JPS6251277A - Gas laser device - Google Patents

Gas laser device

Info

Publication number
JPS6251277A
JPS6251277A JP18991285A JP18991285A JPS6251277A JP S6251277 A JPS6251277 A JP S6251277A JP 18991285 A JP18991285 A JP 18991285A JP 18991285 A JP18991285 A JP 18991285A JP S6251277 A JPS6251277 A JP S6251277A
Authority
JP
Japan
Prior art keywords
cathode
gas
anode
flow
auxiliary 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
JP18991285A
Other languages
Japanese (ja)
Inventor
Osamu Morimiya
森宮 脩
Setsuo Suzuki
鈴木 節雄
Etsuo Noda
悦夫 野田
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 JP18991285A priority Critical patent/JPS6251277A/en
Publication of JPS6251277A publication Critical patent/JPS6251277A/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 simplify the structure of a cathode, to decrease man-hours in manufacturing the title device and in maintenance and inspection and to reduce the capacity of a gas circulating blower, by providing a plurality of auxiliary discharge electrodes between the cathode and an anode on a plane, which intersects the flow of laser gas at a right angle. CONSTITUTION:A cathode 10 is arranged at the upstream side of the flow of laser gas P. An anode 13 is arranged at the downstream side. A DC voltage is applied across both electrodes 10 and 13, and glow discharge is generated in the same direction as the flow of the laser gas P. The laser beam output C is taken out with the excitation of the laser gas and the resonation of an optical resonator. A plurality of auxiliary discharge electrodes 15 are provided between the cathode 10 and the anode 13 on a plane, which intersect the flow of the laser gas P at a right angle. The electrodes 15 generate auxiliary discharge in the direction crossing the flow of the laser gas P between the cathode 10 and the anode 13. A plate body 12 provided with a plurality of projections 12a is provided at the side part of the cathode 10 or the anode 13 facing the auxiliary discharge electrodes generating the auxiliary discharge.

Description

【発明の詳細な説明】 〔寥で明の技術分野〕 、この11明は、レーザガスの流れど略同一方向に放電
を、生じさ、せ、かつ上記ガスレーザの流れと直交する
。方向にレーザビームを取出すガス循環型二軸直交型の
ガスレーザ装置に関する。
DETAILED DESCRIPTION OF THE INVENTION [Technical field of the invention] This eleventh generation generates a discharge in substantially the same direction as the flow of the laser gas, and is perpendicular to the flow of the gas laser. The present invention relates to a gas circulation type biaxially orthogonal type gas laser device that emits a laser beam in a direction.

〔発明のだ術的背祭とその問題点〕[The trickery of invention and its problems]

従来より1.ガス2レーザ装置として二輪直交型のもの
が知られている。第7図、に二軸直交型の 。
1. A two-wheel orthogonal type device is known as a two-gas laser device. Figure 7 shows the biaxial orthogonal type.

CO2レーザ装置を示M0 −によって図中矢印で示す向きで循環しており、このガ
ス]〕の流れの上流側に陰極1が、また、同下流側に陽
極2か配設されている。陰極1は、多数の陰極ビン3を
ガスPの流れと直交する面内て等間隔に配置して構成さ
れる。また、陽極2は、カスPの流れと直交する方向に
平行l1il!置された複数の陽極棒4で構成される。
The CO2 laser device is circulated by M0 - in the direction shown by the arrow in the figure, and a cathode 1 is disposed on the upstream side of the flow of this gas, and an anode 2 is disposed on the downstream side of the flow. The cathode 1 is constructed by arranging a large number of cathode bottles 3 at equal intervals in a plane perpendicular to the flow of the gas P. Further, the anode 2 is parallel to the direction perpendicular to the flow of the waste P. It is composed of a plurality of anode rods 4 placed in one place.

そして、陰極1.陽極2間をバラスト抵抗5,6を介し
て直流型#i7に接続し、両電極間の空間Qにグ[]−
敢電を生起口しめ、空間Qを挟むように設けられた全反
則ミラー8とハーフミラ−9とによってレーザビームC
を取出すようにしている。
And cathode 1. The anode 2 is connected to the DC type #i7 via the ballast resistors 5 and 6, and the space Q between both electrodes is connected to the
A laser beam C is generated by a full anti-fouling mirror 8 and a half mirror 9 provided so as to sandwich a space Q between them.
I'm trying to take it out.

このように構成された従来の二軸直交型カスレーザ装置
のビーム出力を数kw以上に上をさせるには、電極間の
空間Qに生成される放電の空間的−(革性が要求される
。このため、従来の高出力ガスレーザ装置においては、
第7図にも示すように、数百乃至千という撓めて多数の
陰極ビン3を^d置する必要があり、l1ifの製作に
当たって多くの手間がかかるうえ、保守・点検にも多大
な肋間が費やされるという欠点があった。
In order to increase the beam output of the conventional two-axis orthogonal Cass laser device configured in this manner to more than several kilowatts, the discharge generated in the space Q between the electrodes must have spatial characteristics. For this reason, in conventional high-power gas laser equipment,
As shown in Fig. 7, it is necessary to bend and place a large number of cathode bins 3 in the order of hundreds to thousands, which requires a lot of effort in manufacturing the l1if, and also requires a large amount of space between the ribs for maintenance and inspection. The disadvantage was that it was costly.

また、陰極1を多数の陰極ビン3で構成すると、必然的
にガス循環路の流体抵抗が増Jため、ガス循環用のブロ
アーを大出力にしな4(ればならないという欠点もあっ
た。
Furthermore, if the cathode 1 is constituted by a large number of cathode bins 3, the fluid resistance of the gas circulation path will inevitably increase, so there is also the drawback that the blower for gas circulation must have a high output.

〔ブを明の目的) 本発明は、かかる従来の欠点の基つきなされたものであ
り、その目的と覆るところは、陰極構造の簡素化を図る
ことができ、これにJ:って装置の製作時、保守・点検
時の工数低減を図るとともにカス循環用ブロアーの小容
量化を図り得るカスレーザ装置を提供することにある。
[Purpose of the present invention] The present invention was made based on these conventional drawbacks, and its purpose is to simplify the cathode structure, and to improve the structure of the J: device. It is an object of the present invention to provide a waste laser device that can reduce the number of man-hours during manufacturing, maintenance, and inspection, and can also reduce the capacity of a blower for circulating waste.

〔発明の概要〕[Summary of the invention]

本発明は、レーザガスの流れの上流側に陰極を配置する
とともに同下流側に陽極を配置し、両極間に直流電圧を
印加して前記レー17”カスの流れと同方向にグロー放
電を生じさせ、レーザガスの励起と光共振器による共振
どによってレーザビーム出力を取出すガスレーザ装置に
おいて、前iiL!隙極と前記陽極との間でかつ前記レ
ーザガスの流れと直交りる面上に配置され前記陰極若し
くは前記陽極との間で前記レーザガスの流れを横切る方
向の補助放電を生起さけるための複数の補助放電電極を
備えるとともに、前記補助放電電極との間で補助放電を
生じさせる前記陰極若しくは前記陽極を前記補助放電電
極に対向する辺部に複数の突起を有する板状体で形成し
たことを特徴としている。
In the present invention, a cathode is placed on the upstream side of the flow of laser gas, and an anode is placed on the downstream side of the same, and a DC voltage is applied between the two electrodes to generate a glow discharge in the same direction as the flow of the laser gas. , in a gas laser device which extracts a laser beam output by excitation of laser gas and resonance by an optical resonator, the cathode or A plurality of auxiliary discharge electrodes are provided to avoid generating an auxiliary discharge in a direction transverse to the flow of the laser gas between the anode and the cathode or the anode that causes an auxiliary discharge between the auxiliary discharge electrode and the anode. It is characterized by being formed of a plate-like body having a plurality of protrusions on the side facing the auxiliary discharge electrode.

(発明の効果〕 このような構造であると、印加電圧が低い場合でも陰極
若しくは陽極の突起部と補助放電電極との間で補助放電
が始まり、板状電極の全体から補助放電電1iに放電が
広がる。イして、この放電はカスの流れを横切るように
発生するので、陰極と陽極との間の主グロー放電の幅が
広がり、結果的に放電の空間的−横付が増すことになる
(Effect of the invention) With this structure, even when the applied voltage is low, auxiliary discharge starts between the protrusion of the cathode or anode and the auxiliary discharge electrode, and discharge from the entire plate electrode to the auxiliary discharge electrode 1i. Since this discharge occurs across the flow of dregs, the width of the main glow discharge between the cathode and the anode increases, resulting in an increase in the spatial distribution of the discharge. Become.

このように、本発明によれば多数の電極ビンではなく、
板状電極と補助放電電極とによって放電の空間的−横付
を確保するようにしているので、電極の構成要素を削減
することができ、装置の製造工数、保守・点検時の手間
を大幅に削減することができる。
Thus, according to the present invention, instead of a large number of electrode bins,
Since the plate electrode and the auxiliary discharge electrode ensure the spatial and horizontal distribution of discharge, the number of electrode components can be reduced, significantly reducing the number of man-hours required for manufacturing the device and the effort required for maintenance and inspection. can be reduced.

また、陰極の構成要素を少なくできることにJ−って同
時にガス循環路の流体抵抗も少なくできるので、ガス循
環用のブロアーの小容量を図ることができる。
Moreover, since the number of components of the cathode can be reduced, the fluid resistance of the gas circulation path can also be reduced, so that the capacity of the blower for gas circulation can be reduced.

〔発明の実施例) 以下、図面を参照しながら、本発明の一実施例について
説明する。なお、第1図乃〒第3図において第4図と同
一部分には同一符号を付し、詳しい説明は省くことにす
る。
[Embodiment of the Invention] Hereinafter, an embodiment of the present invention will be described with reference to the drawings. In addition, in FIGS. 1 to 3, the same parts as in FIG. 4 are given the same reference numerals, and detailed explanations will be omitted.

第1図および第2図は一実施例に係る二軸直交型のガス
レーザ装置を示したもので、ガスPの流れと光の共振方
向とが略直交するものである。すなわち、陰極10は、
上下2段でかつ共振方向に配設され先端部がガスPの流
れの向きに延出している複数の陰極ビン11と、これら
陰極ビン11の先端部に固定された陰極板12とで構成
されている。陰極ビン11の数は第7図に示した従来も
のより大幅に少なくなっている。陰極板12は、その両
面を前記共振方向と平行に配置したもので、先端側の両
端部に突起12aを形成したものとなっている。ガスの
下流側に設けられた陽極13は、共振方向を長手方向ど
し上下2段に平行配置された2本の陽惨棒14で構成さ
れている。さらに、陰4fi10と@極13との間で、
かつ陰極10に近接するfff Itには、補助放電電
極15が配置されている。この補助放電N極15は、第
2図にも示すように、陰極10に対し上下方向位置を異
ならせかつ陽極棒14と平行に配置された3本の補助電
極棒16で構成される。そして。
FIGS. 1 and 2 show a biaxial orthogonal type gas laser device according to an embodiment, in which the flow of gas P and the resonance direction of light are substantially perpendicular to each other. That is, the cathode 10 is
It is composed of a plurality of cathode bins 11 arranged in upper and lower stages in the resonance direction and whose tips extend in the direction of the flow of gas P, and cathode plates 12 fixed to the tips of these cathode bins 11. ing. The number of cathode bins 11 is significantly smaller than the conventional one shown in FIG. The cathode plate 12 has both surfaces arranged parallel to the resonance direction, and has protrusions 12a formed at both ends on the tip side. The anode 13 provided on the downstream side of the gas is composed of two rods 14 disposed parallel to each other in two upper and lower stages with the resonance direction aligned in the longitudinal direction. Furthermore, between the negative 4fi10 and the @pole 13,
Further, an auxiliary discharge electrode 15 is arranged at fff It close to the cathode 10 . As shown in FIG. 2, this auxiliary discharge N-electrode 15 is composed of three auxiliary electrode rods 16 arranged at different positions in the vertical direction with respect to the cathode 10 and parallel to the anode rod 14. and.

この補助放電電1ii15は、バラスト抵抗11を介し
て電源7の陽極側に接続される。
This auxiliary discharge voltage 1ii15 is connected to the anode side of the power source 7 via the ballast resistor 11.

このような構造であると、夕日−放電は、まず陰極10
と補助放電電極15どの間に生じる。ここで生じた荷電
粒子の一部はガス流に乗って陽極13に達する。したが
って、主グロー放電は補助放電電極15がない場合に比
べて低い電圧で始動する。
With such a structure, the sunset discharge first occurs at the cathode 10.
and the auxiliary discharge electrode 15. Some of the charged particles generated here reach the anode 13 on the gas flow. Therefore, the main glow discharge starts at a lower voltage than when the auxiliary discharge electrode 15 is not present.

ところで、一般にカス流中の放電は、放電路がガスの流
れに沿う傾向にあるので、陰極側の間隔が1 cm以上
であると、放電の空間的一様性が失われる。したがって
、従来は陰極ビンの数を減らすことができなかった。
By the way, in general, in a discharge in a waste flow, the discharge path tends to follow the gas flow, so if the gap on the cathode side is 1 cm or more, the spatial uniformity of the discharge will be lost. Therefore, conventionally it has not been possible to reduce the number of cathode bins.

しかし、この場合には陰極10に陰極板12を用い、こ
の陰極板12に突起12aを形成しているので、ガス圧
が50Torr以上の高圧下でもグローの偏りが生じず
、陰極グローを陰極板12の表面に均一に広げることが
できる。つまり、陰極10ど補助hQ電電極15と間に
ガス流を横切るように生じる補助放電が、陰極板12の
全体に均一に広がるので、第2図に示すように、陰惨1
0と陽4I113との間の主グロー放電の空間的一様性
も高めることができる。
However, in this case, the cathode plate 12 is used as the cathode 10, and the protrusion 12a is formed on the cathode plate 12, so that even under high gas pressure of 50 Torr or more, the glow does not become uneven, and the cathode glow is transferred to the cathode plate. It can be spread evenly over 12 surfaces. In other words, the auxiliary discharge generated across the gas flow between the cathode 10 and the auxiliary hQ electrode 15 spreads uniformly over the entire cathode plate 12, resulting in a disastrous 1
The spatial uniformity of the main glow discharge between 0 and positive 4I113 can also be increased.

これは本発明者等が行なった実験によっても確認された
。すなわち、この実験では、陰極ビン11を従来の二分
の−に減らしても、放電の空間的一様性は失われること
がなく、ガスの励起領域(空間Q)に投入される放電電
力が大幅に増加することが判明した。
This was also confirmed by experiments conducted by the present inventors. In other words, in this experiment, even if the cathode bin 11 was reduced to half of the conventional size, the spatial uniformity of the discharge was not lost, and the discharge power input into the gas excitation region (space Q) was significantly reduced. was found to increase.

ぞして、この場合には、ガスPの流れに直交する面内に
おける陰極ビン11の密度を従来に比べて疎にすること
ができるので、ガス循環路の流体抵抗を減らすことがで
きる。このため、ガス循環用のブロアー容麺を少なくす
ることができる。
Therefore, in this case, the density of the cathode bins 11 in the plane perpendicular to the flow of the gas P can be made sparser than in the conventional case, so that the fluid resistance of the gas circulation path can be reduced. Therefore, the number of blowers for gas circulation can be reduced.

尚、本発明は上記実施例に限定されるものではない。Note that the present invention is not limited to the above embodiments.

一ト記実施例では陰極板12を共振方向と平行に配置し
たが、第3図および第4図に示すように、陰極板12を
共振方向と直交する向きに配置するようにしても良い。
In the first embodiment, the cathode plate 12 is arranged parallel to the resonance direction, but as shown in FIGS. 3 and 4, the cathode plate 12 may be arranged perpendicular to the resonance direction.

また、第5図に示すように、電極板12および補助電極
棒16の両者を共振方向に対して直交する向きに配置す
るようにしても良い。
Further, as shown in FIG. 5, both the electrode plate 12 and the auxiliary electrode rod 16 may be arranged in a direction perpendicular to the resonance direction.

これらいずれも、従来の装置に比べて構成要素の数が大
幅に少なく、製造、保守・点検の工数削減に寄与するこ
とは明らかである。
All of these devices have a significantly smaller number of components than conventional devices, and it is clear that they contribute to reducing man-hours for manufacturing, maintenance, and inspection.

また、第6図に示す装置は、補助放電電極15と直流電
源7との間に電流制限インピーダンス21と交流電源2
2とを直列に介挿したものである。
The device shown in FIG. 6 also includes a current limiting impedance 21 and an AC power source 2 between the auxiliary discharge electrode 15 and the DC power source 7.
2 are inserted in series.

このような装置によれば、前述した効果を秦することは
勿論のこと、直流電源7の負担を軽減できるという効果
を秦する。
According to such a device, not only the above-mentioned effects are achieved, but also the effect that the load on the DC power supply 7 can be reduced is achieved.

また、本弁明は、補助放電電極15をグラファイト、シ
リコンカーバイト・などの抵抗体で構成するようにして
も良い。この場合には、バラスト抵抗17やインピーダ
ンス21の一部を省略づることが可能である。
Further, in the present invention, the auxiliary discharge electrode 15 may be made of a resistor such as graphite or silicon carbide. In this case, it is possible to omit part of the ballast resistor 17 and impedance 21.

また、以上の各実施例では陰極を板状体としたが、補助
放電N極15が陽極どの間で補助放電を起こさせるもの
である場合には、陽極を板状体にし、この板状体の補助
放電電極に対向する辺部に複数の突起を形成するように
すれば良い。
Further, in each of the above embodiments, the cathode is a plate-shaped body, but if the auxiliary discharge N-electrode 15 is to cause an auxiliary discharge between the anodes, the anode is formed into a plate-shaped body, and the plate-shaped body is used as the anode. A plurality of protrusions may be formed on the side facing the auxiliary discharge electrode.

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

第1図は本発明の一実施例に係るカスレーず装置の゛要
部を゛示す斜視図、第2図は同装置の模式的側面図、第
3図〜第6図は本発明の他の実施例に係るガスレーザ装
置をそれぞれ示す図、第7図は従来のガスレーザ装置の
要部を示す斜視図である。 1.10・・・陰極、2,13・・・陽極、3.11・
・・陰極ビン、4.14・・・陽極棒、5 、6 、1
7・・・バラスト抵抗、8・・・全反射ミラー、9・・
・ハーフミラ−112a・・・突起、15・・・補助放
電電極、16・・・補助電極棒、21・・・電流制限イ
ンピーダンス、31・・・陰極板、P・・・カス、Q・
・・空間、0・・・レーザビーム。
FIG. 1 is a perspective view showing the essential parts of a casslaying device according to an embodiment of the present invention, FIG. 2 is a schematic side view of the same device, and FIGS. FIG. 7 is a perspective view showing main parts of a conventional gas laser device. 1.10... cathode, 2,13... anode, 3.11.
...Cathode bottle, 4.14...Anode rod, 5, 6, 1
7... Ballast resistance, 8... Total reflection mirror, 9...
- Half mirror 112a... Protrusion, 15... Auxiliary discharge electrode, 16... Auxiliary electrode rod, 21... Current limiting impedance, 31... Cathode plate, P... Scrap, Q.
...Space, 0...Laser beam.

Claims (4)

【特許請求の範囲】[Claims] (1)レーザガスの流れの上流側に陰極を配置するとと
もに同下流側に陽極を配置し、両極間に直流電圧を印加
して前記レーザガスの流れと同方向にグロー放電を生じ
させ、レーザガスの励起と光共振器による共振とによっ
てレーザビーム出力を取出すガスレーザ装置において、
前記陰極と前記陽極との間でかつ前記レーザガスの流れ
と直交する面上に配置され前記陰極若しくは前記陽極と
の間で前記レーザガスの流れを横切る方向の補助放電を
生起させるための複数の補助放電電極を備えるとともに
、前記補助放電電極との間で補助放電を生じさせる前記
陰極若しくは前記陽極が前記補助放電電極に対向する辺
部に複数の突起を形成してなる板状体であることを特徴
とするガスレーザ装置。
(1) A cathode is placed on the upstream side of the flow of laser gas, and an anode is placed on the downstream side of the same, and a DC voltage is applied between the two electrodes to generate a glow discharge in the same direction as the flow of the laser gas to excite the laser gas. In a gas laser device that extracts laser beam output by resonance with an optical resonator,
A plurality of auxiliary discharges arranged between the cathode and the anode and on a plane orthogonal to the flow of the laser gas, and for generating auxiliary discharges in a direction transverse to the flow of the laser gas between the cathode and the anode. The cathode or the anode, which is provided with an electrode and generates an auxiliary discharge between the auxiliary discharge electrode and the auxiliary discharge electrode, is a plate-like body formed with a plurality of protrusions on a side facing the auxiliary discharge electrode. gas laser equipment.
(2)前記補助放電電極は、前記陰極との間でグロー放
電を生じさせるものであ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装置。
(2) The gas laser device according to claim 1, wherein the auxiliary discharge electrode generates a glow discharge between the auxiliary discharge electrode and the cathode.
(3)前記補助放電電極と、前記陰極若しくは前記陽極
との間で交流放電を生じさせる特許請求の範囲第1項記
載のガスレーザ装置。
(3) The gas laser device according to claim 1, wherein an alternating current discharge is caused between the auxiliary discharge electrode and the cathode or the anode.
(4)前記補助放電電極は、抵抗体であることを特徴と
する特許請求の範囲第1項記載のガスレーザ装置。
(4) The gas laser device according to claim 1, wherein the auxiliary discharge electrode is a resistor.
JP18991285A 1985-08-30 1985-08-30 Gas laser device Pending JPS6251277A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP18991285A JPS6251277A (en) 1985-08-30 1985-08-30 Gas laser device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP18991285A JPS6251277A (en) 1985-08-30 1985-08-30 Gas laser device

Publications (1)

Publication Number Publication Date
JPS6251277A true JPS6251277A (en) 1987-03-05

Family

ID=16249288

Family Applications (1)

Application Number Title Priority Date Filing Date
JP18991285A Pending JPS6251277A (en) 1985-08-30 1985-08-30 Gas laser device

Country Status (1)

Country Link
JP (1) JPS6251277A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0553533U (en) * 1991-12-25 1993-07-20 コクヨ株式会社 Steel locker

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0553533U (en) * 1991-12-25 1993-07-20 コクヨ株式会社 Steel locker

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