JPS58223392A - Ion laser device - Google Patents

Ion laser device

Info

Publication number
JPS58223392A
JPS58223392A JP10741582A JP10741582A JPS58223392A JP S58223392 A JPS58223392 A JP S58223392A JP 10741582 A JP10741582 A JP 10741582A JP 10741582 A JP10741582 A JP 10741582A JP S58223392 A JPS58223392 A JP S58223392A
Authority
JP
Japan
Prior art keywords
laser
output
laser tube
gas
tube
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
JP10741582A
Other languages
Japanese (ja)
Inventor
Norio Takahashi
鷹「はし」 紀雄
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.)
NEC Corp
Original Assignee
NEC Corp
Nippon Electric Co Ltd
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 NEC Corp, Nippon Electric Co Ltd filed Critical NEC Corp
Priority to JP10741582A priority Critical patent/JPS58223392A/en
Publication of JPS58223392A publication Critical patent/JPS58223392A/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
    • H01S3/131Stabilisation of laser output parameters, e.g. frequency or amplitude by controlling the active medium, e.g. by controlling the processes or apparatus for excitation

Abstract

PURPOSE:To keep light output constant by correcting the gas pressure of a laser tube automatically and properly by a method wherein a gas reserve whose package is a bellows is provided to the laser tube. CONSTITUTION:The gas reserve 16 in a bellows structure is connected to the laser tube 9 via a supporting tube 17. Partial laser light 13 of the laser output 12 is detected by a photodetector 6, and the difference voltage between the output voltage and reference voltage thereof is amplified by a comparing amplifier 3. This output is supplied to a motor cylinder 15 via a motor cylinder drive circuit 14. Thereby, the gas pressure of the laser tube 9 is adjusted so that the volume of the gas reserver 16 changes into the specified laser output. Thus, the output can be kept constant by correcting the gas pressure of the laser tube automatically and properly.

Description

【発明の詳細な説明】 本発明は、イオンレーザ装置、特に光出力の安定化を図
ったイオンレーザ装置に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an ion laser device, and particularly to an ion laser device with stabilized optical output.

従来、イオンレーザ装置では光出力の安定化を図るため
、レーザ出力の一部を検出しそれが一定になるようにレ
ーザ管の放電電流を制御する帰還回路が用いられている
。すなわち、141図に示すように直流電源Iの一つの
出力端をレーザ管9のカソード10に接続し、他端をト
ランジスタ2全通してレーザ管9のアノード11に接続
する。そして、レーザ光12の一部のレーザ光13を光
検出器6で検出し、抵抗5の両端に現われる出力電圧と
基準電源4との差電圧を比較増幅器3で増幅゛シ、トラ
ンジスタ2のベースに供給し、差電圧が0になるように
制御している。しかし、イオンレーザ装置は、レーザ管
内の封入希ガスをイオン化するために大電流(20〜4
0A)のアーク放電をさせるため、トランジスタ2は大
容量、大型。
Conventionally, in order to stabilize the optical output of an ion laser device, a feedback circuit has been used that detects a portion of the laser output and controls the discharge current of the laser tube so that it remains constant. That is, as shown in FIG. 141, one output end of the DC power supply I is connected to the cathode 10 of the laser tube 9, and the other end is connected to the anode 11 of the laser tube 9 through the entire transistor 2. Then, a part of the laser beam 13 of the laser beam 12 is detected by the photodetector 6, and the difference voltage between the output voltage appearing across the resistor 5 and the reference power source 4 is amplified by the comparator amplifier 3. The voltage difference is controlled to be zero. However, the ion laser device requires a large current (20 to 4
Transistor 2 has a large capacity and is large in order to generate an arc discharge of 0 A).

高価となる。また、アーク放電によるガスクリーンアッ
プ作用によリレーザ管内のガスが減少する。
It becomes expensive. Further, the gas inside the laser tube decreases due to the gas clean-up effect caused by the arc discharge.

レーザ封入ガスが減少すると、レーザ管電圧が減少し、
減少が進むと正常な放電が行なわれなくなり、管の動作
が停止して使用不能となる。
When the laser fill gas decreases, the laser tube voltage decreases,
As the amount decreases, normal discharge will no longer occur, and the tube will stop operating and become unusable.

本発明の目的は、トランジスタ2を使用せず小型、安価
にし、レーザ管のガス圧を自動的かつ適正に補正し、長
期間にわたり安定な動作をするイオンレーザ装置を提供
するにある。
An object of the present invention is to provide an ion laser device that does not use a transistor 2, is small and inexpensive, automatically and appropriately corrects the gas pressure in the laser tube, and operates stably over a long period of time.

次に第2図に示した実施例により本発明の詳細な説明す
る。図において、直流電源lの一つの出力端をレーザ管
9のカソード10に接続し、他端をレーザ管9のアノー
ド11に接続する。7.7′はレーザ管9をはさんで対
向配置の共振器ミラーであり、16はレーザ管9と支管
17により接続されたガスリザーバで、ガスリザーバ1
6はベローズ構造になっており、モータシリンダ15に
よって容積を変えられる。
Next, the present invention will be explained in detail with reference to the embodiment shown in FIG. In the figure, one output end of the DC power supply l is connected to the cathode 10 of the laser tube 9, and the other end is connected to the anode 11 of the laser tube 9. 7.7' is a resonator mirror placed oppositely across the laser tube 9; 16 is a gas reservoir connected to the laser tube 9 by a branch pipe 17;
6 has a bellows structure, and its volume can be changed by a motor cylinder 15.

レーザ管9が放電し、レーザ出力■2の一部のレーザ光
13が光検出器6により検出され、抵抗5の両端に現わ
れる出力電圧と基準電源4との差電圧を比較増幅器3で
増幅し、モータシリンダ駆動回路14を動作させ、モー
タシリンダ15を駆動し、ガスリザーバ16のベローズ
部を縮め、レーザ管9のガス圧を上昇させ、規定のレー
ザ出力になるまでレーザ管9のガス圧を調整する。その
結果、初期状態では第3図(麹の曲線19の(a)点に
レーザ管9のガス圧は調整される。また約1oooH動
作後レーザ管9の光学窓22.22’がある程度汚れる
と、第3図(B)の曲線20の(b)点にレーザ管9の
ガス圧は調整される。そして約2000H動作後レーザ
管9の光学窓22.27がさらに汚れると、第3図(B
)の曲線21のFC)点にレーザ管9のガス圧は調整さ
れる。なお前記第3図fBlのfa)、 (b)。
The laser tube 9 discharges, a part of the laser beam 13 of the laser output 2 is detected by the photodetector 6, and the difference voltage between the output voltage appearing across the resistor 5 and the reference power source 4 is amplified by the comparator amplifier 3. , operates the motor cylinder drive circuit 14, drives the motor cylinder 15, contracts the bellows portion of the gas reservoir 16, increases the gas pressure in the laser tube 9, and adjusts the gas pressure in the laser tube 9 until the specified laser output is reached. do. As a result, in the initial state, the gas pressure in the laser tube 9 is adjusted to point (a) of the koji curve 19 in FIG. , the gas pressure in the laser tube 9 is adjusted to point (b) of the curve 20 in FIG. B
The gas pressure in the laser tube 9 is adjusted to the point FC) of the curve 21 of ). In addition, fa) and (b) of FIG. 3 fBl.

(C)点のガス圧の時レーザ管9のアノード11. カ
ッーFlO間の放電電流(アノード電流〕は第3図(四
の曲線18の(a)、 (b)、 (C)点の電流とな
る。
At the gas pressure at point (C), the anode 11 of the laser tube 9. The discharge current (anode current) between Ka-FLO is the current at points (a), (b), and (C) of curve 18 in Figure 3 (4).

以上のように、レーザ管9のガス圧を制御することによ
りレーザ出力12は一定に保たれ、前記アーク放電によ
るガスクリーンアップ作用によるレーザ管9のガス圧減
少も自動的に補正されるので、常にレーザ管9のガス圧
は適正に保たれる。
As described above, by controlling the gas pressure in the laser tube 9, the laser output 12 is kept constant, and the decrease in the gas pressure in the laser tube 9 due to the gas clean-up effect due to the arc discharge is automatically corrected. The gas pressure in the laser tube 9 is always maintained at an appropriate level.

以上のべたように規格レーザ出力を出力するためにレー
ザ管9のガス圧は最高に、アノード電流は最小に自動的
に調整される。よってレーザ管9のアーク放電によるガ
スクリーンアップは最少になるよう抑制され、長期間に
わたって安定なレーザ出力を得ることができる。
As described above, in order to output the standard laser output, the gas pressure in the laser tube 9 is automatically adjusted to the maximum and the anode current to the minimum. Therefore, gas clean-up due to arc discharge in the laser tube 9 is suppressed to a minimum, and stable laser output can be obtained over a long period of time.

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

第1図は従来のイオンレーザ装置を示すブロック図、第
2図は本発明のイオンレーザ装置を示すブロック図、第
3図(A)は本発明のイオンレーザ装置のレーザ管内ガ
ス圧対アノード電流、第3図(均はレーザ管内ガス圧対
レーザ出力特性を示す曲線図である。 ■・・・・・・直流電源、2・・・・・・トランジスタ
、3・・・・・・比較増幅器、4・・・・・・基準電源
、5・・・・・・抵抗、6・・・・・・光検出器、7.
1・・・・・・光共振器、8・・・・・・ビームスプリ
ッタ、9・・・・・・ガスレーザ管、10・・・・・・
カソード、11・・・・・・アノード、12.13・・
・・・・レーザi、14・・・・・・モータシリンダ駆
動回路、15・・・・・・モータシリンダ、16・・・
・・・ガスリザーバ、17.・・・・・支管。 5 − し−プ゛藩井何カス圧(Torr し−サ噛−9〃′ヌ圧(丁Or腔〕 狛37 (A) ン (ヒシ) 401−
FIG. 1 is a block diagram showing a conventional ion laser device, FIG. 2 is a block diagram showing an ion laser device of the present invention, and FIG. 3 (A) is a graph showing gas pressure in the laser tube versus anode current of the ion laser device of the present invention. , Figure 3 (average is a curve diagram showing the gas pressure in the laser tube vs. laser output characteristics. ■...DC power supply, 2...transistor, 3...comparison amplifier , 4...Reference power source, 5...Resistor, 6...Photodetector, 7.
1... Optical resonator, 8... Beam splitter, 9... Gas laser tube, 10...
Cathode, 11... Anode, 12.13...
...Laser i, 14...Motor cylinder drive circuit, 15...Motor cylinder, 16...
...Gas reservoir, 17. ...Branch pipe. 5 - Torr Shi-Sagami-9〃'nu Pressure (Teng Or cavity) Koma 37 (A) N (Hashi) 401-

Claims (1)

【特許請求の範囲】[Claims] ベローズを外囲器とするガスリザーバを備えたレーザ管
と、このレーザ管の動作電圧を供給する直流電源と、レ
ーザ管からのレーザ光の一部を検出し、その値が一定に
なるよう前記ガスリザーバのベローズ部を制御するモー
タシリンダを駆動するモータシリンダ駆動回路とを備え
たことを特徴とするイオンレーザ装置。
A laser tube equipped with a gas reservoir having a bellows as an envelope, a DC power supply that supplies the operating voltage of this laser tube, and a part of the laser beam from the laser tube that detects a portion of the laser beam and uses the gas reservoir to keep the value constant. An ion laser device comprising: a motor cylinder drive circuit that drives a motor cylinder that controls a bellows portion of the ion laser device.
JP10741582A 1982-06-22 1982-06-22 Ion laser device Pending JPS58223392A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP10741582A JPS58223392A (en) 1982-06-22 1982-06-22 Ion laser device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP10741582A JPS58223392A (en) 1982-06-22 1982-06-22 Ion laser device

Publications (1)

Publication Number Publication Date
JPS58223392A true JPS58223392A (en) 1983-12-24

Family

ID=14458563

Family Applications (1)

Application Number Title Priority Date Filing Date
JP10741582A Pending JPS58223392A (en) 1982-06-22 1982-06-22 Ion laser device

Country Status (1)

Country Link
JP (1) JPS58223392A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5947786A (en) * 1982-08-06 1984-03-17 フエランテイ・ピ−エルシ− Gas laser device
WO1995034927A1 (en) * 1994-06-16 1995-12-21 Komatsu Ltd. Laser gas controller and charging-discharging device for discharge-excited laser

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5947786A (en) * 1982-08-06 1984-03-17 フエランテイ・ピ−エルシ− Gas laser device
JPH023313B2 (en) * 1982-08-06 1990-01-23 Ferranti Plc
WO1995034927A1 (en) * 1994-06-16 1995-12-21 Komatsu Ltd. Laser gas controller and charging-discharging device for discharge-excited laser
US5754579A (en) * 1994-06-16 1998-05-19 Komatsu Ltd. Laser gas controller and charging/discharging device for discharge-excited laser

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