JPS60198878A - Gas laser oscillator - Google Patents

Gas laser oscillator

Info

Publication number
JPS60198878A
JPS60198878A JP5582184A JP5582184A JPS60198878A JP S60198878 A JPS60198878 A JP S60198878A JP 5582184 A JP5582184 A JP 5582184A JP 5582184 A JP5582184 A JP 5582184A JP S60198878 A JPS60198878 A JP S60198878A
Authority
JP
Japan
Prior art keywords
duct
sealed chamber
medium gas
gas
laser
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
Application number
JP5582184A
Other languages
Japanese (ja)
Other versions
JPS641950B2 (en
Inventor
Yoshihide Kanehara
好秀 金原
Shuichi Noda
野田 修一
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi 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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP5582184A priority Critical patent/JPS60198878A/en
Publication of JPS60198878A publication Critical patent/JPS60198878A/en
Publication of JPS641950B2 publication Critical patent/JPS641950B2/ja
Granted 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

Abstract

PURPOSE:To prevent it for laser medium gas to stagnate by a method wherein a sealed chamber including an internal space of a cylindrical part is provided and this sealed chamber is provided with an air blower, and at the same time, the sealed chamber is provided with an aperture consisting of a pipe-shaped duct. CONSTITUTION:A container 1 is provided with a sealing duct 25 and a sealed chamber has been formed of the container 1, the sealing duct 25, a bellows 21 and so forth, and at the same time, a cylindrical internal space part has been provided in this sealed chamber. A pipe-shaped duct 24 is provided in parallel with the axial direction of a laser beam 8 in the sealed chamber and an aperture consisting of the duct 24 has been provided. The duct 24 has been arranged in such a way that the laser beam 8 penetrates the interior of the duct 24. Furthermore, the duct 25 has been provided with an air blower 26, which is used for sending laser medium gas within the container 1 in the duct 24. The laser medium gas 27 sent in by this air blower 26 is sent in the gap part between the bellows 21 and the duct 24, furthermore passes through the gap part between a partially transmitting mirror 7 and the duct 24 and pushes out laser medium gas replete in the interior of the duct 24 in the direction of the electrode of this element.

Description

【発明の詳細な説明】 〔発明の技術分野〕 この発明はガスレーザ発振器のレーザ発振特性の改良に
関するものである。 ゛ 〔従来技術〕 従来この種の整置として第1図に示すものがあった。
DETAILED DESCRIPTION OF THE INVENTION [Technical Field of the Invention] The present invention relates to improving the laser oscillation characteristics of a gas laser oscillator.゛[Prior Art] This type of arrangement has conventionally been shown in Fig. 1.

図にかいて、容器(1)内にレーザ媒質ガス(2)を封
入し電線(8A) (8B)間にに源(4)から電圧を
印加すると、放電(5)が発生し、レーザ媒質ガス(2
)を励起し、この放電(5)を挾んで対向して蕗かれた
全反射鏡(6)と部分透過鏡(7)の間でレーザ発振が
起こり、レーザ光(8)を出力する。また放電(5)に
より高温になったレーザ媒質ガス(2)は熱交換器(9
)を通ることにより冷却され、再度送風機a1によりi
[(8A)(BB)間に送られ循環される。インバー(
2)は容器(1)が仮にた゛わんでも影智されない様形
成されている。光学基板a隷はインバーαaにより保持
され、平行状態を温度変化等があっても安定に保つよう
になっている。また光学基板α4α0にはマイクロメー
タaυ〜(19が取付けられておシ、さらにこのマイク
ロメータ■〜QIニ光学基板Q1)@に接してhる。
As shown in the figure, when a laser medium gas (2) is sealed in a container (1) and a voltage is applied from a source (4) between electric wires (8A) and (8B), a discharge (5) is generated and the laser medium gas Gas (2
) is excited, and laser oscillation occurs between the total reflection mirror (6) and the partial transmission mirror (7), which are opposed to each other with this discharge (5) in between, and output a laser beam (8). In addition, the laser medium gas (2), which has become high temperature due to the discharge (5), is transferred to the heat exchanger (9).
), and is cooled again by blower a1.
[It is sent and circulated between (8A) and (BB). Invar (
2) is formed so that even if the container (1) bends, it will not be noticed. The optical substrate a is held by an inverter αa to keep the parallel state stable even if there is a temperature change. Further, micrometers aυ~ (19) are attached to the optical substrate α4α0, and the micrometers ~QI are in contact with the optical substrate Q1)@.

また光学基板04)θQには全反射鏡(6)または部分
透過鏡(7)が取付けられマイクロメータαd−(1(
eの表示される数値によって光学基板α4αOを調整す
ることにより角度調整ができるようになって匹る。ベロ
ーズB)(2ηは光学基板(14Jαυが自由に卯1〈
ことができるよう構成されており、V−ザ媒質ガス(2
)と大気とをしゃ断する機能もしている。
In addition, a total reflection mirror (6) or a partial transmission mirror (7) is attached to the optical board 04) θQ, and a micrometer αd-(1(
The angle can be adjusted by adjusting the optical substrate α4αO according to the displayed value of e. bellows B) (2η is the optical substrate (14Jαυ is freely
V-the medium gas (2
) and the atmosphere.

従来のガスレーザ発揚器は以上のように構成されている
ので、レーザ発振をするとベローズcqaυがi聞4犬
となっているためにレーザ媒質ガス(5)−が充満し、
さらにレーザ光を吸収することによシ温度が上昇し、さ
らに温度が高くなることにより吸収率が増加するという
現象が起こり、レーザ発振効率が下ってしまう。
Conventional gas laser generators are constructed as described above, so when the laser oscillates, the bellows cqaυ is filled with the laser medium gas (5)-, and
Furthermore, absorption of laser light causes a rise in temperature, and as the temperature rises further, a phenomenon occurs in which the absorption rate increases, resulting in a decrease in laser oscillation efficiency.

これを第3因におめて説明すると、(4)は放ボボ力に
対するV−ザ出力であり、放電π力を増加してもレーザ
出力が増加しなくなり、発振効率が低下するといった欠
点があった。
To explain this in terms of the third factor, (4) is the V-za output with respect to the discharge force, which has the disadvantage that even if the discharge π force is increased, the laser output does not increase and the oscillation efficiency decreases. there were.

〔発明の概要〕[Summary of the invention]

この発明は上記の工うな往来のものの欠点を除去するた
めになされたもので、ベローズの内側のレーザ媒質ガス
を・滞留しないように送風機により流れを作る構成にす
ることに191発振効率の良めガスレーザ発掛器を得る
ことを目的としている。
This invention was made in order to eliminate the drawbacks of the conventional methods described above, and it is possible to improve the 191 oscillation efficiency by creating a flow using a blower to prevent the laser medium gas inside the bellows from stagnation. The aim is to obtain a gas laser generator.

〔発明の実施例〕[Embodiments of the invention]

以下この発明の一寅施例を第2図につbて説明する。 Hereinafter, one embodiment of the present invention will be explained with reference to FIG.

図において、第1図と同一符号は同一または相当部分を
示し、ベローズelDによシ形成されている筒状部の内
部空間部には、容器(1)にシールダクト(2)−、y
咽付けられて囲われ、密閉室が形成されてbる。この密
閉室のレーザ光の光軸方向にはアルミニウム材、樹脂材
などより成形されたパイプ状のダクト■が設けられ開口
されている。パイプ状のダク)I’241は上記密閉室
の光軸方向と同方向でかつV−ザ光が貯油ずるよう配設
されており、一端は部分透過鏡(7)ノ近傍1部に、池
@ld!li (8A) (8B>の近傍部まで伸びて
b7)、さらにダクト(財)の外側のV−ザ媒質ガス(
2)がもれないような構造にしたシールダクト(ハ)に
は、容器(1)内のレーザ媒質ガス(2)をダクト■内
に送9込むための送風機(イ)が取付けられている。そ
して送風機(イ)の吸込側にはエアフィルタ(2)が設
けられており、このエアフィMり(至)によって容器(
1)内に混入している塵埃を吸着し、全反射鏡(6)や
部分透過鏡(7)の表面への塵埃の付着。
In the figure, the same reference numerals as those in FIG.
It is sealed and enclosed, forming a closed room. A pipe-shaped duct (2) made of aluminum, resin, or the like is provided and opened in the optical axis direction of the laser beam in this sealed chamber. The pipe-shaped duct (I'241) is arranged in the same direction as the optical axis direction of the sealed chamber and so that the V-za light is stored therein, and one end is connected to a part near the partially transmitting mirror (7). @ld! li (8A) (extends to the vicinity of 8B> b7), further outside the duct (goods) V-the medium gas (
A blower (A) is attached to the seal duct (C), which has a structure to prevent 2) from leaking, to blow the laser medium gas (2) in the container (1) into the duct ■. . An air filter (2) is provided on the suction side of the blower (a), and this air filter (to) allows the container (
1) Adsorbs dust mixed in the mirror and prevents dust from adhering to the surface of the total reflection mirror (6) and the partial transmission mirror (7).

破損を防いでいる。このエアフィルタ翰にょうで清浄に
さノ1〜たレーザ媒質ガス@はベロー・ズQDとダクト
(ハ)との隙間部に送り連棟れ、さらに部分透過鏡(7
)と、ダクト(財)との隙間部を通ってダクト(ハ)内
の充満しているレーザ媒質ガス(2)を* # (8A
)(8B)の方向に押し出される。
Prevents damage. The laser medium gas cleaned by this air filter is sent to the gap between the bellows QD and the duct (C), and then further filtered through the partially transmitting mirror (7).
) and the duct (goods) through the gap between the laser medium gas (2) filling the duct (c) * # (8A
) (8B).

このようにして、第8図の放電電力に対するレーザ出力
(至)に示す如く、レーザ媒質ガス(2)の吸収による
影響がなく、放電π力に対して直線的にレーザ出力が増
加するため、放uカが高くな9レーザ出力も同様に高く
なることができる。すなわち、発振効率が良くなるとい
うことである。しかるにレーザ媒質ガス(2)によるレ
ーザ光(8)の吸収率は低下し、よってレーザ出力の不
安定さけなくなる。
In this way, as shown in the laser output (to) versus discharge power in Fig. 8, there is no effect of absorption of the laser medium gas (2), and the laser output increases linearly with respect to the discharge π power. 9 laser power with higher emissivity can be increased as well. In other words, the oscillation efficiency is improved. However, the absorption rate of the laser beam (8) by the laser medium gas (2) decreases, thereby preventing instability of the laser output.

なおダクト−〇長さは、ダクト(2)内をレーザ媒質ガ
ス(2)が流通するとき加速されるので、ある程度の長
さを必要とし極端に短ければ流通の力が刊〈効果が少な
い、なお上記実施例ではダクト−の材質はアルミニウム
材、樹脂材などより成るパイプ形状のものを用いたが、
レーザ媒質ガス(2)や熱などの影響を受けない材質の
ものであれは用^ても良い。
Note that the length of the duct is accelerated when the laser medium gas (2) flows through the duct (2), so a certain length is required, and if it is extremely short, the force of the flow will be less effective. In the above embodiment, the duct was made of a pipe-shaped material made of aluminum, resin, etc.
Any material that is not affected by the laser medium gas (2) or heat may be used.

また送風機(LOによって1/−ザ媒質ガス(2)が1
盾環されるが、さらに送風機〜によってダクト(2)内
にレーザ媒質ガス(2)が流通されるので、これらのし
−ザ媒質ガス(2)が容器(1)内で互いに干渉して滞
留することがなくなる。
Also, the blower (by LO the medium gas (2) is 1/- the medium gas (2) is 1
However, since the laser medium gas (2) is further distributed in the duct (2) by the blower, these laser medium gases (2) interfere with each other and stagnate in the container (1). There's nothing left to do.

さらに上記実施例では、部分透過鏡(7)側にダクト(
財)と送風11!(ホ)を設けた場合にりhで説明した
が。
Furthermore, in the above embodiment, a duct (
Goods) and ventilation 11! When (e) is provided, it was explained in h.

全反射鏡(6) fillに同様の構造としてもよく、
また部分透過鏡(7)側!=−工び全反射鏡(6)側の
双方に設けてもよく、上記実施例と同様の効果が得られ
る。
A similar structure may be used for the total reflection mirror (6) fill.
Also on the partially transparent mirror (7) side! =- It may be provided on both sides of the total reflection mirror (6), and the same effect as in the above embodiment can be obtained.

また上記実施例では、送風接圀によりレーザ媒質ガス(
2)ヲダクト(ハ)内に速υ込む場合について説明した
が、ダクト(財)外に排出するようにしてもよ(、上記
実施例と同様の効果が得られる。
Furthermore, in the above embodiment, the laser medium gas (
2) Although the case has been described in which the water is quickly introduced into the duct (c), it may also be discharged outside the duct (the same effect as in the above embodiment can be obtained).

〔発明の効果〕〔Effect of the invention〕

以上のように、この発明によれば筒4ノ’部の内部空間
を含む°、ぢ閉室を設け、この密閉室にレーザ媒質ガス
を圧入または排出する逆風(至)・をが1えるとともに
パイプ状のダクトから吠る開口部を上記密閉室に設けた
ので、レーザ媒質ガスが滞留せずレーザ出力が安定しく
?!b効率の高いガスレーザ発振器を得ることができる
効果がある。
As described above, according to the present invention, a closed chamber including the internal space of the 4th part of the cylinder is provided, and a back wind for pressurizing or discharging the laser medium gas is provided in this closed chamber, and a pipe is also provided. Since an opening from the shaped duct is provided in the sealed chamber, the laser medium gas does not stagnate and the laser output is stabilized. ! (b) It is possible to obtain a gas laser oscillator with high efficiency.

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

第1図は従来のガスレーザ発振器を示す概略図。 第2図はこの発明の一実施例によるガスレーザ発振器の
部分拡大断面図である。第8図は動作を説明するための
特性図である。 図において同一符号は同一または相当部分を示し、(1
)は容器、(2)(至)に)翰はレーザ媒質ガス、(5
)は放電、(6)は全反射鏡、(7)は部分透過鏡、(
8)はレーザ光、(9)は熱交換器、(10@は逆風機
、(イ)Qηはベローズ、(ハ)はダクト、@はエアフ
ィルタである。 代−人 大岩増雄 第3図 放1電力
FIG. 1 is a schematic diagram showing a conventional gas laser oscillator. FIG. 2 is a partially enlarged sectional view of a gas laser oscillator according to an embodiment of the present invention. FIG. 8 is a characteristic diagram for explaining the operation. In the figures, the same reference numerals indicate the same or corresponding parts, (1
) is the container, (2) (to)) is the laser medium gas, (5
) is a discharge, (6) is a total reflection mirror, (7) is a partial transmission mirror, (
8) is a laser beam, (9) is a heat exchanger, (10@ is a headwind fan, (a) Qη is a bellows, (c) is a duct, and @ is an air filter. 1 electric power

Claims (4)

【特許請求の範囲】[Claims] (1) レーザ媒質ガスを満たした容器と、この容器内
に対向配設された電極と、この醒極間の放電により励起
されて発生するレーザ光の光軸上の双方に、容器に接続
され端面に全反射鏡を有する第1の筒状部と、MA面に
部分透過鏡を有する第2の筒状部とケ備えたガスレーザ
発振器において、一方の上記筒状部の内部空間を含む密
閉室を設け、この密閉室にV−ザ媒質ガスを圧入または
排出する送風機を備えるとともに、上記レーザ光の光軸
方向にレーザ光が貫通するパイプ状ダクトから成る開口
部?上記密閉室の上記R5[に対向した側に備えたこと
を特徴とするガスレーザ発振器。
(1) A container filled with a laser medium gas, electrodes arranged facing each other in this container, and electrodes connected to the container both on the optical axis of the laser beam excited and generated by the discharge between the heating electrodes. In a gas laser oscillator comprising a first cylindrical part having a total reflection mirror on an end face and a second cylindrical part having a partially transmitting mirror on an MA surface, a sealed chamber including an internal space of one of the cylindrical parts. The sealed chamber is provided with a blower for pressurizing or discharging the V-za medium gas, and an opening consisting of a pipe-shaped duct through which the laser beam passes in the optical axis direction of the laser beam. A gas laser oscillator, characterized in that the gas laser oscillator is provided on the side opposite to the R5 of the sealed chamber.
(2)パイプ状ダクトは筒状部まで挿入されて成ること
を特徴とする特許請求の範囲第1項記載のガスレーザ発
振器。
(2) The gas laser oscillator according to claim 1, wherein the pipe-like duct is inserted up to the cylindrical portion.
(3)パイプ状ダクトはアルミニウム材より成ることを
特徴とする特許請求の範囲第1項寸たけ第2項記載のガ
スレーザ発振器。
(3) The gas laser oscillator according to claim 1 and claim 2, wherein the pipe-shaped duct is made of aluminum.
(4)送風機はレーザ媒質ガスのフィルタを有するもの
であることを特徴とする特許請求の範囲第1項または第
2項または第8項記載のガスレーザ発振器。
(4) The gas laser oscillator according to claim 1, 2, or 8, wherein the blower has a filter for the laser medium gas.
JP5582184A 1984-03-23 1984-03-23 Gas laser oscillator Granted JPS60198878A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5582184A JPS60198878A (en) 1984-03-23 1984-03-23 Gas laser oscillator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5582184A JPS60198878A (en) 1984-03-23 1984-03-23 Gas laser oscillator

Publications (2)

Publication Number Publication Date
JPS60198878A true JPS60198878A (en) 1985-10-08
JPS641950B2 JPS641950B2 (en) 1989-01-13

Family

ID=13009611

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5582184A Granted JPS60198878A (en) 1984-03-23 1984-03-23 Gas laser oscillator

Country Status (1)

Country Link
JP (1) JPS60198878A (en)

Also Published As

Publication number Publication date
JPS641950B2 (en) 1989-01-13

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