JPH088392B2 - Variable wavelength light source - Google Patents

Variable wavelength light source

Info

Publication number
JPH088392B2
JPH088392B2 JP26102387A JP26102387A JPH088392B2 JP H088392 B2 JPH088392 B2 JP H088392B2 JP 26102387 A JP26102387 A JP 26102387A JP 26102387 A JP26102387 A JP 26102387A JP H088392 B2 JPH088392 B2 JP H088392B2
Authority
JP
Japan
Prior art keywords
light source
output
frequency
wavelength
light
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.)
Expired - Lifetime
Application number
JP26102387A
Other languages
Japanese (ja)
Other versions
JPH01102978A (en
Inventor
明 大手
浩二 秋山
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.)
Yokogawa Electric Corp
Original Assignee
Yokogawa Electric 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 Yokogawa Electric Corp filed Critical Yokogawa Electric Corp
Priority to JP26102387A priority Critical patent/JPH088392B2/en
Publication of JPH01102978A publication Critical patent/JPH01102978A/en
Publication of JPH088392B2 publication Critical patent/JPH088392B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S5/00Semiconductor lasers
    • H01S5/06Arrangements for controlling the laser output parameters, e.g. by operating on the active medium
    • H01S5/062Arrangements for controlling the laser output parameters, e.g. by operating on the active medium by varying the potential of the electrodes
    • H01S5/06209Arrangements for controlling the laser output parameters, e.g. by operating on the active medium by varying the potential of the electrodes in single-section lasers
    • H01S5/0622Controlling the frequency of the radiation

Description

【発明の詳細な説明】 《産業上の利用分野》 本発明は、光スペクトル・アナライザ等に用いられて
精密な波長測定を可能にする可変波長光源の改良に関す
る。
TECHNICAL FIELD The present invention relates to an improvement of a variable wavelength light source which is used in an optical spectrum analyzer or the like and enables precise wavelength measurement.

《従来の技術》 従来、光スペクトル・アナライザや分光器などを用い
て波長特性や分光特性を測定する場合、精度を上げるに
は波長の基準となる光源が必要であった。
<< Prior Art >> Conventionally, when measuring a wavelength characteristic or a spectral characteristic using an optical spectrum analyzer, a spectroscope, or the like, a light source serving as a wavelength reference is required to improve accuracy.

《発明が解決しようとする問題点》 しかしながら、基準波長光源の波長から離れた帯域を
測定する場合に誤差が大きくなるという欠点があった。
<< Problems to be Solved by the Invention >> However, there is a drawback that an error becomes large when a band away from the wavelength of the reference wavelength light source is measured.

また、基準波長光源として可変波長光源を使用すれ
ば、波長範囲は広くとれるが、可変波長光源の入力と発
振波長を精度よく対応づけをするのは容易でない。
Also, if a variable wavelength light source is used as the reference wavelength light source, the wavelength range can be widened, but it is not easy to accurately associate the input of the variable wavelength light source with the oscillation wavelength.

本発明はこのような問題点を解決するためになされた
もので、広い帯域にわたって高精度な波長測定を可能と
する可変波長光源を実現することを目的とする。
The present invention has been made to solve such a problem, and an object thereof is to realize a variable wavelength light source that enables highly accurate wavelength measurement over a wide band.

《問題点を解決するための手段》 本発明は入力信号に対応して出力光の波長が変化する
可変波長光源に係るもので、その特徴とするところは基
準波長光源と、この基準波長光源の出力光を位相変調し
てサブキャリア光を発生させる位相変調器と、レーザ光
源と、このレーザ光源の出力光の一部と前記位相変調器
の出力光とを合波する光学手段と、この光学手段からの
合波された光を受光してそのビート周波数の電気信号を
発生する受光素子と、この受光素子からのビート周波数
が一定となるように前記レーザ光源の出力周波数を制御
する制御手段とを備え、位相変調器の変調周波数に対応
してレーザ光源の出力波長を可変とした点にある。
<< Means for Solving the Problems >> The present invention relates to a variable wavelength light source in which the wavelength of output light changes in response to an input signal, and is characterized by a reference wavelength light source and a reference wavelength light source. A phase modulator that phase-modulates output light to generate subcarrier light, a laser light source, an optical unit that combines a part of the output light of the laser light source and the output light of the phase modulator, and the optical device. A light-receiving element that receives the combined light from the means and generates an electric signal of the beat frequency, and a control means that controls the output frequency of the laser light source so that the beat frequency from the light-receiving element becomes constant. In addition, the output wavelength of the laser light source is variable according to the modulation frequency of the phase modulator.

《作用》 位相変調器が発生するサブキャリア光の一つにレーザ
光源の波長を制御し、位相変調器の変調周波数を変化さ
せれば、サブキャリア光の波長が変化するので、レーザ
光源の波長も変化する。
<< Function >> If the wavelength of the laser light source is controlled to one of the sub-carrier lights generated by the phase modulator and the modulation frequency of the phase modulator is changed, the wavelength of the sub-carrier light changes. Also changes.

《実施例》 以下本発明を図面を用いて詳しく説明する。<Example> The present invention will be described in detail below with reference to the drawings.

第1図は本発明に係る可変波長光源の一実施例を示す
構成ブロック図である。図において、光路を帯状の信号
線で表し、電気信号と区別している。1は例えばCsやRb
等の原子吸収線に半導体レーザの波長を制御したもの等
を用いた波長の非常に安定な基準波長光源、2はこの基
準波長光源1の出力光を入射して位相変調する位相変調
器、3は入力周波数信号が印加される入力端子、4はこ
の入力端子3からの入力電気信号を増幅しその出力で前
記位相変調器2を周波数変調する増幅器、5は前記位相
変調器2の出力光を入射するビームスプリッタ、6はこ
のビームスプリッタ5の出力光を入射する受光素子、7
はこの受光素子6の電気出力を入力する制御回路、8は
レーザ光源を構成しこの制御回路7の出力を入力する半
導体レーザ、9はこの半導体レーザ8の出力光を入射す
るビームスプリッタ、10,11はこのビームスプリッタ9
の反射光を反射して前記ビームスプリッタ5に入射させ
るミラーである。ビームスプリッタ5,9およびミラー10,
11はレーザ光源8の出力光の一部と位相変調器2の出力
光とを合波する光学手段を構成する。位相変調器2はバ
ルク型,導波路型等種々のものを用いることができる
が、低パワーで多数のサブキャリアが発生するという点
で導波路型が優れている。半導体レーザ8としてはでき
るだけスペクトル幅が狭くて、モードホッピングの少な
い半導体レーザ、例えばDFBレーザ等を用いる。
FIG. 1 is a configuration block diagram showing an embodiment of a variable wavelength light source according to the present invention. In the figure, the optical path is represented by a band-shaped signal line to distinguish it from an electric signal. 1 is, for example, C s or R b
A reference wavelength light source having a very stable wavelength using a semiconductor laser whose wavelength is controlled by an atomic absorption line, etc., 2 is a phase modulator for phase-modulating the output light of the reference wavelength light source 1 by phase modulation, 3 Is an input terminal to which an input frequency signal is applied, 4 is an amplifier that amplifies the input electric signal from this input terminal 3 and frequency-modulates the phase modulator 2 with its output, and 5 is the output light of the phase modulator 2. An incident beam splitter, 6 is a light receiving element for injecting the output light of the beam splitter 5, 7
Is a control circuit for inputting the electric output of the light receiving element 6, 8 is a semiconductor laser which constitutes a laser light source and receives the output of the control circuit 7, 9 is a beam splitter which makes the output light of the semiconductor laser 8 incident, 11 is this beam splitter 9
It is a mirror that reflects the reflected light of and makes it enter the beam splitter 5. Beam splitter 5,9 and mirror 10,
Reference numeral 11 constitutes an optical means for multiplexing a part of the output light of the laser light source 8 and the output light of the phase modulator 2. Various types such as a bulk type and a waveguide type can be used as the phase modulator 2, but the waveguide type is superior in that a large number of subcarriers are generated with low power. As the semiconductor laser 8, a semiconductor laser having a spectrum width as narrow as possible and less mode hopping, such as a DFB laser, is used.

第2図は基準波長光源1の具体的構成例を示す構成ブ
ロック図である。図において、11は半導体レーザ、12は
この半導体レーザ11の出力光が入射するビームスプリッ
タ、13はこのビームスプリッタ12の反射光を入射する標
準物質が封入された吸収セル、14はこの吸収セル13の出
力光が入射する受光素子、15はこの受光素子14の電気出
力を入力しこれに対応する出力で前記半導体レーザ11の
電流を制御するロックインアンプ、16は前記半導体レー
ザ11の電流を周波数変調するとともに前記ロックインア
ンプ15の位相検波周波数を供給する発振器である。ビー
ムスプリッタ12の透過光がこの基準波長光源の出力光と
なる。標準物質としてはCs,Rb,NH3,H2Oなど任意の物
質を用いることができる。半導体レーザ11の出力光はビ
ームスプリッタ12で反射されて吸収セル13に入射し、吸
収セル内13の標準物質による吸収を受ける。吸収量受光
素子14で検出し、ロックインアンプ15を介して半導体レ
ーザ11の電流に帰還する。半導体レーザ11の出力波長は
標準物質の吸収スプクトル線にロックされるので、高安
定,高精度の基準波長光源を実現できる。
FIG. 2 is a configuration block diagram showing a specific configuration example of the reference wavelength light source 1. In the figure, 11 is a semiconductor laser, 12 is a beam splitter on which the output light of this semiconductor laser 11 is incident, 13 is an absorption cell in which a standard substance on which the reflected light of this beam splitter 12 is incident is enclosed, and 14 is this absorption cell 13 , A lock-in amplifier for controlling the current of the semiconductor laser 11 with an input corresponding to the electric output of the light-receiving element 14, and 16 for controlling the current of the semiconductor laser 11 by frequency. An oscillator that modulates and supplies the phase detection frequency of the lock-in amplifier 15. The transmitted light of the beam splitter 12 becomes the output light of this reference wavelength light source. As the standard substance, any substance such as C s , R b , NH 3 , and H 2 O can be used. The output light of the semiconductor laser 11 is reflected by the beam splitter 12, enters the absorption cell 13, and is absorbed by the standard substance in the absorption cell 13. The absorption amount is detected by the light receiving element 14, and is fed back to the current of the semiconductor laser 11 via the lock-in amplifier 15. Since the output wavelength of the semiconductor laser 11 is locked to the absorption spectrum line of the standard substance, a highly stable and highly accurate reference wavelength light source can be realized.

第3図は制御回路7の具体例を示す構成ブロック図で
ある。71は受光素子6からの電気出力を入力する比較
器、72は設定用の周波数を発生する発振器、73は前記比
較器71の出力と前記発振器72の出力とを入力する位相比
較器、74はこの位相比較器73の出力を入力するサーボア
ンプである。受光素子6の出力周波数は発振器72の発振
周波数と位相比較器で比較され、その周波数の差を無く
すようにサーポアンプ74が半導体レーザ8の出力周波数
を制御する。
FIG. 3 is a configuration block diagram showing a specific example of the control circuit 7. Reference numeral 71 is a comparator for inputting an electric output from the light receiving element 6, 72 is an oscillator for generating a setting frequency, 73 is a phase comparator for inputting the output of the comparator 71 and the output of the oscillator 72, and 74 is a phase comparator. The servo amplifier receives the output of the phase comparator 73. The output frequency of the light receiving element 6 is compared with the oscillation frequency of the oscillator 72 by the phase comparator, and the servo amplifier 74 controls the output frequency of the semiconductor laser 8 so as to eliminate the difference between the frequencies.

上記のような構成の可変波長光源の動作を次に説明す
る。基準波長光源1から出力された周波数fRの光は位相
変調器2においてその変調周波数fmで位相変調され、第
4図に示すような多数のサブキャリア(副搬送波)を発
生する。半導体レーザ8の出力光の一部はビームスプリ
ッタ9で反射され、ミラー10,11を介してビームスプリ
ッタ5において位相変調器2の出力光と合波され、受光
素子6でそのビート周波数の電気信号を発生する。制御
回路7は前述のように、この受光素子6からの信号周波
数が一定となるように半導体レーザ8を制御する。この
結果半導体レーザ8からビームスプリッタ9を通過して
出力される光の周波数は位相変調器2の特定の波長の出
力光と一定の周波数差をもったものとなる。位相変調器
2からの出力光に含まれるN番目のサブキャリアに半導
体レーザ8の周波数foをロックすると、 fo=fR+N・fm …(1) となるので、入力周波数fmに応じて出力周波数foを可変
できる。
The operation of the variable wavelength light source configured as described above will be described below. The light having the frequency f R output from the reference wavelength light source 1 is phase-modulated at the modulation frequency f m in the phase modulator 2 to generate a large number of subcarriers (subcarriers) as shown in FIG. A part of the output light of the semiconductor laser 8 is reflected by the beam splitter 9, is combined with the output light of the phase modulator 2 in the beam splitter 5 via the mirrors 10 and 11, and is received by the light receiving element 6 as an electric signal of the beat frequency. To occur. As described above, the control circuit 7 controls the semiconductor laser 8 so that the signal frequency from the light receiving element 6 becomes constant. As a result, the frequency of the light output from the semiconductor laser 8 after passing through the beam splitter 9 has a certain frequency difference from the output light of the specific wavelength of the phase modulator 2. When the frequency f o of the semiconductor laser 8 is locked to the Nth subcarrier contained in the output light from the phase modulator 2, f o = f R + Nf m (1) Therefore, the input frequency f m The output frequency f o can be changed accordingly.

このような構成の可変波長光源によれば、基準波長光
源の安定度と位相変調器の入力周波数の安定度とで出力
周波数の安定度が決まるので、安定度が優れている。
According to the variable wavelength light source having such a configuration, the stability of the output frequency is determined by the stability of the reference wavelength light source and the stability of the input frequency of the phase modulator, and thus the stability is excellent.

また基準波長光源の周波数に位相変調器の入力周波数
の整数倍を加算したもの(と一定の周波数差にあるも
の)が出力周波数となるので、出力周波数が高精度であ
る。
Further, since the output frequency is obtained by adding the integer multiple of the input frequency of the phase modulator to the frequency of the reference wavelength light source (the one having a constant frequency difference), the output frequency is highly accurate.

なお上記の実施例において、増幅器4の代りにVCO(V
oltage Controlled Oscillator:電圧制御発振器)また
はシンセサイザを使用することにより、入力信号として
周波数でなく、電圧を用いることもできる。この場合に
は位相変調器2の入力周波数fmが入力電圧Vinによりfm
=G・Vinと変るとすると、 fo=fR+N・G・Vin …(2) となり、入力電圧に応じて出力周波数を可変にできる。
In the above embodiment, instead of the amplifier 4, VCO (V
It is also possible to use voltage as an input signal instead of frequency by using an oltage controlled oscillator (oscillator) or a synthesizer. F m input frequency f m of the phase modulator 2 in this case is the input voltage V in
= G · V in , then f o = f R + N · G · V in (2), and the output frequency can be changed according to the input voltage.

第5図は本発明の変形例を示す構成ブロック図であ
る。制御手段としてロックインアンプ75を使用し、第2
の発振器21により周波数fpの別の周波数変調を位相変調
器2に加えるとともに、ロックインアンプ75の位相検波
周波数として用いれば、オフセット周波数なしに半導体
レーザ8の出力周波数をサブキャリアの中心周波数に制
御できる。なおこの場合の周波数変調は基準波長光源1
において行うこともできる。
FIG. 5 is a configuration block diagram showing a modified example of the present invention. The lock-in amplifier 75 is used as the control means, and the second
If another frequency modulation of the frequency f p is applied to the phase modulator 2 by the oscillator 21 of, and is used as the phase detection frequency of the lock-in amplifier 75, the output frequency of the semiconductor laser 8 becomes the center frequency of the subcarrier without the offset frequency. You can control. In this case, the frequency modulation is performed by the reference wavelength light source 1.
Can also be done in.

なお上記の各実施例において、光学手段としてビーム
スプリッタやミラーの代りに光ファイバカプラや光ファ
イバを用いて小形化することもできる。
In each of the above embodiments, an optical fiber coupler or an optical fiber may be used as the optical means instead of the beam splitter or the mirror to reduce the size.

また基準波長光源1の1実施例として示した第2図の
方式は線形吸収法とよばれ、ドップラシフトにより吸収
スペクトルが比較的太くなるが、飽和吸収法(堀,門
田,北野,藪崎,小川:飽和吸収分光を用いた半導体レ
ーザの周波数安定化,信学技報 OQE82−116)によりド
ップラシフトで隠れている超微細構造の吸収線を検出し
て、これに半導体レーザ11の発振波長をロックすればさ
らに高安定とすることができる。
The method of FIG. 2 shown as one embodiment of the reference wavelength light source 1 is called a linear absorption method, and the absorption spectrum becomes relatively thick due to Doppler shift, but the saturated absorption method (Hori, Kadota, Kitano, Yabusaki, Ogawa) : Frequency stabilization of a semiconductor laser using saturated absorption spectroscopy, and the absorption line of the hyperfine structure hidden by Doppler shift is detected by the technical report of OQE82-116), and the oscillation wavelength of the semiconductor laser 11 is locked to this. If this is done, it can be made even more stable.

《発明の効果》 以上述べたように本発明によれば、広い帯域にわたっ
て高精度な波長測定を可能とする可変波長光源を簡単な
構成で実現することができる。
<< Advantages of the Invention >> As described above, according to the present invention, it is possible to realize a variable wavelength light source that enables highly accurate wavelength measurement over a wide band with a simple configuration.

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

第1図は本発明に係る可変波長光源の1実施例を示す構
成ブロック図、第2図は第1図装置の基準波長光源1の
詳細を示す構成ブロック図、第3図は第1図装置の制御
回路7の詳細を示す構成ブロック図、第4図は位相変調
器2出力の周波数スペクトルを示す図、第5図は第1図
装置の変形例を示す構成ブロック図である。 1……基準波長光源、2……位相変調器、5,9,10,11…
…光学手段、6……受光素子、7,75……制御手段、8…
…レーザ光源、fm……変調周波数。
FIG. 1 is a structural block diagram showing an embodiment of a variable wavelength light source according to the present invention, FIG. 2 is a structural block diagram showing the details of a reference wavelength light source 1 of the apparatus of FIG. 1, and FIG. 3 is an apparatus of FIG. 4 is a block diagram showing the details of the control circuit 7, FIG. 4 is a diagram showing a frequency spectrum of the output of the phase modulator 2, and FIG. 5 is a block diagram showing a modified example of the apparatus shown in FIG. 1 ... Reference wavelength light source, 2 ... Phase modulator, 5, 9, 10, 11 ...
... Optical means, 6 ... Light receiving element, 7,75 ... Control means, 8 ...
… Laser light source, f m … Modulation frequency.

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】入力信号に対応して出力光の波長が変化す
る可変波長光源において、基準波長光源と、この基準波
長光源の出力光を位相変調してサブキャリア光を発生さ
せる位相変調器と、レーザ光源と、このレーザ光源の出
力光の一部と前記位相変調器の出力光とを合波する光学
手段と、この光学手段からの合波された光を受光してそ
のビート周波数の電気信号を発生する受光素子と、この
受光素子からのビート周波数が一定となるように前記レ
ーザ光源の出力周波数を制御する制御手段とを備え、位
相変調器の変調周波数に対応してレーザ光源の出力波長
を可変としたことを特徴とする可変波長光源。
1. A variable wavelength light source in which the wavelength of output light changes in response to an input signal, and a reference wavelength light source, and a phase modulator for phase modulating the output light of the reference wavelength light source to generate subcarrier light. A laser light source, an optical means for combining a part of the output light of the laser light source and the output light of the phase modulator, and the combined light from the optical means for receiving the electric power of the beat frequency. A light receiving element for generating a signal and a control means for controlling the output frequency of the laser light source so that the beat frequency from the light receiving element is constant, and the output of the laser light source corresponding to the modulation frequency of the phase modulator Variable wavelength light source characterized in that the wavelength is variable.
【請求項2】基準波長光源としてCsまたはRbの原子吸収
線に波長を制御した半導体レーザを用いた特許請求の範
囲第1項記載の可変波長光源。
2. The variable wavelength light source according to claim 1, wherein a semiconductor laser whose wavelength is controlled by an atomic absorption line of C s or R b is used as the reference wavelength light source.
【請求項3】レーザ光源として半導体レーザを用い、そ
の電流または温度を操作して出力周波数を制御すること
を特徴とする特許請求の範囲第1項記載の可変波長光
源。
3. The variable wavelength light source according to claim 1, wherein a semiconductor laser is used as the laser light source, and the output frequency is controlled by operating the current or temperature thereof.
JP26102387A 1987-10-16 1987-10-16 Variable wavelength light source Expired - Lifetime JPH088392B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP26102387A JPH088392B2 (en) 1987-10-16 1987-10-16 Variable wavelength light source

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP26102387A JPH088392B2 (en) 1987-10-16 1987-10-16 Variable wavelength light source

Publications (2)

Publication Number Publication Date
JPH01102978A JPH01102978A (en) 1989-04-20
JPH088392B2 true JPH088392B2 (en) 1996-01-29

Family

ID=17355972

Family Applications (1)

Application Number Title Priority Date Filing Date
JP26102387A Expired - Lifetime JPH088392B2 (en) 1987-10-16 1987-10-16 Variable wavelength light source

Country Status (1)

Country Link
JP (1) JPH088392B2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0334484A (en) * 1989-06-30 1991-02-14 Hamamatsu Photonics Kk Stabilized light source
JP2830189B2 (en) * 1989-10-20 1998-12-02 横河電機株式会社 Variable frequency light source

Also Published As

Publication number Publication date
JPH01102978A (en) 1989-04-20

Similar Documents

Publication Publication Date Title
US4856899A (en) Optical frequency analyzer using a local oscillator heterodyne detection of incident light
EP0401799B1 (en) Length measuring apparatus
US6891149B1 (en) Optical phase detector
US5493395A (en) Wavelength variation measuring apparatus
EP0908710B1 (en) Apparatus and method for measuring characteristics of light
JPH088392B2 (en) Variable wavelength light source
JP2830189B2 (en) Variable frequency light source
JP4612938B2 (en) Frequency variable light source
JP3018615B2 (en) Frequency stabilized laser light source
JP2997557B2 (en) Frequency stabilized light source with narrow linewidth oscillation frequency spectrum
JP3005065B2 (en) Reference frequency light source and ultra-high precision optical frequency measurement system using the same
JP2561210B2 (en) Isotope analyzer
JP3351253B2 (en) Optical frequency comb generator
JP2578271Y2 (en) Frequency stabilized laser light source
JP2612919B2 (en) Laser oscillation frequency stabilizer
JPH01102979A (en) Variable wavelength light source
JPH0918074A (en) Light frequency reference light source
JP3223521B2 (en) Optical frequency standard and optical frequency standard calibration device
JP3694379B2 (en) Tunable laser device
JPH0549055B2 (en)
JPH0216784A (en) Photofrequency standard device
JPH0652166B2 (en) Absolute length measuring machine
JP2876498B2 (en) High-precision near-infrared reference light frequency generation method
CN116499969A (en) Device for realizing synchronous stabilization of frequency and power in laser frequency sweeping process
JPH0462477B2 (en)