JPS62265785A - Gas laser oscillator - Google Patents

Gas laser oscillator

Info

Publication number
JPS62265785A
JPS62265785A JP10856186A JP10856186A JPS62265785A JP S62265785 A JPS62265785 A JP S62265785A JP 10856186 A JP10856186 A JP 10856186A JP 10856186 A JP10856186 A JP 10856186A JP S62265785 A JPS62265785 A JP S62265785A
Authority
JP
Japan
Prior art keywords
gas laser
oxygen concentration
discharge tube
point
reference value
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
JP10856186A
Other languages
Japanese (ja)
Inventor
Yutaka Uchida
裕 内田
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.)
Toshiba Corp
Original Assignee
Toshiba 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 Toshiba Corp filed Critical Toshiba Corp
Priority to JP10856186A priority Critical patent/JPS62265785A/en
Publication of JPS62265785A publication Critical patent/JPS62265785A/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
    • H01S3/02Constructional details
    • H01S3/03Constructional details of gas laser discharge tubes
    • H01S3/036Means for obtaining or maintaining the desired gas pressure within the tube, e.g. by gettering, replenishing; Means for circulating the gas, e.g. for equalising the pressure within the tube

Landscapes

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

Abstract

PURPOSE:To perform the stable laser oscillation at the optimum consumption while avoiding the wasteful consumption of medium by a method wherein an oxygen concentration detector 12 is provided in a discharge tube 1 exciting gas laser medeum which is exhausted from and supplied for the discharge tube 1 to keep the oxygen concentration within the range of reference value. CONSTITUTION:When the concentration of oxygen contained in a gas laser medium exceeds 0.3-0.4% changing from glow discharge to arc discharge, the excitation is deteriorated so markedly that it is very important to maintain the glow discharge for stable laser oscillation. A controller 13 provided with a circuit comparing detection signals with the reference value can input operation signals to a flow rate regulating valve 9 and an electromagnetic valve 11 whenever the detection signals exceed the reference value. When the oxygen concentration reaches a point (a), exhaust and supply of oxygen are stopped while reaching a point (c), the flow rate regulating valve 9 and the electromagnetic valve 11 are opened for specified time to reset the oxygen concentration to the point (a). Through these procedures, the stable laser oscillation can be performed while avoiding the wasteful consumption of excessive gas laser medium.

Description

【発明の詳細な説明】 〔発明の目的〕 (産業上の利用分野) 本発明はガスレーザ発鳴装置に係り、特にレーザガスを
所定量補充・排気する方式の装(けに関する。
DETAILED DESCRIPTION OF THE INVENTION [Object of the Invention] (Industrial Field of Application) The present invention relates to a gas laser emitting device, and particularly to a system for replenishing and exhausting a predetermined amount of laser gas.

(従来の技術) 比較的高出力のガスレーザ発振装置ではレーザ運転中の
ガスレーザ媒質の劣化にょるレーザ出力の低下を防止す
るため、ガスレーザ媒質を連続もしくは時間を決めて所
定量補充するようにしてレーザ利得の低下を防いでレー
ザ出力を安定化することが行われている。たとえばガス
レーザ媒質の圧力を1気圧程度にしてレーザ発振するT
EA(Transversely Excited A
tomosphric pressure ) Co。
(Prior art) In a relatively high-output gas laser oscillator, in order to prevent a decrease in laser output due to deterioration of the gas laser medium during laser operation, a predetermined amount of gas laser medium is replenished continuously or at fixed times. Efforts are being made to stabilize the laser output by preventing a decrease in gain. For example, T
EA (Transversely Excited A)
tomosphere pressure) Co.

レーザ発振装!では2L/分程度の量でガスレーザ媒質
が消費されていた。上記の値はガスレーザ媒質のレーザ
発振中におけるガス成分の変化について何ら考慮してお
らず、経験的に求めたもので。
Laser oscillator! In this case, the gas laser medium was consumed at a rate of about 2 L/min. The above values do not take into account any changes in gas components during laser oscillation of the gas laser medium, and were determined empirically.

ガス成分変化を許容範囲内江おさまるように制御してい
るわけではない。したがって、レーザ発振の安定を計る
あまり過剰のガスレーザ媒質を使用することになり、十
分に使用可能なガスレーザ媒質を使用するこ(!:(て
なり、十分に使用可能なガスレーザ媒質を流し捨ててい
た問題があった。
This does not mean that the change in gas composition is controlled to stay within the permissible range. Therefore, in order to stabilize the laser oscillation, an excessive amount of gas laser medium is used. There was a problem.

(発明が解決しようとする問題点) 以上のようにガスレーザ媒質が無駄に消費されていた点
に鑑み1本発明は最適な消費量で安定なレーザ発振が行
えるガスレーザ発振装置を提供することを目的とする。
(Problems to be Solved by the Invention) In view of the wasteful consumption of gas laser media as described above, an object of the present invention is to provide a gas laser oscillation device that can perform stable laser oscillation with optimal consumption. shall be.

〔発明の構成〕[Structure of the invention]

(問題点を解決するための手段と作用)ガスレーザ発振
装置において、ガスレーザ媒質を励起する放電管内に酸
素濃度積出器を設は酸素濃度の基準値を越えた検出信号
で酸素濃度が基準値内になるよう放電管に対するガスレ
ーザ媒質の排気と補充を行う構成にしたものである。
(Means and effects for solving the problem) In a gas laser oscillation device, an oxygen concentration transmitter is installed in the discharge tube that excites the gas laser medium, and a detection signal exceeding the oxygen concentration standard value indicates that the oxygen concentration is within the standard value. The structure is such that the gas laser medium is evacuated and refilled from the discharge tube so as to achieve the following.

(実施例) 以下、実施例を示す図面に基いて本発明を説明する。(Example) EMBODIMENT OF THE INVENTION Hereinafter, this invention will be explained based on drawing which shows an Example.

本発明を説明する前に1本発明に至った経緯について説
明する。すなわち、第2図はTEA Co、レーザ発振
装置におけるガスレーザ媒質中の酸素濃度とアーク発生
率の関係を示したものである。この図から明らかなよう
に酸素濃度が0.3〜0.4%を越えるとアーク発生率
が急激に増加する。周知のようにTEA Co、レーザ
やエキシマレーザ等ではグロー放電によってガスレーザ
媒質を励起しているが。
Before explaining the present invention, the circumstances leading to the present invention will be explained. That is, FIG. 2 shows the relationship between the oxygen concentration in the gas laser medium and the arc generation rate in a TEA Co laser oscillator. As is clear from this figure, when the oxygen concentration exceeds 0.3 to 0.4%, the arc occurrence rate increases rapidly. As is well known, in TEA Co, laser, excimer laser, etc., a gas laser medium is excited by glow discharge.

グロー放電からアーク放電になってしまうと励起作用は
極めて悪くなり、安定したレーザ発振ζつためにはグロ
ー放電を維持させることが重要である。
If the glow discharge turns into an arc discharge, the excitation effect becomes extremely poor, and it is important to maintain the glow discharge in order to achieve stable laser oscillation.

以上のことから1本発明は一実施例である41図に示す
ように構成したものである。すなわち。
In view of the above, one embodiment of the present invention is constructed as shown in FIG. 41, which is an embodiment. Namely.

(1)は筒状の気密容器からなる放電管で、内部には放
気i!極である陽極(2)と陰極(3)とが対峙して設
けられ、電源部(4)から高圧の直流パルスの供給を受
けるようになっている。(5)、CG)は光共振器を構
成する全反射鏡および出力鏡で、放電W(1)の両端側
にこの放電管(1)の軸と同軸に位置して気密に取り付
けられている。(力は放電管(1)内にガスレーザ媒質
を供給する供給源でその供給管(7a)には圧力h!1
1整器(8)および流量調整弁(9)が設けられている
。θQは放電管(1)に接続されている排気管で、′α
電磁弁υが設けられている。上記放電管(1)の内部例
は酸素濃度検出器(121が設けられ、その検出信号は
制御装置α9に送られるようになっている。ここで、上
記符号(7)乃至(11Jで表示された各構成要素でガ
ス交換手段が構成されている。上記制御装置α3は上記
検出信号を基準値と比較する回路を有するとともに基準
値を越えた信号が得られた場合には流量調整弁(9)お
よび電磁弁(lυに作動信号を送るようになっている。
(1) is a discharge tube consisting of a cylindrical airtight container, with air released inside! An anode (2) and a cathode (3), which are poles, are provided facing each other, and are supplied with high-voltage DC pulses from a power source (4). (5), CG) are a total reflection mirror and an output mirror that constitute an optical resonator, and are airtightly installed on both ends of the discharge W (1) coaxially with the axis of the discharge tube (1). . (The force is the supply source that supplies the gas laser medium into the discharge tube (1), and the pressure h!1 in the supply tube (7a)
A regulator (8) and a flow rate regulating valve (9) are provided. θQ is the exhaust pipe connected to the discharge tube (1), and ′α
A solenoid valve υ is provided. The internal example of the discharge tube (1) is provided with an oxygen concentration detector (121), the detection signal of which is sent to the control device α9. Each component constitutes a gas exchange means.The control device α3 has a circuit for comparing the detection signal with a reference value, and when a signal exceeding the reference value is obtained, a flow rate regulating valve (9) is provided. ) and a solenoid valve (lυ).

ここで上記制御装R(13の具体的な制御動作を第3図
に基いて説明する。すなわち、同図において、酸素濃度
の(a)、 (b)、 (C)の各点に達する放電回数
を計測し、酸素濃度が0.3〜0.4%の中間の(d)
点に至るまでの放電回数を予測する。この場合、酸素濃
度の増加は放電回数に対して指数関係で近似できる。な
お、上記(C)点は(d)点の1/2 、 (b)点は
(C)点の1/2 、 (a)点は(b)点の1/2に
なる酸素濃度を示す点である。また、(d)点は、任意
に設定するものとするが好ましくは4%近傍がよい。次
に、(d)点に至るまでの時間C(d点での放電回数−
現在までの放電回数)/放電線り返し数〕tを計算する
う” この値をもとに排気量および同1の補充量を排気
f(補充量)=放′fル管のガス容量/l  C’−、
勢〕の式によって求め、排気および補充を開始する。
Here, the specific control operation of the control device R (13) will be explained based on FIG. Measure the number of times, and (d) where the oxygen concentration is between 0.3 and 0.4%.
Predict the number of discharges until reaching the point. In this case, the increase in oxygen concentration can be approximated by an exponential relationship with the number of discharges. Note that point (C) above is 1/2 of point (d), point (b) is 1/2 of point (C), and point (a) is 1/2 of point (b). It is a point. Further, the point (d) may be set arbitrarily, but preferably around 4%. Next, time C until reaching point (d) (number of discharges at point d -
Calculate the number of discharges up to now)/number of discharge line repetitions] t. Based on this value, calculate the exhaust volume and the replenishment volume of the same 1. Exhaust f (replenishment volume) = gas capacity of the discharge tube / l C'-,
Calculate the amount using the formula and start evacuation and replenishment.

酸素濃度が(a)点以下になれば排気・補充を中止し酸
素濃度が(c)点に達するまで流i調整弁(9)および
tU弁(11)を閉じて封じ切り動作を行うよってする
。(C)点に達した時点で流量調整弁(9)、電磁弁(
11)が所定時間開かれ酸素濃度が(a)点に戻される
。以上のような動作がレーザ発搗中繰り返されることに
なる。
When the oxygen concentration falls below point (a), exhaust/replenishment is stopped and the flow i adjustment valve (9) and tU valve (11) are closed to perform a sealing operation until the oxygen concentration reaches point (c). . When point (C) is reached, the flow rate adjustment valve (9), solenoid valve (
11) is opened for a predetermined time and the oxygen concentration is returned to point (a). The above operations are repeated during laser firing.

〔発明の効果〕〔Effect of the invention〕

レーザ発振中の放電管内におけるガスレーザ媒質の酸素
濃度を常時検出するようにしているので、ガスレーザ媒
質の微妙な変化や突発的な変化【対してもそれら変化を
是正する制御がなされるようにしたので、安定したレー
ザ発振が行えレーザ出力の安定に伴う発振装置自体の信
頼性を向とすることができた。また、ガスレーザ媒質も
定量的な検出に基すいて消費されるようになったので。
Since the oxygen concentration of the gas laser medium in the discharge tube during laser oscillation is constantly detected, control is implemented to correct subtle or sudden changes in the gas laser medium. As a result, stable laser oscillation can be performed, and the reliability of the oscillation device itself can be improved due to the stability of the laser output. In addition, gas laser media have also become consumed based on quantitative detection.

過剰にガスレーザ媒質を使用する無駄を省くことができ
るようになった。
It is now possible to eliminate the waste of using excessive gas laser media.

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

第1図は本発明の一実施例を示す構成図、第2図は酸素
濃度とアーク発生率の関係を示す図、第3図は放電回数
による酸素濃度の増加を示す図である。 (1)・・・放電管      (4)・・・電源部代
理人 弁理士  則 近 倉 缶 周     竹 花 喜久男 電狛ヤ 第 1 図
FIG. 1 is a block diagram showing an embodiment of the present invention, FIG. 2 is a diagram showing the relationship between oxygen concentration and arc generation rate, and FIG. 3 is a diagram showing the increase in oxygen concentration depending on the number of discharges. (1)...Discharge tube (4)...Power supply department representative Patent attorney Nori Chikura Kanshu Takehana Kikuo Denkomaya Figure 1

Claims (1)

【特許請求の範囲】[Claims] 所定の圧力で封入されたガスレーザ媒質を励起する放電
管と、この放電管に放電用の電力を供給する電源部と、
上記放電管内でレーザ発振に使用されたガスレーザ媒質
の一部を排気して同量の未使用ガスレーザ媒質を補充す
るガス交換手段と、上記放電管内に設けられた酸素濃度
検出器と、この酸素濃度検出器からの酸素濃度の検出信
号を入力し上記ガス交換手段に対し上記検出信号が基準
値の範囲外のとき動作させ基準値の範囲内のとき停止さ
せる制御装置とを備えたことを特徴とするガスレーザ発
振装置。
a discharge tube that excites a sealed gas laser medium at a predetermined pressure; a power supply unit that supplies electric power for discharge to the discharge tube;
a gas exchange means for exhausting a part of the gas laser medium used for laser oscillation in the discharge tube and replenishing the same amount of unused gas laser medium; an oxygen concentration detector provided in the discharge tube; It is characterized by comprising a control device which inputs a detection signal of oxygen concentration from a detector and causes the gas exchange means to operate when the detection signal is outside the range of the reference value and stop when the detection signal is within the range of the reference value. Gas laser oscillation device.
JP10856186A 1986-05-14 1986-05-14 Gas laser oscillator Pending JPS62265785A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP10856186A JPS62265785A (en) 1986-05-14 1986-05-14 Gas laser oscillator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP10856186A JPS62265785A (en) 1986-05-14 1986-05-14 Gas laser oscillator

Publications (1)

Publication Number Publication Date
JPS62265785A true JPS62265785A (en) 1987-11-18

Family

ID=14487947

Family Applications (1)

Application Number Title Priority Date Filing Date
JP10856186A Pending JPS62265785A (en) 1986-05-14 1986-05-14 Gas laser oscillator

Country Status (1)

Country Link
JP (1) JPS62265785A (en)

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