JPS6035588A - Frequency stabilized laser device - Google Patents

Frequency stabilized laser device

Info

Publication number
JPS6035588A
JPS6035588A JP14468983A JP14468983A JPS6035588A JP S6035588 A JPS6035588 A JP S6035588A JP 14468983 A JP14468983 A JP 14468983A JP 14468983 A JP14468983 A JP 14468983A JP S6035588 A JPS6035588 A JP S6035588A
Authority
JP
Japan
Prior art keywords
frequency
difference
voltage
positive
negative
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
JP14468983A
Other languages
Japanese (ja)
Inventor
Norito Suzuki
範人 鈴木
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.)
Individual
Original Assignee
Individual
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 Individual filed Critical Individual
Priority to JP14468983A priority Critical patent/JPS6035588A/en
Publication of JPS6035588A publication Critical patent/JPS6035588A/en
Pending 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
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/10Controlling the intensity, frequency, phase, polarisation or direction of the emitted radiation, e.g. switching, gating, modulating or demodulating
    • H01S3/13Stabilisation of laser output parameters, e.g. frequency or amplitude
    • H01S3/139Stabilisation of laser output parameters, e.g. frequency or amplitude by controlling the mutual position or the reflecting properties of the reflectors of the cavity, e.g. by controlling the cavity length

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Engineering & Computer Science (AREA)
  • Plasma & Fusion (AREA)
  • Optics & Photonics (AREA)
  • Lasers (AREA)

Abstract

PURPOSE:To exactly keep constant the resonator length of a laser resonator by a method wherein the positive and negative natures of the difference between a reference frequency and a photo beat frequency are discriminated, and then the electric signal increasing and decreasing according to the positive and negative natures of the frequency difference is added to the signal impressed on a blower driving motor. CONSTITUTION:The photo beat is detected by a detector 3 by passing the oscillated light of a laser oscillation tube 1 in a weak magnetic field through a polarizer 2 and then amplified by a wide band amplifying circuit 4, and the frequency is converted into a voltage by a frequency- voltage converter 5, resulting in obtaining the difference of a meta-reference frequency setter 8 between the meta-reference voltage by a differential amplifying circuit 9. On the other hand, the photo beat frequency is compared, in a comparator 6, with the frequency of a reference frequency generator (reference frequency setting section) 7, the converted into the electric signal slowly increasing and decreasing according to the frequency difference in a circuit 10 having the function of integration, after generating positive and negative voltages according to the negative and positive natures of the difference, and accordingly added to the signal passing through said section 8 by an adder 11. This signal which is slowly increasing and decreasing corrects the bias voltage. The corrected signal is applied to the motor M of the blower.

Description

【発明の詳細な説明】[Detailed description of the invention]

本発明はレーサーの発振周波数の安定化装置に関するも
のである。 地球磁界その他の磁界中にある、内部」(振鏡をr」す
るレー→」−光を偏光子を通してa fltllすると
光ヒ−1・が観+1111され、光ヒートの周波数が一
定となるごと<J(&鏡の間隔を制御すると、発振局l
反数の人定したレー→J−を1;する仁とができること
、 Jl振鏡の間隔を制御するにはレー→” h’l 
I(i管の温度を制御すれはよく、そのためには送風機
によってh!電官のまわりの空気の涼れを制i1+1す
れは筒中な装置で目的が達せら1]ることが知らiして
いる。 ずなわら、光ヒート周波数と希望する設定周波数O)差
を検出し、光ビート周波数が設定周波数と異なっておれ
ば、周波数差がなくなるように送風機に印加する電Ji
Eを加減し、ビート周波数が一定となるように其振鏡の
間隔つまり几振器長を制御することは口J能である。こ
の方V、は、レーザー装置の周flJIの気温が一定で
あれば、1.′l性能を発揮するが。 周囲の気温が変化すれはそれに伴−)゛(周波数の変動
を伴なうという欠点をイjす。九来、送風X、1の加減
は一定の量のまわりの加減であり、零を中心とした加減
は不f+J能であるため常に一定のバイアス送風量を与
えそのまわりで加減しなけfLはならす、従って、送風
機の電動機に印加する電圧は一定のバイアスイ♂Iのオ
オンりで力11減しな(す11はならないが、その電圧
とヒート周波数は一義的に対応がついてしまっているた
め気温が変化すれは困難が生じる。 すなわち、気温が変化すれはb(電管の温度を一定とす
る1こ要する風f1
The present invention relates to a device for stabilizing the oscillation frequency of a racer. When internal light in the earth's magnetic field or other magnetic field is passed through a polarizer, the optical heat becomes +1111, and as the frequency of the optical heat becomes constant, <J(& By controlling the mirror spacing, the oscillation station l
It is possible to control the interval of the J-mirror by setting the reciprocal number of ray→J- to 1;
I (I know that it is good to control the temperature of the tube, and for that purpose, the blower must be used to control the coolness of the air around the electrician. This is accomplished by a device inside the tube. However, the difference between the optical heat frequency and the desired set frequency is detected, and if the optical beat frequency is different from the set frequency, the electric current applied to the blower is adjusted so that the frequency difference disappears.
It is a matter of skill to adjust the value of E and control the distance between the vibrating mirrors, that is, the vibrator length, so that the beat frequency is constant. This direction V, if the temperature around the laser device flJI is constant, 1. 'l shows excellent performance. As the ambient temperature changes, the disadvantage is that the frequency changes. Since the adjustment is an ineffective f + J function, a constant bias air flow rate must always be given and adjustment around it will make fL equal.Therefore, the voltage applied to the blower's motor will decrease by 11 when the bias I is turned on. However, since there is a unique correspondence between the voltage and the heat frequency, it becomes difficult when the temperature changes.In other words, when the temperature changes, It takes 1 wind f1

【か痩化する。従って電動機0)1
cI1.も変化し’、IL Hに対応したし−ト周波数
、ひいては発振周波数が変化する。 本発明は送風機を主体としたレーザー発振周波数の制御
装置において周囲の気温に変化が生しても・発!1if
E波数に変化を生じせしめない制御システムに関するも
ので本発明により、環境の変化の影響を受けることのな
い、しがもム価14周l)l数安定化し−ガー装置の実
現が「り能とtつな。 工゛1下図1h1によりΔ、発明0)訂和1な説明を行
へう第11’4は制御jI:の説明図で7)る。丸ヒ−
Iを検出し光ヒート周ンル数を電Hに変換し、その1u
1(を送風機の電動機に印加した場合の印加電圧をXと
する。こ(D jlj圧は光ヒート周波数に比例した屯
月yと常fこ風11:を一定値のまわりで変化させるt
ζめのハイアノ、を月2の和となっている。光ヒート周
ン皮故に変化が生じると電圧yか変化し、光ヒー 1−
周、Jk数が凡の設定4+1+に0・きもとさお、周波
数の安定化が行なわれる。しかし、テシ圧Xはレーサー
放電管の発生熱h1と冷却J虱量の極めて微妙なバラン
スで決るfilであり周囲の気温が完1゛に安定”Cあ
れは変化することはないが、気温が変動するとそれに従
って微妙に変化する。ある気温で電圧Xが熱バランスに
適した(■−となI)、がっ、yが[1的のヒート周波
数に対応した値になるよう、バイフス電IJE2を調整
設定すると安定化がスタートするのであるが、バイアス
電圧2が一定である場合、気温が変化するとバランスを
とるため゛市1j−Xは自然に変化しそれに従って電月
yつまり安定化さiまた光ビート周波数が変化する。本
発明は気温が変化しても光ビー1・周波数、ひいてはレ
ーザー発振周波数が変化しないようにするものである。 すなわち、光ビート周波数の設定値からの変化め徴候が
見られるとバイアス電月2の値を除々に変化して光ビー
ト周波数の変化を抑制を行なうものであり、Xが変化し
た場合yは変化せず、2のみが変化して温度変化19の
悪影響を除くものである。第2図は本発明の実施例であ
る。弱磁場中のレーづ一発振tic +の発振光を偏光
二f2を通して光ビートを検知間3で検・出し広帯減増
itM略4で増11」シ周波数−’、u 11: 14
’換器5で周波数は°市Hに変換されス動増1+る。準
基′^1・周波数設定部はバイアスZを含めたhiの設
定を行なうものである。 力先ビート周波数は、基準周
波数発生器(基へ(周波数設定部)の周波数と比較回路
(]で比較される。比Il+Q回路fi f4比較さi
]だ周波数のZがゎずがてもI’/’ (Eすれはスの
11、負1こ応し正、負の1tjl土を光(1する。発
生したjl、あるいは負fj) Y(i圧は長時定数。 ) b’J分1741路或いはカウンター雪積5J機能
をイエする回路1()で周波数差に応じゆっくり増減す
る1u気イ1、IIにかえられ加p回路目で、先の((
1hし1(周波数設定部を通った414号に加9さfす
る。前記のゆっくり増減する+、i ’;が+iiJ記
y、 (1)値の補J[、を7fなう。補11:された
(j ’Jは送!la機の電動機Mに加えらJ]る。 第2図は他の実施例である。この例においては加t′7
を電気回路でjfなゎず、準J、L 71!周波数設定
部をj市つたイ11弓を増ij器12で増11ノシて゛
16動機N1に加え、回路10の出方はレーナーb′i
電管の一部fこおがれたヒーターll1t駆−動して熱
的に加37をjfなう例である。 第、3図は他の実施例である。Cの例では光ビートイ1
」号の周波数が電圧fr ’tチに変換された後に((
ξ基準周波数設定部と)J準周波数設定部に配分されて
いる。VH2は準基べ(周波数設定部でる留置波数に対
応しfこ電圧とバイアスのλ−を決めるボテノンヨメー
クーである。ボテノノヨメーターVR2の電圧と周波数
−電圧変換された電圧の差が増rl器】4で増d」され
演算項lJ器】5の一方の入力となっている。 他力ボテノノヨメーターVR,は基準周波数設定部でノ
^準周波数に対応した基へf主1を決める。増ll+ 
2i+13は無限大の利得を有する増I+]器で周波数
−電圧変換された電圧が極くわずかでも悶ければrlの
。 低ければ+1、の一定電月、を発41する1(、Cは長
時定数を自する積分回路で一定11ffl11の正負に
見、じ端子電ttはゆっくり上4あるいは1・降するこ
のゆっくり変化する電圧を増+lJ器16で増巾し演算
増巾器15の他の入力端に入れ、演算増巾器15で加算
を行なった屯ルを電動機Mに印加しでいる。
[Or lose weight. Therefore, electric motor 0)1
cI1. The output frequency also changes, and the output frequency corresponding to ILH changes, and thus the oscillation frequency changes. The present invention provides a laser oscillation frequency control device that uses a blower as its main component, even if there is a change in the ambient temperature. 1if
This invention relates to a control system that does not cause a change in the E wave number, and the present invention makes it possible to realize a device that stabilizes the number of 14 cycles and is not affected by changes in the environment. 11'4 is an explanatory diagram of control jI: 7).
Detect I, convert the number of light heat cycles to electric H, and
Let X be the applied voltage when 1 (is applied to the electric motor of the blower).
The ζth high anno is the sum of 2 per month. Because of the light heat cycle, when a change occurs, the voltage y changes, and the light heat 1-
When the number of laps and Jk is set to 4+1+, the frequency is stabilized. However, the pressure X is determined by the extremely delicate balance between the heat generated by the racer discharge tube and the amount of cooling, so the surrounding temperature remains perfectly stable. When the temperature fluctuates, it changes slightly accordingly.At a certain temperature, the voltage When the bias voltage 2 is adjusted and set, stabilization starts, but if the bias voltage 2 is constant, when the temperature changes, in order to balance In addition, the optical beat frequency changes.The present invention prevents the optical beam 1 frequency and ultimately the laser oscillation frequency from changing even if the temperature changes.In other words, there is no sign of a change in the optical beat frequency from the set value. When , the value of bias electric moon 2 is gradually changed to suppress the change in the optical beat frequency, and when X changes, y does not change, only 2 changes, and temperature change 19. Figure 2 shows an embodiment of the present invention.The oscillation light of the laser beam tic+ in a weak magnetic field is passed through polarized light 2f2, and the optical beat is detected and detected in the detection interval 3. Increase it M approximately 4 and increase 11" frequency -', u 11: 14
The converter 5 converts the frequency to °C and increases the frequency by 1+. The standard '^1/frequency setting section is for setting hi including bias Z. The output beat frequency is compared with the frequency of the reference frequency generator (frequency setting section) by the comparison circuit (). Ratio Il + Q circuit fi f4 comparison
] Even if the Z of the frequency is shifted, I'/' (E is 11 of S, negative 1 corresponds to positive, negative 1tjl earth (1. Generated jl, or negative fj) Y( The i pressure is a long time constant.) b'J minute 1741 circuit or the counter snow accumulation 5J function in circuit 1 (), which increases and decreases slowly according to the frequency difference, is changed to 1, II and added in the pth circuit, Previous((
1h and 1 (Add 9 and f to No. 414 that passed through the frequency setting section. The slowly increasing and decreasing +, i'; is +iiJ notation, (1) Complement J[, of the value is 7f. Complement 11 :(j 'J is added to the electric motor M of the sending!la machine). Figure 2 shows another embodiment. In this example,
In electrical circuits, jf, quasi J, L 71! The frequency setting part is set to J, and the 11 bow is increased by 11 to 12 by the intensifier 12.16 In addition to the motive N1, the output of the circuit 10 is Lehner b
This is an example in which a part of the electric tube is burnt and the heater is driven to thermally heat the tube. Figures 3 and 3 show other embodiments. In the example of C, optical beat toy 1
After the frequency of ' is converted into voltage fr't ((
ξ reference frequency setting section and ) J quasi-frequency setting section. VH2 is a reference standard (corresponding to the indwelling wave number output from the frequency setting section, and is a bottom value that determines the voltage and bias λ-.The difference between the voltage of the bottom weight meter VR2 and the frequency-voltage converted voltage) is incremented by 4 and becomes one input of the operational term lJ5. Decide on main 1. Increase +
2i+13 is an intensifier I+ with infinite gain, and if the frequency-voltage converted voltage is even slightly distorted, rl. If it is low, it emits a constant electric current of +1, 41 (1), C is an integrating circuit with a long time constant, and it is a constant 11ffl11. The voltage is amplified by an intensifier 16 and inputted to the other input terminal of the arithmetic amplifier 15, and the voltage added by the arithmetic amplifier 15 is applied to the motor M.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は原理説明図、第2図は本発明の実施例第4図は
他の実施例第4図は他の実施例である。 1・・・・・ レーザー管 2・・・・・・・・・偏光子 3・・・・・・ 検知器 5・・・−周波数−電圧変換器 6・・・・・−比較回路 7・ ・ JA準局周波数設定 器 −−i′1!+ )A 116周波数設定F1.’
4!)、+ 2−11T & Ifl I 品1()−
・・積分機能を杓する回路 11 − 加Z′11回路 1、(・・・ 利?1)無限大の増巾器」4.15.1
ら ・ −・ 直於増11J Ri4M−・・・ 送風
機駆動電動機 X・yiZ −電圧準位 VR,、va2・ −ボテノノヨメーター1ζ ・ 抵
抗イμl C・−・・容Iル 19 命 オH幻 昨41¥1
FIG. 1 is a diagram illustrating the principle, and FIG. 2 is an embodiment of the present invention. FIG. 4 is another embodiment. 1...Laser tube 2...Polarizer 3...Detector 5...-Frequency-voltage converter 6...-Comparison circuit 7-・JA quasi-station frequency setter --i'1! +)A 116 Frequency setting F1. '
4! ), + 2-11T & Ifl I item 1()-
...Circuit 11 that scales the integral function - Addition Z'11 circuit 1, (... profit? 1) Infinite amplifier" 4.15.1
Era・-・Direct increase 11J Ri4M-... Blower drive motor Phantom past 41 yen 1

Claims (1)

【特許請求の範囲】 地球1」場その他の弱磁場により生ずる2つのムダする
(lnin発光光の光ヒート周波数が一定となるごとく
送風機の風Ulを変化せしめることによりレーサー敢+
tr tqの温度を制御する周波数安定化レー→を一装
置において、花9!周波数と送風機駆動電動機のバイア
ス値を設定する準基ハt・周波数設定部とh(岸周波数
を設定する2i; i(a周波数設定部をもうけ1、−
(準基7i1−周波数設定部において設定された設定値
と光ビート局波数の差を1a気信シ)に変換しバイアス
準(ifを加えて送風機駆動1【L動機に印加し、光ビ
ないごとく該印加4:、1 ”jを変化せしめレーサー
共振器長をはシ一定に保つと共に110記基準周波数設
定部により設定された)I(準用波数と光ビート周波数
のスの正、負を判別し、積分機能を有する回路等により
該周波数差の比色に応じ除々に増加あるいは減lトを行
なう電気411号をつくり該Gj号を前記の送風機駆動
電動機h機に印加されるイ、1月に加pすることにより
+iil記レーサし共振黙の」)、搬体;長を正確に一
定に保つ、ことを特徴とする周波数人定化レーサー装置
[Claims] By changing the wind Ul of the blower so that the optical heat frequency of the light emitted light is constant, two wastes caused by the earth's field and other weak magnetic fields can be improved.
A frequency stabilizing relay → that controls the temperature of tr tq is placed in one device, and flower 9! A reference standard for setting the frequency and the bias value of the blower drive motor.
(Standard standard 7i1 - Convert the difference between the set value set in the frequency setting section and the optical beat station wave number to 1a air signal) and apply it to the blower drive 1 [L motor by adding the bias standard (if). The application 4:,1''j is varied to keep the laser resonator length constant, and the positive or negative of the wave number and the optical beat frequency set by the reference frequency setting section 110 is determined. Then, a circuit having an integral function or the like is used to create electricity No. 411 that gradually increases or decreases in accordance with the colorimetry of the frequency difference, and the Gj No. 411 is applied to the blower drive motor h. A frequency-regulated racer device characterized in that the length of the carrier is maintained accurately constant by adding the laser beam to the laser beam and the length of the carrier is kept accurately constant.
JP14468983A 1983-08-08 1983-08-08 Frequency stabilized laser device Pending JPS6035588A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP14468983A JPS6035588A (en) 1983-08-08 1983-08-08 Frequency stabilized laser device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP14468983A JPS6035588A (en) 1983-08-08 1983-08-08 Frequency stabilized laser device

Publications (1)

Publication Number Publication Date
JPS6035588A true JPS6035588A (en) 1985-02-23

Family

ID=15367967

Family Applications (1)

Application Number Title Priority Date Filing Date
JP14468983A Pending JPS6035588A (en) 1983-08-08 1983-08-08 Frequency stabilized laser device

Country Status (1)

Country Link
JP (1) JPS6035588A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62270875A (en) * 1986-05-17 1987-11-25 Toshio Takemura Drain cock controller
US4918700A (en) * 1988-03-31 1990-04-17 Cselt - Centro Studi E Laboratori Telecomunicazioni S.P.A. Method and device for automatic frequency control of semiconductor lasers

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62270875A (en) * 1986-05-17 1987-11-25 Toshio Takemura Drain cock controller
US4918700A (en) * 1988-03-31 1990-04-17 Cselt - Centro Studi E Laboratori Telecomunicazioni S.P.A. Method and device for automatic frequency control of semiconductor lasers

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