between the frequency x and the gain y is a straight line (linear function) using this measured value, the gain x is y = y H + (x−x H ) (y H −y L ) / (x H − x L ) ... (1), and the approximate value x ′ ADJ of the frequency at y ADJ is x ′ ADJ = x H + (y ADJ −y H ) (x H −x L ) / (y H − y L ) ... Represented by (2). As a result, the approximate value x ′ ADJ of the frequency for matching the gain with the predetermined value y ADJ can be obtained by calculation from the linear approximation. However, as shown in FIG. 2A, the approximate value x ′ of the frequency obtained by the linear approximation
If ADJ is significantly different from the actual frequency value, x ADJ , this approximation will lack accuracy.

【0014】そこで図2(b)について説明する。図2
(b)は周波数xL,xH間に任意の周波数x1,x2をと
り、それぞれの周波数xL,x1,x2,xHの利得yL
1,y2,yHを測定する。次にyADJがどの利得の間に
存在しているか確認する。図2(b)の場合はyADJ
L,y1間に存在しているため、周波数xL,x1におい
て上述と同様に周波数xと利得yとの関係を直線と仮定
することで、yADJ時の周波数の近似値x’ADJを演算に
より求めることができる。
2 (b) will be described. Figure 2
(B) the frequency x L, x H takes an arbitrary frequency x 1, x 2 between the respective frequencies x L, x 1, x 2, x H gain y L,
Measure y 1 , y 2 , y H. Next, check which gain y ADJ exists between. In the case of FIG. 2B, since y ADJ exists between y L and y 1 , it is possible to assume that the relationship between the frequency x and the gain y at the frequencies x L and x 1 is a straight line. , Y ADJ , the approximate value x ′ ADJ of the frequency at the time of ADJ can be calculated.

【0015】つまり周波数特性を折れ線と仮定して近似
することにより、直線近似の場合に比べて、精度のよい
測定値が得られる。
That is, by approximating the frequency characteristic assuming that it is a broken line, it is possible to obtain a more accurate measured value than in the case of linear approximation.

【0016】図2(b)は周波数を3分割した場合につ
いて示しているが、さらに分割数を多くすれば、折れ線
近似の精度がよくなる。
Although FIG. 2B shows the case where the frequency is divided into three, if the number of divisions is further increased, the accuracy of the polygonal line approximation will be improved.

【0017】なお、実施例では周波数特性であるカット
オフ周波数の折れ線近似による測定方法について説明し
たが、周波数測定以外の非直線特性においても同様な折
れ線近似による測定を行える。
In the embodiment, the method of measuring the cutoff frequency, which is the frequency characteristic, by the polygonal line approximation has been described, but the similar polygonal line approximation can be used for the non-linear characteristic other than the frequency measurement.

【0018】[0018]

【発明の効果】この発明の半導体デバイスの測定方法
は、近似による測定精度を上げ、かつ測定点数を大幅に
減らすことができるため測定時間の大幅な短縮が可能と
なる。
According to the semiconductor device measuring method of the present invention, the accuracy of measurement by approximation can be improved and the number of measurement points can be greatly reduced, so that the measurement time can be greatly shortened.

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

【図1】本発明の一実施例における半導体デバイスの試
験回路図
FIG. 1 is a test circuit diagram of a semiconductor device according to an embodiment of the present invention.

【図2】(a),(b)は図1に示す回路において測定
される周波数特性を示す図
2A and 2B are diagrams showing frequency characteristics measured in the circuit shown in FIG.

【図3】従来例の測定方法を説明するための図FIG. 3 is a diagram for explaining a conventional measuring method.

【符号の説明】[Explanation of symbols]

1 信号発生器 2 半導体デバイス 3 ACレベルメーター 1 signal generator 2 semiconductor device 3 AC level meter

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 半導体デバイスの出力信号の周波数特性
を測定する方法において、上記出力信号の所定周波数の
間隔で利得を折れ線近似して、演算によりカットオフ周
波数を求めることを特徴とする半導体デバイスの測定方
法。
1. A method for measuring a frequency characteristic of an output signal of a semiconductor device, wherein the cutoff frequency is calculated by performing a linear approximation of a gain at intervals of a predetermined frequency of the output signal and calculating the cutoff frequency. Measuring method.
JP6184434A 1994-08-05 1994-08-05 Measuring method of semiconductor device Pending JPH0850161A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6184434A JPH0850161A (en) 1994-08-05 1994-08-05 Measuring method of semiconductor device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6184434A JPH0850161A (en) 1994-08-05 1994-08-05 Measuring method of semiconductor device

Publications (1)

Publication Number Publication Date
JPH0850161A true JPH0850161A (en) 1996-02-20

Family

ID=16153092

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6184434A Pending JPH0850161A (en) 1994-08-05 1994-08-05 Measuring method of semiconductor device

Country Status (1)

Country Link
JP (1) JPH0850161A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US8694145B2 (en) 2001-06-19 2014-04-08 Applied Materials, Inc. Feedback control of a chemical mechanical polishing device providing manipulation of removal rate profiles

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US8694145B2 (en) 2001-06-19 2014-04-08 Applied Materials, Inc. Feedback control of a chemical mechanical polishing device providing manipulation of removal rate profiles

Similar Documents

Publication Publication Date Title
JPH10145231A (en) Data correcting method for a/d conversion device and d/a conversion device
JPH0850161A (en) Measuring method of semiconductor device
JP3194653B2 (en) How to measure crystal oscillator constants
JP2672690B2 (en) Semiconductor device testing method
JP3205603B2 (en) Mass calibration method for magnetic field type mass spectrometer
JPH05322941A (en) Adjusting method for ac measuring apparatus
SU1453343A1 (en) Device for testing inductive voltage dividers
JPH08248072A (en) Method and apparatus for measuring impedance characteristics of crystal oscillator
JPH08136593A (en) Spectrum analyzer
JPS61149869A (en) Waveform analytic system
JPH10339751A (en) Analog-digital mixed simulation method and verification system
JPH08160100A (en) Semiconductor tester
JP2002267507A (en) Method for automatically adjusting internal calibration signal and device using the same
JPS618676A (en) Level meter
RU2036481C1 (en) Device for graduation of central board electromagnetic instruments
JPS6033410Y2 (en) High frequency impedance measurement device
SU1109667A1 (en) Meter of standing wave total resistance and coefficient
SU1200182A1 (en) Method of measuring electric and non-electric parameters
JPS6333667A (en) Method for measuring amplification noise and frequency band of amplifying ic
JPH05322942A (en) Adjusting method for ac measuring apparatus
JPH07111489A (en) Method for calculating loss of transmission line
US20020171570A1 (en) AD converter evaluation apparatus
JPS61235768A (en) Measuring instrument for characteristic of semiconductor element
JPS5981509A (en) Magnetic goniometer
JPH08145713A (en) Calculation method of characteristic central value of group