JPH0560615A - Light spectrum analyzer - Google Patents
Light spectrum analyzerInfo
- Publication number
- JPH0560615A JPH0560615A JP22576691A JP22576691A JPH0560615A JP H0560615 A JPH0560615 A JP H0560615A JP 22576691 A JP22576691 A JP 22576691A JP 22576691 A JP22576691 A JP 22576691A JP H0560615 A JPH0560615 A JP H0560615A
- Authority
- JP
- Japan
- Prior art keywords
- spectrum
- converted
- digital signal
- range
- power
- 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
Links
Landscapes
- Spectrometry And Color Measurement (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】この発明は干渉計の出力をデジタ
ル信号に変換し、そのデジタル信号をフーリエ変換して
入力光の解析を行う光スペクトラムアナライザに関す
る。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an optical spectrum analyzer for converting an output of an interferometer into a digital signal and Fourier-transforming the digital signal to analyze input light.
【0002】[0002]
【従来の技術】光スペクトラムアナライザにおいては入
力光をマイケルソン干渉計に入射し、その干渉光を電気
信号に変換し、その電気信号を必要に応じて増幅器で増
幅し、その増幅出力をAD変換器でデジタル信号に変換
し、そのデジタル信号を高速フーリエ変換して周波数領
域の信号とし、つまりスペクトラムを求め、これらによ
り入力光に対する各種の解析が行われる。2. Description of the Related Art In an optical spectrum analyzer, input light is incident on a Michelson interferometer, the interference light is converted into an electric signal, the electric signal is amplified by an amplifier as necessary, and the amplified output is AD-converted. A digital signal is converted into a digital signal by a detector, and the digital signal is subjected to fast Fourier transform to obtain a signal in the frequency domain, that is, a spectrum is obtained, and various analyzes are performed on the input light.
【0003】[0003]
【発明が解決しようとする課題】入力光に対する最適な
感度を設定するため、つまり最適レンジを決めるため、
入力光をスペクトル解析し、表示し、その表示を見て適
当にレンジを変更し、つまり増幅器の増幅利得やAD変
換器の変換利得を変更し、再び入力光のスペクトル解析
を行い、同様のことを繰返して最適レンジに設定してい
た。このような操作を行うため、最適レンジを得るため
多い場合は、5回も測定を行わなければならなかった。
マイケルソン干渉計はミラーを機械的に移動させて所定
範囲の干渉光を得るため、高速に行うことが困難であ
り、1回の測定に比較的長い時間が掛る。このため最適
レンジ設定のために何回も測定を行うことは全体として
の測定時間が長くなり好ましくなかった。In order to set the optimum sensitivity to the input light, that is, to determine the optimum range,
The spectrum of the input light is analyzed and displayed, the range is changed appropriately by looking at the display, that is, the amplification gain of the amplifier or the conversion gain of the AD converter is changed, and the spectrum analysis of the input light is performed again. Was repeated to set the optimum range. Since such an operation is performed, in order to obtain the optimum range, it is often necessary to perform the measurement five times.
Since the Michelson interferometer mechanically moves a mirror to obtain interference light within a predetermined range, it is difficult to perform at high speed, and one measurement takes a relatively long time. For this reason, it is not preferable to perform the measurement many times for setting the optimum range because the measurement time as a whole becomes long.
【0004】[0004]
【課題を解決するための手段】この発明によればフーリ
エ変換されて得られたスペクトラムがパワースペクトラ
ムに変換され、そのパワースペクトラムが全周波数帯域
にわたって積分され、その積分値に応じてレンジ設定が
行われる。According to the present invention, the spectrum obtained by Fourier transform is converted into a power spectrum, the power spectrum is integrated over the entire frequency band, and the range is set according to the integrated value. Be seen.
【0005】[0005]
【実施例】図1にこの発明の実施例を示す。入力光はマ
イケルソン干渉計11に入射され、その干渉光が電気信
号に変換されて出力され、その電気信号は増幅器12で
増幅され、その増幅出力はAD変換器13でデジタル信
号に変換され、そのデジタル信号はデジタルフィルタ1
4を通じ、又はこれを通じることなく高速フーリエ変換
器15へ供給されて高速フーリエ変換され、その変換に
より得られたスペクトラムは表示器16に表示される。FIG. 1 shows an embodiment of the present invention. The input light is incident on the Michelson interferometer 11, the interference light is converted into an electric signal and output, the electric signal is amplified by the amplifier 12, and the amplified output is converted into a digital signal by the AD converter 13. The digital signal is digital filter 1
4 or not, and is supplied to the fast Fourier transformer 15 for fast Fourier transform, and the spectrum obtained by the transform is displayed on the display 16.
【0006】この発明においては高速フーリエ変換器1
5より得られたスペクトラムはパワー演算部17でパワ
ースペクトラムに変換され、そのパワースペクトラムは
積分部18で全周波数帯域にわたって積分される。その
積分値に応じて増幅器12の増幅利得及び/又はAD変
換器13の変換利得が設定され、最適なレンジが自動的
に設定される。In the present invention, the fast Fourier transformer 1
The spectrum obtained from 5 is converted into a power spectrum by the power calculator 17, and the power spectrum is integrated by the integrator 18 over the entire frequency band. The amplification gain of the amplifier 12 and / or the conversion gain of the AD converter 13 is set according to the integrated value, and the optimum range is automatically set.
【0007】つまり測定に当り、まず、適当にレンジ設
定を行い、即ち入力光がどの積分のパワーであるかを推
定し、そのパワーを基準パワーレベルとしてレンジ設定
を行う。そのレンジ設定後、入力光を測定し、前述のよ
うにパワースペクトラムの積分値を求め、この積分値と
前記設定レンジの基準パワーレベルとの差を求め、その
差に応じてレンジ設定を変更する。例えば積分値の方が
大き過ぎた場合はその大き過ぎに積分に応じてレンジを
下げ、当初から基準パワーレベルとして、前記積分値を
設定したように制御する。That is, in the measurement, first, the range is set appropriately, that is, the integral power of the input light is estimated, and the range is set with the power as a reference power level. After setting the range, the input light is measured, the integral value of the power spectrum is obtained as described above, the difference between the integral value and the reference power level of the setting range is obtained, and the range setting is changed according to the difference. .. For example, when the integral value is too large, the range is lowered according to the integral when the integral value is too large, and control is performed as if the integral value was set as the reference power level from the beginning.
【0008】なお最初に設定した基準パワーレベル(設
定レンジ)が入力光のパワーと極端に異なる場合は、一
回の測定でも最適レンジに設定できない場合があり、こ
の場合は表示器16の表示スペクトラムがなまったりす
るため、最適レンジでないことがわかり、再レンジ設定
(再測定)を行えばよい。しかし通常は被測定光のパワ
ーがどの程度のものか、おおよその値がわかっているこ
とが多く、そのおおよその値を測定開始時に、基準パワ
ーレベルとしてレンジ設定を行えば1回の測定で最適レ
ンジに自動的に設定される。If the reference power level (setting range) initially set is extremely different from the power of the input light, it may not be possible to set the optimum range even with one measurement. In this case, the display spectrum of the display 16 is displayed. Since it is blunt, it can be understood that the range is not the optimum range, and rerange setting (remeasurement) may be performed. However, in general, it is often known how much the power of the measured light is, and if the range is set as the reference power level at the start of measurement, it is optimal for one measurement. The range is automatically set.
【0009】[0009]
【発明の効果】以上述べたようにこの発明によれば、1
回の測定で得られたスペクトラムからパワースペクトラ
ムを得、これを積分し、その積分値でレンジ設定が行わ
れ、1回の測定で最適レンジ設定が得られ、それだけ全
体の測定時間が短かくなり、かつ測定操作も簡単とな
る。As described above, according to the present invention, 1
The power spectrum is obtained from the spectrum obtained by one measurement, this is integrated, the range is set by the integrated value, the optimum range setting is obtained by one measurement, and the total measurement time becomes shorter. Also, the measurement operation becomes simple.
【図1】この発明の実施例を示すブロック図。FIG. 1 is a block diagram showing an embodiment of the present invention.
Claims (1)
そのデジタル信号をフーリエ変換する光スペクトラムア
ナライザにおいて、 上記フーリエ変換して得られたスペクトラムをパワース
ペクトラムに変換する手段と、 その変換されたパワースペクトラムを全周波数帯域にわ
たって積分する手段と、 そのパワースペクトラムの積分値に応じて測定レンジを
設定する手段と、 を設けたことを特徴とする光スペクトラムアナライザ。1. The output of the interferometer is converted into a digital signal,
In the optical spectrum analyzer for Fourier transforming the digital signal, a means for converting the spectrum obtained by the Fourier transform into a power spectrum, a means for integrating the converted power spectrum over the entire frequency band, and a means for integrating the power spectrum An optical spectrum analyzer comprising means for setting a measurement range according to an integrated value and.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3225766A JP3055716B2 (en) | 1991-09-05 | 1991-09-05 | Optical spectrum analyzer |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3225766A JP3055716B2 (en) | 1991-09-05 | 1991-09-05 | Optical spectrum analyzer |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH0560615A true JPH0560615A (en) | 1993-03-12 |
JP3055716B2 JP3055716B2 (en) | 2000-06-26 |
Family
ID=16834473
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP3225766A Expired - Fee Related JP3055716B2 (en) | 1991-09-05 | 1991-09-05 | Optical spectrum analyzer |
Country Status (1)
Country | Link |
---|---|
JP (1) | JP3055716B2 (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0755020A2 (en) | 1995-07-19 | 1997-01-22 | Canon Kabushiki Kaisha | Vibration-transmitting tablet and coordinate-input apparatus using said tablet |
US5744760A (en) * | 1995-09-07 | 1998-04-28 | Canon Kabushiki Kaisha | Coordinates input apparatus |
-
1991
- 1991-09-05 JP JP3225766A patent/JP3055716B2/en not_active Expired - Fee Related
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0755020A2 (en) | 1995-07-19 | 1997-01-22 | Canon Kabushiki Kaisha | Vibration-transmitting tablet and coordinate-input apparatus using said tablet |
US5936207A (en) * | 1995-07-19 | 1999-08-10 | Canon Kabushiki Kaisha | Vibration-transmitting tablet and coordinate-input apparatus using said tablet |
US5744760A (en) * | 1995-09-07 | 1998-04-28 | Canon Kabushiki Kaisha | Coordinates input apparatus |
Also Published As
Publication number | Publication date |
---|---|
JP3055716B2 (en) | 2000-06-26 |
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Legal Events
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Free format text: JAPANESE INTERMEDIATE CODE: A01 Effective date: 20000307 |
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