JPH01272173A - Laser oscillating device - Google Patents

Laser oscillating device

Info

Publication number
JPH01272173A
JPH01272173A JP10104088A JP10104088A JPH01272173A JP H01272173 A JPH01272173 A JP H01272173A JP 10104088 A JP10104088 A JP 10104088A JP 10104088 A JP10104088 A JP 10104088A JP H01272173 A JPH01272173 A JP H01272173A
Authority
JP
Japan
Prior art keywords
dielectrics
metal electrodes
members
tubular dielectric
discharge
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
JP10104088A
Other languages
Japanese (ja)
Inventor
Tamio Takeda
武田 民雄
Shigeo Kusunoki
楠 成夫
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 JP10104088A priority Critical patent/JPH01272173A/en
Publication of JPH01272173A publication Critical patent/JPH01272173A/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 eliminate vibrations from the outside, marring of tubular dielectrics due to external forces, the generation of damages and the variety of discharge and to contrive the stabilization of output by a method wherein annular members consisting of elastic material are closely arranged between the tubular dielectrics and metal electrodes. CONSTITUTION:Annular members 22 and 23 all consist of an elastic material, which is superior in a high frequency resistance and a high temperature resistance and consist of fluorine or a silicone rubber or the like, for example, are formed into the configuration of an O-ring and are pressed to the outer faces of tubular dielectrics 21 by metal electrodes 24 and 25 making a pair in combination with the upper and lower ones. Laser gas is circulated in the inner sides of the dielectrics 21 and silent discharge 34 is performed through the dielectrics 21 between the electrodes 24 and 25 to induce the laser gas. The members 22 and 23 are put in a high-frequency electric field and keep coming into contact to the high-temperature dielectrics 21, but as the members 22 and 23 consist of the high frequency-resistant and high temperature-resistant material, vibrations from the outside and external forces are also absorbed by the elasticity of the members 22 and 23, marring due to the dielectrics and the generation of cracks and failures are prevented and each spaces between the dielectrics 21 and the electrodes 24 and 25 is filled with the members 22 and 23. Thereby, as the generation of spaces is avoided, the variation of the silent discharge 34 is eliminated.

Description

【発明の詳細な説明】 [発明の目的] (産業上の利用分野) 本発明はレーザガスの励起を無声放電によって行なうレ
ーザ発振装置に関する。
DETAILED DESCRIPTION OF THE INVENTION [Object of the Invention] (Industrial Application Field) The present invention relates to a laser oscillation device that excites laser gas by silent discharge.

(従来の技術) 一般にレーザ加工に供されるレーザ光線の発振装置とし
ては、C02レーザ発振装置などガスレーザ発振装置が
主流であり、そのレーザガスの励起は直流放電により行
なわれていた。ところが、直流放電では、金属電極がレ
ーザガス中に露出しているため、放電がアーク放電に移
行しやす(、放電に安定性を欠くとか、放電により金属
がレーザガスと反応してガスを汚染するとかいった欠点
を有していた。
(Prior Art) Generally, gas laser oscillation devices such as a C02 laser oscillation device are mainstream as laser beam oscillation devices used for laser processing, and the excitation of the laser gas is performed by direct current discharge. However, in direct current discharge, the metal electrode is exposed in the laser gas, so the discharge easily turns into an arc discharge (the discharge may lack stability, or the metal may react with the laser gas due to the discharge and contaminate the gas). It had some drawbacks.

このため、近年、上記直流放電の欠点を除去し且つ単位
電極長の放電入力を飛躍的に増大し得る放電方式として
、金属電極間に誘電体を介在させて行なう交流放電すな
わち無声放電をレーザガスの励起に応用することが考え
られている。
Therefore, in recent years, as a discharge method that can eliminate the above-mentioned drawbacks of DC discharge and dramatically increase the discharge input per unit electrode length, AC discharge, that is, silent discharge, which is performed by interposing a dielectric between metal electrodes, has been developed using laser gas. Application to excitation is being considered.

しかしてこの種の装置としては、例えば特開昭61−2
83184号公報に示されるものが知られており、これ
を第8図及び第9図に示す。
However, as this type of device, for example, JP-A-61-2
A device disclosed in Japanese Patent No. 83184 is known, and is shown in FIGS. 8 and 9.

すなわち、この装置においては、石英ガラス等で製造さ
れた断面円形の管状誘電体1の外側に、対を成す金属電
極2,3がそれぞれ密着配置され、放電電極管4が構成
されている。放電電極管4の両側には、この放電電極管
4の軸心がレーザ光軸と一致するように、全反射ミラー
5とレーザ取出し可能な反射ミラー6とが配置されてい
る。更に、放電電極管4にはガス循環体7がその両側で
接続されており、ガス循環体7の中央部には送風機8が
冷却器9.10と共に設けられている。そして金属電極
2.3には高電圧の高周波電源11が接続されている。
That is, in this device, a discharge electrode tube 4 is constructed by disposing a pair of metal electrodes 2 and 3 in close contact with each other on the outside of a tubular dielectric body 1 made of quartz glass or the like and having a circular cross section. A total reflection mirror 5 and a reflection mirror 6 from which the laser can be taken out are arranged on both sides of the discharge electrode tube 4 so that the axis of the discharge electrode tube 4 coincides with the laser optical axis. Furthermore, a gas circulation body 7 is connected to the discharge electrode tube 4 on both sides, and a blower 8 is provided in the center of the gas circulation body 7 together with a cooler 9.10. A high-voltage, high-frequency power source 11 is connected to the metal electrode 2.3.

このような構成で、ガス循環体7内に供給されたレーザ
媒質としてのガスすなわちレーザガスが、送風機8によ
りガス循環体7から管状誘電体1にかけ冷却器9,10
を通して循環され、その管状誘電体1の内側を流通され
る。そしてそのような状況で、金属電極2,3には電源
11から高周波の高電圧が印加され、それによって金属
電極2゜3間では管状誘電体1を介する無声放電12が
行なわれ、レーザガスの励起をする。これに伴い、ミラ
ー5,6間ではレーザ発振が起こり、ミラー6からレー
ザ光13が取出される。
With such a configuration, the gas as a laser medium supplied into the gas circulation body 7, that is, the laser gas, is passed from the gas circulation body 7 to the tubular dielectric body 1 by the blower 8 to the coolers 9, 10.
and is circulated through the tubular dielectric 1. In such a situation, a high frequency high voltage is applied from the power source 11 to the metal electrodes 2 and 3, and as a result, a silent discharge 12 is generated between the metal electrodes 2 and 3 through the tubular dielectric 1, and the laser gas is excited. do. Accordingly, laser oscillation occurs between mirrors 5 and 6, and laser light 13 is extracted from mirror 6.

(発明が解決しようとする課居) 上述のレーザ発振装置においては、管状誘電体1の外側
に金属電極2.3をそれぞれ密着して配置しているため
、例えば送風機8の運転や輸送中での外部からの振動、
外力があると、それが上記管状誘電体1と金属電極2.
3との間に直接影響し、石英ガラス等から成る管状誘電
体1に金属電極2,3による傷付きやクラック、更には
破損をきたすという問題点を有していた。又、石英ガラ
ス等から成る管状誘電体1は通常引抜き方式で製造され
るもので、機械加工で製造される金属電極2.3に比し
、外形のばらつきが大きく、従ってそれらを全面密着さ
せることは困難で、一部空間を生じることから、無声放
電12にもその空間を因としてばらつきを生じ、レーザ
出力が安定しないという問題点を有していた。
(Problem to be Solved by the Invention) In the laser oscillation device described above, since the metal electrodes 2 and 3 are arranged in close contact with each other on the outside of the tubular dielectric 1, for example, during operation of the blower 8 or during transportation, vibration from the outside,
When there is an external force, it causes the above-mentioned tubular dielectric body 1 and metal electrode 2.
3, causing scratches, cracks, and even damage to the tubular dielectric body 1 made of quartz glass or the like due to the metal electrodes 2 and 3. Further, the tubular dielectric body 1 made of quartz glass or the like is usually manufactured by a drawing method, and has a larger variation in external shape than the metal electrodes 2.3 manufactured by machining. It is difficult to do so, and since a certain space is created, the silent discharge 12 also varies due to the space, which poses a problem in that the laser output is unstable.

本発明は上述の事情に鑑みてなされたものであり、従っ
てその目的は、外部からの振動、外力による管状誘電体
の傷付きやクラック、破損の発生をなくシ、併せて無声
放電のばらつきをもなくして、レーザ出力の安定化を図
り得る優れたレーザ発振装置を提供するにある。
The present invention has been made in view of the above-mentioned circumstances, and therefore, its purpose is to eliminate scratches, cracks, and damage to the tubular dielectric material caused by external vibrations and external forces, and also to reduce variations in silent discharge. It is an object of the present invention to provide an excellent laser oscillation device that can stabilize the laser output without any problems.

[発明の構成] (課題を解決するための手段) 本発明のレーザ発振装置は、管状誘電体の外側に対を成
す金属電極を配置し、内側にレーザガスを流通させて、
その励起を前記管状誘電体を介する金属電極間の無声放
電により行なうようにしたものにあって、上記管状誘電
体と金属電極との間に、弾性材から成る環状体を密着配
置したところに特徴を有するものである。
[Structure of the Invention] (Means for Solving the Problems) The laser oscillation device of the present invention has a tubular dielectric body, in which a pair of metal electrodes is arranged on the outside, and a laser gas is caused to flow inside.
The excitation is performed by silent discharge between metal electrodes via the tubular dielectric, and the feature is that an annular body made of an elastic material is closely disposed between the tubular dielectric and the metal electrode. It has the following.

(作用) 上記手段によれば、管状誘電体に対する金属電極の接触
が環状体によって避けられ、外部からの振動や外力もそ
の環状体によって吸収される。
(Function) According to the above means, contact of the metal electrode with the tubular dielectric body is avoided by the annular body, and external vibrations and external forces are also absorbed by the annular body.

又、管状誘電体と金属電極との間は環状体によって埋め
られ、空間の発生が避けられる。
Furthermore, the space between the tubular dielectric and the metal electrode is filled with the annular body, thereby avoiding the creation of a space.

(実施例) 以下本発明の一実施例につき第1図乃至第3図を参照し
て説明する。
(Embodiment) An embodiment of the present invention will be described below with reference to FIGS. 1 to 3.

まず第1図及び第2図において、21は石英ガラス等に
より断面円形に製造した管状誘電体であり、これの外側
両端部にそれぞれ環状体22.23を装着している。環
状体22.23は、いずれも耐高周波性及び耐高温性に
優れた例えばふっ素或いはシリコンゴム等の弾性材から
成るもので、断面円形の第3図に示すようなOリング状
に製造されている。これに対して24.25は図中上下
で対を成す金属電極であり、それぞれ内面が管状誘電体
21の外面より大なる曲率の円弧状を成していて、その
各円弧面により環状体22.23を管状誘電体1の外面
に押付けるようにして、これら環状体22.23の外側
従って又管状誘電体21の外側に配置している。この結
果、環状体22゜23は管状誘電体21とその外側に配
置した金属電極24.25との間に密着配置された形態
となっている。
First, in FIGS. 1 and 2, reference numeral 21 is a tubular dielectric body made of quartz glass or the like with a circular cross section, and annular bodies 22 and 23 are attached to both outer ends of the dielectric body, respectively. The annular bodies 22 and 23 are both made of an elastic material such as fluorine or silicone rubber that has excellent high frequency resistance and high temperature resistance, and are manufactured in the shape of an O-ring with a circular cross section as shown in FIG. There is. On the other hand, 24 and 25 are metal electrodes that form a pair at the top and bottom in the figure, and each inner surface forms an arc shape with a larger curvature than the outer surface of the tubular dielectric body 21. .23 are placed on the outside of these annular bodies 22, 23, and thus also on the outside of the tubular dielectric 21, so as to press against the outer surface of the tubular dielectric 1. As a result, the annular bodies 22 and 23 are arranged in close contact between the tubular dielectric body 21 and the metal electrodes 24 and 25 disposed on the outside thereof.

26は上述の管状誘電体21及び管状体22゜23並び
に金属電極24.25により構成した放電電極管で、こ
れの両側には放電電極管26の軸心がレーザ光軸と一致
するように、全反射ミラー27とレーザ取出し可能な反
射ミラー28とを配置している。更に、放電電極管26
にはガス循環体29をその両側で接続しており、ガス循
環体29の中央部には送風機30を冷却器31.32と
共に設けている。そして金属電極24.25には高電圧
の高周波電源33を接続している。
Reference numeral 26 denotes a discharge electrode tube constituted by the above-mentioned tubular dielectric body 21, tubular bodies 22, 23, and metal electrodes 24, 25, and on both sides of the discharge electrode tube 26 are provided such that the axis of the discharge electrode tube 26 coincides with the laser optical axis. A total reflection mirror 27 and a reflection mirror 28 from which a laser can be taken out are arranged. Furthermore, the discharge electrode tube 26
A gas circulation body 29 is connected on both sides of the gas circulation body 29, and a blower 30 is provided in the center of the gas circulation body 29 together with coolers 31, 32. A high-voltage, high-frequency power source 33 is connected to the metal electrodes 24 and 25.

以上のような構成で、ガス循環体29内に供給されたレ
ーザ媒質としてのガスすなわちレーザガスが、送風機3
0によりガス循環体29から管状誘電体21にかけ冷却
器31.32を通して循環され、その管状誘電体21の
内側を流通される。
With the above configuration, the gas as a laser medium supplied into the gas circulation body 29, that is, the laser gas, is supplied to the blower 3.
0 is circulated from the gas circulation body 29 to the tubular dielectric body 21 through the coolers 31 and 32, and is circulated inside the tubular dielectric body 21.

そしてそのような状況で、金属電極24.25には電源
33から高周波の高電圧が印加され、それによって金属
電極24.25間では管状誘電体21を介する無声放電
34が行なわれ、前記レーザガスの励起をする。これに
伴い、ミラー27.28間ではレーザ発振が起こり、ミ
ラー28からレーザ光35が取出される。
In such a situation, a high frequency high voltage is applied from the power source 33 to the metal electrodes 24, 25, and a silent discharge 34 occurs between the metal electrodes 24, 25 through the tubular dielectric 21, and the laser gas is Excite. Accordingly, laser oscillation occurs between mirrors 27 and 28, and laser light 35 is extracted from mirror 28.

この折り、環状体22.23は高周波の電界中に置かれ
、且つ高温(約20CM”C])になる管状誘電体21
に接し続けるが、前述のように耐高周波性及び耐高温性
に優れる材質から成るため、何ら問題なく使用し続ける
ことができる。
During this folding, the annular bodies 22 and 23 are placed in a high-frequency electric field, and the tubular dielectric body 21 is heated to a high temperature (approximately 20 CM"C).
However, as mentioned above, it is made of a material with excellent high frequency resistance and high temperature resistance, so it can be used without any problems.

そして、管状誘電体21に対する金属電極24゜25の
接触は上記環状体22.23によって避は続けられるも
のであり、外部からの振動や外力もその環状体22.2
3の弾性によって吸収され続ける。よって、石英ガラス
等から成る管状誘電体21に金属電極24.25による
傷付きやクラック更には破損をきたすということがなく
なる。
The contact of the metal electrodes 24 and 25 with the tubular dielectric body 21 is continued to be avoided by the annular body 22.23, and vibrations and external forces from the outside are also avoided by the annular body 22.2.
It continues to be absorbed by the elasticity of 3. Therefore, the tubular dielectric body 21 made of quartz glass or the like is prevented from being scratched, cracked, or even damaged by the metal electrodes 24,25.

又、管状誘電体21と金属電極24.25との各間は、
これもそれぞれ環状体22.23によって埋められるも
ので、それによりそこでの空間の発生が避けられること
から、無声放電34のばらつきをもなくして、レーザ出
力の安定化を達成することができる。
Moreover, between the tubular dielectric 21 and the metal electrodes 24 and 25,
These are also respectively filled by the annular bodies 22 and 23, thereby avoiding the generation of spaces therein, thereby eliminating variations in the silent discharge 34 and achieving stabilization of the laser output.

ここで、第4図は本発明の異なる実施例を示したもので
、前述の金属電極24.25に代わるそれよりも厚さの
大なる金属電極36.37にそれぞれ溝38.39を形
成し、それに環状体22゜23をそれぞれ嵌入させるよ
うにしたものであり、このようにすることによって、環
状体22.23及び金属電極36.37の固定をより確
実にすることができる。
FIG. 4 shows a different embodiment of the present invention, in which grooves 38 and 39 are formed in metal electrodes 36 and 37, which are thicker than the metal electrodes 24 and 25 described above, respectively. , and the annular bodies 22 and 23 are respectively fitted therein. By doing so, the annular bodies 22 and 23 and the metal electrodes 36 and 37 can be fixed more reliably.

又、第5図乃至第7図は本発明の更に異なる実施例を示
したもので、前述の環状体22.23に代え、管状誘電
体21と金属電極24.25との間に密着配置されるだ
けでなく金属電極24,25の両端部を覆いもする溝4
0.41を有する環状体42.43を使用するようにし
たものであり、このようにすることによって、金属電極
24.25の両端部での電界集中を低減でき、それらと
装置全体のアース部との距離を小さくできるため、装置
全体の小形化を達成することができる。又この場合、装
置を高出力化するに際しては、放電電極管26を特開昭
61−283184号公報に示されるように複数個設け
るが、このとき、上述同様の理由から、各放電電極管2
6の金属電極24゜25相互間隔を小さくすることがで
き、よってやはり全体の小形化を達成することができる
Further, FIGS. 5 to 7 show still another embodiment of the present invention, in which instead of the annular body 22, 23 described above, a ring body 22, 23 is disposed in close contact between the tubular dielectric body 21 and the metal electrode 24, 25. The groove 4 not only covers both ends of the metal electrodes 24 and 25, but also covers both ends of the metal electrodes 24 and 25.
0.41, and by doing so, it is possible to reduce the electric field concentration at both ends of the metal electrodes 24, 25, and to reduce the concentration of the electric field at both ends of the metal electrodes 24, 25, and to reduce the concentration of the electric field at both ends of the metal electrodes 24, 25. Since the distance between the two can be reduced, the entire device can be made smaller. In this case, when increasing the output of the device, a plurality of discharge electrode tubes 26 are provided as shown in Japanese Unexamined Patent Publication No. 61-283184, but in this case, for the same reason as above, each discharge electrode tube 2
The mutual spacing between the metal electrodes 24 and 25 of No. 6 can be reduced, so that the overall size can be reduced.

このほか、本発明は上記し且つ図面に示した実施例にの
み限定されるものではなく、要旨を逸脱しない範囲内で
適宜変更して実施し得る。
In addition, the present invention is not limited to the embodiments described above and shown in the drawings, but can be implemented with appropriate changes within the scope of the gist.

[発明の効果] 以上の記述で明らかなように、本発明のレーザ発振装置
は、管状誘電体と金属電極との間に、弾性材から成る環
状体を密芒配置したところに特徴を有するもので、それ
により、外部からの振動。
[Effects of the Invention] As is clear from the above description, the laser oscillation device of the present invention is characterized in that annular bodies made of an elastic material are closely arranged between the tubular dielectric body and the metal electrode. And as a result, vibrations from the outside.

外力による管状誘電体の傷付きやクラック、破損の発生
をなくし得、併せて無声放電のばらつきをもなくし得て
、レーザ出力の安定化を達成できるという優れた効果を
奏するものである。
This has the excellent effect of eliminating scratches, cracks, and breakage of the tubular dielectric due to external forces, as well as eliminating variations in silent discharge and stabilizing the laser output.

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

第1図乃至第3図は本発明の一実施例を示したもので、
第1図は全体の縦断正面図、第2図は第1図の■−■線
に沿う縦断側面図、第3図は環状体単体の斜視図である
。第4図は本発明の異なる実施例を示した第1図部分相
当図、第5図乃至第7図は本発明の更に異なる実施例を
示したもので、第5図は第1図相当図、第6図は第2図
相当図、第7図は第3図相当図である。そして第8図及
び第9図は従来のものを示したもので、第8図は第1図
相当図、第9図は第2図相当図である。 図面中、21は管状誘電体、22.23は環状体、24
.25は金属電極、36.37は金属電極、42.43
は環状体を示す。
1 to 3 show an embodiment of the present invention,
FIG. 1 is a longitudinal sectional front view of the whole, FIG. 2 is a longitudinal sectional side view taken along line 1--2 in FIG. 1, and FIG. 3 is a perspective view of the annular body alone. FIG. 4 is a partial view corresponding to FIG. 1 showing a different embodiment of the present invention, and FIGS. 5 to 7 are views showing further different embodiments of the present invention, and FIG. , FIG. 6 is a diagram equivalent to FIG. 2, and FIG. 7 is a diagram equivalent to FIG. 3. FIGS. 8 and 9 show conventional devices, with FIG. 8 being a diagram corresponding to FIG. 1, and FIG. 9 being a diagram corresponding to FIG. 2. In the drawing, 21 is a tubular dielectric body, 22.23 is an annular body, and 24
.. 25 is a metal electrode, 36.37 is a metal electrode, 42.43
indicates a toroidal body.

Claims (1)

【特許請求の範囲】[Claims] 1.管状誘電体の外側に対を成す金属電極を配置し、前
記管状誘電体の内側にレーザガスを流通させて、その励
起を前記管状誘電体を介する金属電極間の無声放電によ
り行なうレーザ発振装置において、前記管状誘電体と金
属電極との間に、弾性材から成る環状体を密着配置した
ことを特徴とするレーザ発振装置。
1. A laser oscillation device in which a pair of metal electrodes is arranged outside a tubular dielectric, a laser gas is caused to flow inside the tubular dielectric, and the excitation is performed by silent discharge between the metal electrodes via the tubular dielectric, A laser oscillation device characterized in that an annular body made of an elastic material is closely disposed between the tubular dielectric body and the metal electrode.
JP10104088A 1988-04-22 1988-04-22 Laser oscillating device Pending JPH01272173A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP10104088A JPH01272173A (en) 1988-04-22 1988-04-22 Laser oscillating device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP10104088A JPH01272173A (en) 1988-04-22 1988-04-22 Laser oscillating device

Publications (1)

Publication Number Publication Date
JPH01272173A true JPH01272173A (en) 1989-10-31

Family

ID=14290040

Family Applications (1)

Application Number Title Priority Date Filing Date
JP10104088A Pending JPH01272173A (en) 1988-04-22 1988-04-22 Laser oscillating device

Country Status (1)

Country Link
JP (1) JPH01272173A (en)

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