JPH05121797A - Gas laser oscillation device - Google Patents

Gas laser oscillation device

Info

Publication number
JPH05121797A
JPH05121797A JP28275591A JP28275591A JPH05121797A JP H05121797 A JPH05121797 A JP H05121797A JP 28275591 A JP28275591 A JP 28275591A JP 28275591 A JP28275591 A JP 28275591A JP H05121797 A JPH05121797 A JP H05121797A
Authority
JP
Japan
Prior art keywords
mirror
side wall
holding member
optical axis
airtight container
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
JP28275591A
Other languages
Japanese (ja)
Inventor
Noboru Okamoto
昇 岡本
Koji Kakizaki
弘司 柿崎
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 JP28275591A priority Critical patent/JPH05121797A/en
Publication of JPH05121797A publication Critical patent/JPH05121797A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To enable a gas laser oscillation device to recover its output without breaking the airtightness of an airtight chamber due to the dismount of a mirror by a method wherein a hold/drive mechanism which moves a holding member in parallel with the side wall of the airtight chamber is provided. CONSTITUTION:When a gas laser oscillation device is lessened in output due to the contamination of a mirror 28, a pressing nut 36 screwed to the thread 35a of four adjustment rods 35 is loosened, and then an adjustment nut 37 is screwed into the adjustment rod 35. By this setup, the holding member 27 is displaced in a direction (shown by an arrow a) so as to approach the side wall 21a of the airtight chamber 21 compressing a bellows 25 as it resists the restoring force of the bellows 25. The holding member 27 moves in the widthwise direction of the side wall 21a or a direction (an arrow b) vertical to the optical axis O1 of laser rays L in parallel with the side wall 21a. By this setup, the mirror 28 is made to move in the widthwise direction to enable its one end in the widthwise direction to get out of the optical axis O1 of laser rays L, and the other new part of the mirror 28 or an uncontaminated part of the mirror 28 where no discharge product is attached is located on the optical axis O1 of laser rays L.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】この発明は光共振器を形成する出
力ミラ−と高反射ミラ−とがガスレ−ザ媒質が充填され
る気密容器と一体的に設けられる内部鏡型のガスレ−ザ
発振装置に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an internal mirror type gas laser oscillation in which an output mirror forming an optical resonator and a highly reflective mirror are integrally provided with an airtight container filled with a gas laser medium. Regarding the device.

【0002】[0002]

【従来の技術】F2 レ−ザ、エキシマレ−ザあるいはT
EACO2 レ−ザなどのようにガスレ−ザ媒質を大気圧
よりも高い圧力で気密容器内に充填して使用するガスレ
−ザ発振装置においては、光共振器を気密容器と一体的
に設ける、いわゆる内部鏡型としたものがある。
2. Description of the Related Art F 2 laser, excimer laser or T
In a gas laser oscillating device such as an EACO 2 laser which is filled with a gas laser medium at a pressure higher than atmospheric pressure and used, an optical resonator is provided integrally with the airtight container. There is a so-called internal mirror type.

【0003】図6と図7は従来の内部鏡型のガスレ−ザ
発振装置を示す。すなわち、図中1は内部にガスレ−ザ
媒質が充填された気密容器である。この気密容器1内に
は一対の主電極2が所定間隔で離間対向して配設されて
いる。これら主電極2は高圧電源3にそれぞれ接続され
ている。そして、これら主電極2に高電圧を印加して放
電を発生させれば、その放電によって上記ガスレ−ザ媒
質が励起されてレ−ザ光Lが発生する。
6 and 7 show a conventional internal mirror type gas laser oscillator. That is, reference numeral 1 in the figure is an airtight container having a gas laser medium filled therein. A pair of main electrodes 2 are arranged in the airtight container 1 so as to face each other at a predetermined interval. These main electrodes 2 are connected to a high voltage power source 3, respectively. When a high voltage is applied to the main electrodes 2 to generate a discharge, the gas laser medium is excited by the discharge to generate laser light L.

【0004】上記気密器密1のレ−ザ光Lの光軸方向両
端側壁にはそれぞれ第1の透光部4が形成されている。
この第1の透光部4と対応する上記側壁の外面にはベロ
−ズ5の軸方向一端が気密に取着されている。このベロ
−ズ5の他端は板状の保持部材6の一側面に気密に接合
されている。この保持部材6には図7に示すように第2
の透光部7が形成されている。この第2の透光部7と対
応する上記保持部材6の外面には光共振器を形成するミ
ラ−8が固定フランジ9によって気密に保持されてい
る。
A first light transmitting portion 4 is formed on each side wall of the laser light L of the airtight device 1 in the direction of the optical axis.
An axial end of a bellows 5 is hermetically attached to the outer surface of the side wall corresponding to the first light transmitting portion 4. The other end of the bellows 5 is airtightly joined to one side surface of the plate-shaped holding member 6. As shown in FIG. 7, the holding member 6 has a second
The transparent portion 7 is formed. A mirror 8 forming an optical resonator is hermetically held by a fixing flange 9 on the outer surface of the holding member 6 corresponding to the second light transmitting portion 7.

【0005】上記保持部材6の四隅部にはそれぞれねじ
ロッド11が螺合されている。このねじロッド11の一
端にはボ−ル部12が設けられ、このボ−ル部12は上
記側壁の外面に設けられた支持部13に回転自在に支持
されている。上記ねじロッド11の他端には摘み14が
設けられ、この摘み14によってねじロッド11を回転
させることで上記保持部材6に保持されたミラ−8の傾
きを調整できるようになっている。
Screw rods 11 are screwed into the four corners of the holding member 6, respectively. A ball portion 12 is provided at one end of the screw rod 11, and the ball portion 12 is rotatably supported by a support portion 13 provided on the outer surface of the side wall. A knob 14 is provided at the other end of the screw rod 11, and the tilt of the mirror 8 held by the holding member 6 can be adjusted by rotating the screw rod 11 by the knob 14.

【0006】ところで、このような構成のガスレ−ザ発
振装置においては、一対の主電極2間で放電が繰り返し
て点弧されることでこれら主電極2間の放電空間部に多
量の放電生成物が発生することが避けられない。この放
電生成物は放電時の衝撃波で伝播したり、ガスレ−ザ媒
質に混入しレ−ザ光Lによって化学反応を起こすなどし
て上記ミラ−8の内面に付着する。
By the way, in the gas laser oscillator having such a structure, a large amount of discharge products are generated in the discharge space between the main electrodes 2 because the discharge is repeatedly ignited between the pair of main electrodes 2. Is inevitable. This discharge product is attached to the inner surface of the mirror 8 by propagating by a shock wave at the time of discharge, mixing in the gas laser medium and causing a chemical reaction by the laser light L.

【0007】そのため、上記ミラ−8のレ−ザ光Lが当
たる部分は黒く汚れ、その汚れが種になって加速度的に
汚れが進から、レ−ザ光Lの出力低下や汚れがレ−ザ光
Lの熱エネルギを吸収し、ミラ−8を損傷させるなどの
ことがある。
For this reason, the portion of the mirror 8 which is exposed to the laser light L is smeared in black, and the dirt becomes a seed to accelerate the dirt, resulting in a decrease in the output of the laser light L and dirt. The heat energy of the light L may be absorbed and the mirror 8 may be damaged.

【0008】上記ミラ−8の汚れを除去するには、ミラ
−8を保持部材6から外して清掃しなければならないか
ら、気密容器1の気密状態が壊される。そのため、ミラ
−8を清掃する度に気密容器1に対して排気やガスレ−
ザ媒質の入れ替えなどを行わなければならないから、レ
−ザ発振を再開させるのに時間が掛かるということがあ
る。
In order to remove the stains on the mirror 8, the mirror 8 must be removed from the holding member 6 and cleaned, so that the airtight state of the airtight container 1 is destroyed. Therefore, every time the mirror 8 is cleaned, the airtight container 1 is evacuated and gas is discharged.
Since it is necessary to replace the laser medium, it may take time to restart the laser oscillation.

【0009】[0009]

【発明が解決しようとする課題】このように、従来は光
共振器を形成するミラ−が汚れると、このミラ−を取り
外して清掃したり、交換しなければならなかったので、
気密容器の気密状態が壊されるため、レ−ザ発振を再開
させるのに多くの手間と時間がかかるということがあっ
た。
As described above, conventionally, when the mirror forming the optical resonator becomes dirty, the mirror had to be removed for cleaning or replacement.
Since the airtight state of the airtight container is destroyed, it takes a lot of time and labor to restart the laser oscillation.

【0010】この発明は上記事情にもとづきなされたも
ので、その目的とするところは、ミラ−が汚れて出力が
低下したときに、そのミラ−を気密容器から取り外すこ
となく出力を回復させることができるようにしたをガス
レ−ザ発振装置を提供することにある。
The present invention has been made in view of the above circumstances, and an object thereof is to recover the output without removing the mirror from the airtight container when the mirror becomes dirty and the output decreases. Another object of the present invention is to provide a gas laser oscillating device.

【0011】[0011]

【課題を解決するための手段】上記課題を解決するため
にこの発明は、ガスレ−ザ媒質が充填される気密容器
と、この気密容器内に対向して配設されこれらの間で発
生する放電で上記ガスレ−ザ媒質を励起する一対の主電
極と、上記気密容器の上記レ−ザ光の光軸方向に対応す
る両端側壁に形成された透光部と、この透光部と対向す
る上記側壁の外面側に配設されているとともに光共振器
を形成するミラ−を保持した保持部材と、一端を上記側
壁の外面の上記透光部の周囲に接合させ他端を上記保持
部材の上記ミラ−の周囲に接合させるとともに軸線を上
記レ−ザ光の光軸に対して所定角度傾斜させて設けられ
たベロ−ズと、このベロ−ズをその軸線方向に圧縮し上
記保持部材を上記側壁の外面に対して接近する方向と上
記光軸と交差する方向とに移動させるとともに所定の移
動位置を越えさせない保持駆動機構とを具備したことを
特徴とする。
SUMMARY OF THE INVENTION In order to solve the above-mentioned problems, the present invention relates to an airtight container filled with a gas laser medium, and an electric discharge generated between the airtight container and facing each other. A pair of main electrodes for exciting the gas laser medium, a light transmitting portion formed on both side walls of the airtight container corresponding to the optical axis direction of the laser light, and the light transmitting portion facing the light transmitting portion. A holding member that is disposed on the outer surface side of the side wall and holds a mirror that forms an optical resonator, and one end of the holding member is joined to the outer surface of the side wall around the transparent portion, and the other end of the holding member A bellows, which is joined to the periphery of the mirror and has its axis inclined at a predetermined angle with respect to the optical axis of the laser beam, and the bellows is compressed in the axial direction to hold the holding member as described above. A direction that approaches the outer surface of the side wall and intersects the optical axis Characterized by comprising a holding drive mechanism not to exceed the predetermined movement position is moved to and.

【0012】[0012]

【作用】上記構成によれば、ミラ−の一部が汚れたなら
ば、保持部材を保持駆動機構によって気密容器の側壁に
対して平行移動させることで、上記ミラ−の汚れていな
い部分をレ−ザ光の光軸上に位置させることができる。
According to the above construction, when a part of the mirror is contaminated, the holding member is moved in parallel with the side wall of the airtight container by the holding drive mechanism, so that the uncleaned part of the mirror is removed. -It can be located on the optical axis of the light.

【0013】[0013]

【実施例】以下、この発明を図面を参照して説明する。DESCRIPTION OF THE PREFERRED EMBODIMENTS The present invention will be described below with reference to the drawings.

【0014】図1乃至図4はこの発明の第1の実施例を
示し、図4において21は内部にガスレ−ザ媒質が大気
圧よりも高い圧力で封入された気密容器である。この気
密容器21の内部には一対の主電極22が離間対向して
配設されている。これら主電極22の一方は高圧電源2
3のプラス側に接続され、他方はマイナス側に接続され
ている。これら一対の主電極22に高電圧が印加される
と、これらの間に上記ガスレ−ザ媒質を励起する主放電
が点弧され、レ−ザ光Lが発生するようになっている。
1 to 4 show a first embodiment of the present invention. In FIG. 4, reference numeral 21 is an airtight container in which a gas laser medium is enclosed at a pressure higher than atmospheric pressure. Inside the airtight container 21, a pair of main electrodes 22 are arranged facing each other with a space therebetween. One of these main electrodes 22 is a high voltage power source 2
3 is connected to the plus side, and the other is connected to the minus side. When a high voltage is applied to the pair of main electrodes 22, the main discharge that excites the gas laser medium is ignited between them, and the laser light L is generated.

【0015】上記気密容器21の上記レ−ザ光Lの光軸
1 方向に沿う一端側と他端側との側壁21aにはそれ
ぞれ開孔からなる第1の透光部24が形成されている。
上記側壁21a外面の上記第1の透光部24の周囲に対
応する部分には、図1に示すように軸線O2 を上記レ−
ザ光Lの光軸O1 に対して角度θで傾斜させて金属製の
ベロ−ズ25の一方のフランジ25aが気密に接合固定
されている。このベロ−ズ25の他方のフランジ25b
は第2の透光部26が形成された矩形板状の保持部材2
7の一側面の上記第2の透孔部26の周囲に対応する部
分に接合固定されている。つまり、このベロ−ズ25
は、蛇腹状の本体部25cの両端に設けられた一対の上
記フランジ部25a、25bが上記本体部25cの軸線
2 に対して予め角度θで同方向に傾斜して設けられて
いる。
The side walls 21a of the airtight container 21 on one end side and the other end side along the optical axis O.sub.1 direction of the laser light L are provided with first light transmitting portions 24 each having an opening. There is.
As shown in FIG. 1, the axis O 2 is attached to the portion of the outer surface of the side wall 21a corresponding to the periphery of the first light transmitting portion 24.
One flange 25a of the metal bellows 25 is hermetically bonded and fixed to the optical axis O 1 of the light L at an angle θ. The other flange 25b of this bellows 25
Is a rectangular plate-shaped holding member 2 on which the second light transmitting portion 26 is formed.
7 is joined and fixed to a portion of one side surface of the No. 7 corresponding to the periphery of the second through hole 26. In other words, this bellows 25
Has a pair of flanges 25a, 25b provided at both ends of a bellows-shaped main body 25c, which are inclined in advance in the same direction at an angle θ with respect to the axis O 2 of the main body 25c.

【0016】上記ベロ−ズ25の内径寸法は上記第1、
第2の透光部24、26の内径寸法に比べて十分に大径
に形成され、このベロ−ズ25の内部空間を介して上記
一対の透光部24、26が連通している。
The inner diameter of the bellows 25 has the above-mentioned first and second dimensions.
The diameter of the second light transmitting portions 24 and 26 is sufficiently larger than the inner diameter of the second light transmitting portions 24 and 26, and the pair of light transmitting portions 24 and 26 communicate with each other through the inner space of the bellows 25.

【0017】上記保持部材27の他側面には上記第2の
透光部26を閉塞する状態でミラ−28の一方の面の周
辺部が第1のOリング29を介して接合されている。こ
のミラ−28の他方の面の周辺部には第2のOリング3
1を介して押えフランジ32が接合されている。この押
えフランジ32は上記保持部材27にねじ33によって
取付け固定されている。上記気密容器21の光軸方向一
端側と他端側に設けられた一対のミラ−28(一方が高
反射ミラ−で、他方が部分反射ミラ−である。)で光共
振器を形成しており、この光共振器によって気密容器2
1内で発生したレ−ザ光Lを増幅するようになってい
る。
A peripheral portion of one surface of the mirror 28 is joined to the other side surface of the holding member 27 in a state of closing the second light transmitting portion 26 via a first O-ring 29. A second O-ring 3 is provided around the other surface of the mirror 28.
The presser flange 32 is joined via 1. The pressing flange 32 is attached and fixed to the holding member 27 with a screw 33. An optical resonator is formed by a pair of mirrors 28 (one is a highly reflective mirror and the other is a partially reflective mirror) provided on one end side and the other end side of the airtight container 21 in the optical axis direction. And this optical resonator is used to seal the airtight container 2
The laser light L generated within 1 is amplified.

【0018】上記保持部材27の四隅部には、図3に示
すように上記ベロ−ズ25の傾斜方向に沿って長い長孔
34が形成されている。各長孔34には調整ロッド35
のおねじ35aが形成された一端部が挿入されている。
このおねじ35aには保持部材27の一側面に接合する
押えナット36と、他側面に接合する調整ナット37と
が螺合されている。また、上記各調整ロッド35の他端
は気密容器21の側壁21aの外面に設けられた取付部
38に連結されている。
As shown in FIG. 3, elongated holes 34 are formed at the four corners of the holding member 27 along the direction of inclination of the bellows 25. Each long hole 34 has an adjustment rod 35.
One end portion where the male screw 35a is formed is inserted.
A holding nut 36 joined to one side surface of the holding member 27 and an adjustment nut 37 joined to the other side surface are screwed to the male screw 35a. The other end of each of the adjusting rods 35 is connected to a mounting portion 38 provided on the outer surface of the side wall 21 a of the airtight container 21.

【0019】上記構成のガスレ−ザ発振装置において、
最初はベロ−ズ25を最も伸長させ、かつ一対のミラ−
28が平行に対向するよう調整する。ベロ−ズ25を伸
長させた状態では、ミラ−28の幅方向一端側がレ−ザ
光Lの光軸O1 上に位置している。
In the gas laser oscillator having the above structure,
At first, the bellows 25 is extended the most and a pair of mirrors
28 so that they face each other in parallel. In the state where the bellows 25 is extended, one end in the width direction of the mirror 28 is located on the optical axis O 1 of the laser light L.

【0020】このような状態で高圧電源23を作動さ
せ、一対の主電極22間に高電圧を印加すれば、これら
主電極22間で発生する主放電によってガスレ−ザ媒質
が励起されてレ−ザ光Lが発生する。レ−ザ光Lは一対
のミラ−28間で反射を繰り返して増幅され、反射率の
低い一方のミラ−28から発振出力される。
When the high voltage power supply 23 is operated in such a state and a high voltage is applied between the pair of main electrodes 22, the gas laser medium is excited by the main discharge generated between the main electrodes 22 and laser. The light L is generated. The laser light L is repeatedly reflected and amplified between a pair of mirrors 28, and is oscillated and output from one mirror 28 having a low reflectance.

【0021】このようなレ−ザ発振を繰り返すと、ミラ
−28のレ−ザ光Lの光軸O1 上に位置する部分に放電
生成物が付着して汚損され、レ−ザ光Lの出力低下やミ
ラ−28の損傷を招く。
When such laser oscillation is repeated, the discharge products adhere to the portion of the mirror 28 located on the optical axis O 1 of the laser light L and are contaminated. The output is reduced and the mirror 28 is damaged.

【0022】そこで、ミラ−28が汚れて出力が低下し
た場合には、保持部材27を保持した4本の調整ロッド
35のおねじ35aに螺合された押えナット36を緩め
てから、調整ナット37をねじ込む。それによって、保
持部材27はベロ−ズ25を復元力に抗して圧縮させな
がら図1に矢印aで示す気密容器21の側壁21aに接
近する方向に変位する。
Therefore, when the mirror 28 becomes dirty and the output is reduced, the holding nut 36 screwed to the male screws 35a of the four adjusting rods 35 holding the holding member 27 is loosened, and then the adjusting nut. Screw in 37. As a result, the holding member 27 is displaced in the direction approaching the side wall 21a of the airtight container 21 shown by the arrow a in FIG. 1 while compressing the bellows 25 against the restoring force.

【0023】また、上記ベロ−ズ25はその軸線O1
レ−ザ光Lの軸線O2 に対して角度θで傾けて設けられ
ているから、このベロ−ズ25を圧縮させることによっ
て保持部材27は矢印aで示す接近方向だけでなく、矢
印bで示す上記側壁21aの幅方向である、レ−ザ光L
の光軸O1 と直交する方向にも上記側壁21aに対して
平行に移動する。
Further, since the bellows 25 is provided so that its axis O 1 is inclined with respect to the axis O 2 of the laser light L at an angle θ, it is held by compressing the bellows 25. The member 27 is not only in the approach direction indicated by the arrow a, but also in the width direction of the side wall 21a indicated by the arrow b.
It also moves parallel to the side wall 21a in the direction orthogonal to the optical axis O 1 .

【0024】上記保持部材27が平行移動すれば、図2
に示すようにミラ−28も幅方向に移動し、その幅方向
一端側がレ−ザ光Lの光軸O1 上からずれ、レ−ザ光L
の光軸O1 上にはミラ−28の新たな部分、つまり、放
電生成物が付着していない清浄な部分が位置することに
なる。したがって、その状態で保持部材27を固定して
レ−ザ光Lを出力すれば、レ−ザ光Lは一対のミラ−2
7の放電生成物が付着していない部分で反射することに
なるから、出力の低下やミラ−27を損傷させるような
ことがない。
If the holding member 27 is moved in parallel, as shown in FIG.
As shown in FIG. 5, the mirror 28 also moves in the width direction, and one end side in the width direction is displaced from the optical axis O 1 of the laser light L, and the laser light L
A new portion of the mirror 28, that is, a clean portion on which the discharge products are not attached, is located on the optical axis O 1 of . Therefore, if the holding member 27 is fixed and the laser light L is output in that state, the laser light L will generate a pair of mirror lights L-2.
Since the discharge products of No. 7 are reflected at the portions where they are not attached, there is no reduction in output and no damage to the mirror 27.

【0025】すなわち、上記構成のガスレ−ザ装置によ
れば、ミラ−27が放電生成物で汚損されても、そのミ
ラ−27を気密容器21から取り外すことなく、出力の
回復を計ることができる。
That is, according to the gas laser device having the above-mentioned configuration, even if the mirror 27 is contaminated with discharge products, the output can be recovered without removing the mirror 27 from the airtight container 21. ..

【0026】図5はこの発明の第2の実施例を示す。こ
の実施例は気密容器21の側壁21a外面と、保持部部
材27の上記側壁21aと対向する一側面とにそれぞれ
テ−パ面41を有するスペ−サ42が設けられている。
これらスペ−サ42のテ−パ面41は、平行に離間対向
しているとともに、上記側壁21aに対して所定の角度
で傾斜している。また、各スペ−サ42には側壁21a
に形成された第1の透光部24および保持部材27に形
成された第2の透光部26に対応する連通孔42aが形
成されている。
FIG. 5 shows a second embodiment of the present invention. In this embodiment, a spacer 42 having a taper surface 41 is provided on the outer surface of the side wall 21a of the airtight container 21 and on one side surface of the holding member 27 facing the side wall 21a.
The taper surfaces 41 of these spacers 42 are parallel and spaced apart and face each other, and are inclined at a predetermined angle with respect to the side wall 21a. Further, each spacer 42 has a side wall 21a.
A communication hole 42a corresponding to the first light-transmitting portion 24 formed in and the second light-transmitting portion 26 formed in the holding member 27 is formed.

【0027】各スペ−サ42のテ−パ面41には、ベロ
−ズ43の蛇腹状の本体部43aの両端に設けられたフ
ランジ部43bが接合固定されている。このフランジ部
43bは、上記本体部43aの軸線に対してほぼ直角に
設けられている。
To the taper surface 41 of each spacer 42, flange portions 43b provided at both ends of a bellows-shaped main body portion 43a of the bellows 43 are joined and fixed. The flange portion 43b is provided substantially at right angles to the axis of the main body portion 43a.

【0028】このような構成によれば、ベロ−ズ43は
上記スペ−サ42のテ−パ面41の傾斜角度に応じてそ
の軸線をレ−ザ光Lの光軸O1 に対して傾斜させて設け
ることができるから、保持部材27を気密容器21の側
壁21aに接近する方向に移動させれば、この保持部材
27を上記側壁21aの幅方向に対して平行に移動させ
ることができる。つまり、スペ−サ42を用いること
で、本体部42aに対してフランジ部42bがほぼ直角
に設けられた通常のベロ−ズ43を用いることができ
る。
With this structure, the bevel 43 has its axis inclined with respect to the optical axis O 1 of the laser light L in accordance with the inclination angle of the taper surface 41 of the spacer 42. Since the holding member 27 can be provided in parallel with the side wall 21a of the airtight container 21, the holding member 27 can be moved parallel to the width direction of the side wall 21a. That is, by using the spacer 42, it is possible to use an ordinary bezel 43 in which the flange portion 42b is provided at a substantially right angle to the main body portion 42a.

【0029】[0029]

【発明の効果】以上述べたようにこの発明によれば、気
密容器の軸方向一端側と他端側とにそれぞれ設けられる
光共振器用のミラ−を保持するベロ−ズの軸線を、レ−
ザ光の光軸に対して所定の角度で傾斜させるようにし
た。
As described above, according to the present invention, the axis lines of the bellows for holding the mirrors for the optical resonators, which are respectively provided on the one end side and the other end side in the axial direction of the airtight container, are arranged in the radial direction.
The light is inclined at a predetermined angle with respect to the optical axis.

【0030】そのため、上記ミラ−のレ−ザ光の光軸上
に位置する部分が放電生成物によって汚れたならば、上
記ベロ−ズを圧縮すれば、上記ミラ−が平行移動し、放
電生成物が付着していない清浄な部分をレ−ザ光の光軸
上に位置させることができるから、ミラ−が汚れて出力
が低下する度に、ミラ−を取外して気密容器の気密状態
を壊すことなく出力の回復を計ることができる。
Therefore, if the portion of the mirror located on the optical axis of the laser light is contaminated by the discharge product, the bellows are compressed to move the mirror in parallel and generate the discharge. Since a clean part without any object can be located on the optical axis of the laser light, the mirror is removed and the airtight condition of the airtight container is destroyed every time the mirror becomes dirty and the output decreases. You can measure the output recovery without.

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

【図1】この発明の第1の実施例を示すミラ−の保持構
造の拡大断面図。
FIG. 1 is an enlarged cross-sectional view of a mirror holding structure showing a first embodiment of the present invention.

【図2】同じくベロ−ズを圧縮させた状態の拡大断面
図。
FIG. 2 is an enlarged sectional view showing a state in which the bellows is also compressed.

【図3】同じく気密容器の端面図。FIG. 3 is an end view of the airtight container.

【図4】同じく一部断面した気密容器の平面図。FIG. 4 is a plan view of the airtight container, which is also partially sectioned.

【図5】この発明の第2の実施例を示すミラ−の保持構
造の拡大断面図。
FIG. 5 is an enlarged cross-sectional view of a mirror holding structure showing a second embodiment of the present invention.

【図6】従来の気密容器の平面図。FIG. 6 is a plan view of a conventional airtight container.

【図7】同じくミラ−の保持構造の拡大断面図。FIG. 7 is an enlarged sectional view of the holding structure of the mirror.

【符号の説明】[Explanation of symbols]

21…気密容器、22…主電極、24…第1の透光部、
25…ベロ−ズ、27…保持部材、28…ミラ−、35
…調整ロッド(保持駆動機構)、36…押えナット(保
持駆動機構)、37…調整ナット(保持駆動機構)。
21 ... Airtight container, 22 ... Main electrode, 24 ... First light transmitting part,
25 ... Bellows, 27 ... Holding members, 28 ... Millers, 35
... adjusting rod (holding drive mechanism), 36 ... press nut (holding drive mechanism), 37 ... adjusting nut (holding drive mechanism).

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 ガスレ−ザ媒質が充填される気密容器
と、この気密容器内に対向して配設されこれらの間で発
生する放電で上記ガスレ−ザ媒質を励起する一対の主電
極と、上記気密容器の上記レ−ザ光の光軸方向に対応す
る両端側壁に形成された透光部と、この透光部と対向す
る上記側壁の外面側に配設されているとともに光共振器
を形成するミラ−を保持した保持部材と、一端を上記側
壁の外面の上記透光部の周囲に接合させ他端を上記保持
部材の上記ミラ−の周囲に接合させるとともに軸線を上
記レ−ザ光の光軸に対して所定角度傾斜させて設けられ
たベロ−ズと、このベロ−ズをその軸線方向に圧縮し上
記保持部材を上記側壁の外面に対して接近する方向と上
記光軸と交差する方向とに移動させるとともに所定の移
動位置を越えさせない保持駆動機構とを具備したことを
特徴とするガスレ−ザ発振装置。
1. An airtight container filled with a gas laser medium, and a pair of main electrodes which are arranged facing each other in the airtight container and excite the gas laser medium by an electric discharge generated therebetween. A light transmitting portion formed on both side walls of the airtight container corresponding to the optical axis direction of the laser light, and an optical resonator provided on the outer surface side of the side wall facing the light transmitting portion. A holding member holding a mirror to be formed, one end of which is joined to the outer surface of the side wall around the light-transmitting portion and the other end of which is joined to the surrounding of the mirror of the holding member, and an axis line is formed into the laser beam. And a direction in which the bevel is compressed in the axial direction to make the holding member approach the outer surface of the side wall and the optical axis intersects. Move in the same direction and do not exceed the specified movement position. A gas laser oscillator comprising a holding and driving mechanism.
JP28275591A 1991-10-29 1991-10-29 Gas laser oscillation device Pending JPH05121797A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP28275591A JPH05121797A (en) 1991-10-29 1991-10-29 Gas laser oscillation device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP28275591A JPH05121797A (en) 1991-10-29 1991-10-29 Gas laser oscillation device

Publications (1)

Publication Number Publication Date
JPH05121797A true JPH05121797A (en) 1993-05-18

Family

ID=17656643

Family Applications (1)

Application Number Title Priority Date Filing Date
JP28275591A Pending JPH05121797A (en) 1991-10-29 1991-10-29 Gas laser oscillation device

Country Status (1)

Country Link
JP (1) JPH05121797A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN116448718A (en) * 2023-04-19 2023-07-18 河北子曰机械设备有限公司 Cavity ring-down tuning unit and cavity ring-down spectroscopy device

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN116448718A (en) * 2023-04-19 2023-07-18 河北子曰机械设备有限公司 Cavity ring-down tuning unit and cavity ring-down spectroscopy device
CN116448718B (en) * 2023-04-19 2023-12-05 河北子曰机械设备有限公司 Cavity ring-down tuning unit and cavity ring-down spectroscopy device

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