JPS6356973A - Laser exciting device - Google Patents

Laser exciting device

Info

Publication number
JPS6356973A
JPS6356973A JP20108386A JP20108386A JPS6356973A JP S6356973 A JPS6356973 A JP S6356973A JP 20108386 A JP20108386 A JP 20108386A JP 20108386 A JP20108386 A JP 20108386A JP S6356973 A JPS6356973 A JP S6356973A
Authority
JP
Japan
Prior art keywords
discharge
cathode
electrodes
anode
capacitors
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
JP20108386A
Other languages
Japanese (ja)
Inventor
Takekuni Azuma
吾妻 健国
Akira Usui
明 臼井
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 JP20108386A priority Critical patent/JPS6356973A/en
Publication of JPS6356973A publication Critical patent/JPS6356973A/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
    • H01S3/09Processes or apparatus for excitation, e.g. pumping
    • H01S3/097Processes or apparatus for excitation, e.g. pumping by gas discharge of a gas laser
    • H01S3/0971Processes or apparatus for excitation, e.g. pumping by gas discharge of a gas laser transversely excited

Landscapes

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

Abstract

PURPOSE:To obtain a laser output of a high crest value caused by a short-time discharge by fixing the capacitors for storing the charges required for a pair of opposedly placed discharge electrodes to cause a discharge between the discharge electrodes as spacers. CONSTITUTION:Four capacitors 16 are charged to about 15-20KV by a d.c. power supply 14, and this charging voltage is continuously applied across an anode 4 and a cathode 3. In this condition, when a pulse power supply 21 provides a gate pulse to a thyristor 20 to momentarily turn it on, the potential of a preliminary discharge electrode 12 rises to cause a spark discharge between a preliminary discharge electrode 11 and simultaneously to ionize with ultraviolet rays a mixed gas containing a CO2 gas in the primary discharge space wherein the anode 4 and the cathode 3 are opposed to each other. Also, an avalanche discharge phenomenon is induced by the ionization between both electrodes, causing a laser oscillation. In this case, since the four capacitors 16 are directly connected to the primary discharge electrodes, the connecting conductors between the two become the shortest thereby making the inductance of the discharge circuit remarkably small, which enables a short-time discharge as well as availability of a laser output of a short pulse, high crest value.

Description

【発明の詳細な説明】 [産業上の利用分野〕 この発明は、グロー放電を起こしてレーザ媒質ガスを励
起させるレーザ励起装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a laser excitation device that excites a laser medium gas by generating a glow discharge.

[従来の技術] この種のレーザとしては、エキシマレーザ(Exci+
wer La5er)あるいは横方向励起式大気圧炭酸
ガス(Transversely Excited A
tmosphericpressureccJ2Las
er 、以下TEA CO2L/−ザと言う)等がある
。第3図は従来のTEA coz レーザ励起装置を1
部分的に破断した斜視図である。同図において、レーザ
励起空間を形成する金属円筒(1)の一端には部分反射
鏡(2)が、その他端には図示されない全反射鏡がそれ
ぞれ取付けられ、さらにその内部には陰極(3)と陽極
(4)とが所定の間隙で対向配置されて放電部(5)を
形成している。また、陰極(3)の近傍には予@i’t
ta用の予備放電電極(6)が設けられ、さらに、陽極
(4)の下方にガスを循環させるファン(7)が設けら
れている。一方、金属円筒(1)の外部には高圧電源部
(8)と、この高圧電源部(8)によって充電され、そ
の充電電圧を陰極(3)および陽極(4)間に印加した
り、あるいは、陰極(3)および予備放電電極(6)間
に印加したりするコンデンサ(3)とが設けられている
[Prior Art] As this type of laser, excimer laser (Exci+
wer La5er) or Transversely Excited A
tmosphericpressureccJ2Las
er, hereinafter referred to as TEA CO2L/-za). Figure 3 shows a conventional TEA coz laser excitation device.
FIG. 3 is a partially cutaway perspective view. In the same figure, a partial reflection mirror (2) is attached to one end of a metal cylinder (1) forming a laser excitation space, and a total reflection mirror (not shown) is attached to the other end, and a cathode (3) is attached inside the metal cylinder (1). and an anode (4) are arranged facing each other with a predetermined gap to form a discharge section (5). In addition, there is a pre-@i't near the cathode (3).
A preliminary discharge electrode (6) for ta is provided, and a fan (7) for circulating gas below the anode (4) is also provided. On the other hand, the outside of the metal cylinder (1) is charged by a high voltage power source (8), and the charging voltage is applied between the cathode (3) and the anode (4), or , a capacitor (3) for applying voltage between the cathode (3) and the preliminary discharge electrode (6).

かかる構成により、金属円筒(1)の内部に1気圧程度
の炭酸ガスを含む混合ガスを供給する一方、コンデンサ
(9)の充電電圧を陰極(3)および陽極(4)間、陰
極(3)および予備放電電極(6)間にそれぞれ印加す
ると放電部(5)にグロー放電が起きて混合ガスが励起
されると共に、部分反射鏡(2)からレーザ光(10)
が放射される。
With this configuration, a mixed gas containing carbon dioxide at about 1 atm is supplied to the inside of the metal cylinder (1), while the charging voltage of the capacitor (9) is transferred between the cathode (3) and the anode (4), and between the cathode (3) and the anode (4). and the preliminary discharge electrode (6) respectively, a glow discharge occurs in the discharge part (5), the mixed gas is excited, and the laser beam (10) is emitted from the partially reflecting mirror (2).
is emitted.

[発明が解決しようとする問題点] 上記のように構成された従来のレーザ励起装置は、コン
デンサ(9〕を金属円筒(1)7の外部に設置し、この
コンデンサ(8)と金属円筒(1)の内部の各電極とを
導線で接続していたがために、放電回路の浮遊インダク
タンスが増えて瞬間的な放電ができず、その分だけ高波
高値のレーザ出力が得難かった。
[Problems to be Solved by the Invention] In the conventional laser excitation device configured as described above, the capacitor (9) is installed outside the metal cylinder (1) 7, and the capacitor (8) and the metal cylinder ( 1) Since each internal electrode was connected with a conductive wire, the stray inductance of the discharge circuit increased and instantaneous discharge was not possible, making it difficult to obtain a laser output with a high wave peak value.

また、金属円筒(1)の内部に収納配置される陰極(3
)および陽極(4)は相互間隔を一定に保持する必要が
あるが、長期間に亘って間隔を一定に保持することが難
しく、放電状態もばらつくという問題があった。
In addition, a cathode (3) is housed inside the metal cylinder (1).
) and the anode (4), it is necessary to keep the mutual spacing constant, but there is a problem in that it is difficult to keep the spacing constant over a long period of time, and the discharge state also varies.

一方、金属円筒(1)の外部に設置したコンデンサ(9
)は、形状の異る種々のものを用いるが、その占有スペ
ースもかなり大きくなって、装置全体を小型化し難かっ
た。
On the other hand, a capacitor (9) installed outside the metal cylinder (1)
) uses a variety of different shapes, but they occupy a considerable amount of space, making it difficult to downsize the entire device.

この発明は上記の問題点を解決するためになされてもの
で、高波高値のレーザ出力を長期に亘って安定的に取り
出し得、しかも、小型化が容易なレーザ励起装置の提供
を目的とする。
The present invention has been made to solve the above-mentioned problems, and aims to provide a laser excitation device that can stably extract laser output with a high peak value over a long period of time, and that can be easily miniaturized.

[問題点を解決するための手段] この発明に係るレーザ励起装置は、対向装置した一対の
放電電極が放電を起こすに必要な電荷を蓄えるコンデン
サを、放電電極間にスペーサとして固定したものである
[Means for Solving the Problems] In the laser excitation device according to the present invention, a capacitor that stores the electric charge necessary for causing a discharge between a pair of facing discharge electrodes is fixed as a spacer between the discharge electrodes. .

[作用] この発明においてはレーザ励起に適した放電を得るため
のコンデンサを放電電極のスペーサとすることにより、
この両者間の接続導線が最短で済むと同時に放電回路の
浮遊インダクタンスが最小になり、短時間放電による高
波高値のレーザ出力が得られる。また、コンデンサを放
電電極のスペーサとすることにより、電極間隙が長期に
亘って一定に保持され、安定な放電状態が得られること
になる。さらに、コンデンサを放電電極のスペーサとし
た場合には、金属円筒の外部に設置するコンデンサの個
数が大幅に減らされ、これによって装置全体の小型化が
可能になる。
[Function] In this invention, by using a capacitor as a spacer of the discharge electrode to obtain a discharge suitable for laser excitation,
The connecting conductor between the two can be kept as short as possible, and at the same time, the stray inductance of the discharge circuit can be minimized, and a laser output with a high peak value can be obtained by short-time discharge. Furthermore, by using a capacitor as a spacer for the discharge electrodes, the gap between the electrodes is maintained constant over a long period of time, resulting in a stable discharge state. Furthermore, if a capacitor is used as a spacer for the discharge electrode, the number of capacitors installed outside the metal cylinder can be significantly reduced, thereby making it possible to downsize the entire device.

[実施例コ 第1図および第2図はこの発明の一実施例を示もので、
このうち、第2図はTEA CO2レーザ励起装置の電
気回路図、第1図はこの装置の主要部の詳細な構成を示
す餌視図である。これら各図において、所定の間隙で対
向配置される陰極(3)および陽極(4)は多孔質の鉄
板を船底状に滑らかにプレス成形したものでなり、陰極
(3)の背面部に予備放電電極対(11)、(12)が
設置されている。ここで、予備放電電極(11)は矩形
断面を有し、第3図に示す金属円筒(1)の軸方向に細
長く形成され。
[Example 1] Figures 1 and 2 show an example of this invention.
Of these, FIG. 2 is an electric circuit diagram of the TEA CO2 laser excitation device, and FIG. 1 is a bait-view diagram showing the detailed configuration of the main parts of this device. In each of these figures, the cathode (3) and anode (4), which are arranged opposite to each other with a predetermined gap, are made of a porous iron plate press-molded smoothly into the shape of a ship's bottom. Electrode pairs (11) and (12) are installed. Here, the preliminary discharge electrode (11) has a rectangular cross section and is formed elongated in the axial direction of the metal cylinder (1) shown in FIG.

予備放電電極数(12)はピン状でその先端がそれぞれ
予備放電電極(11)の側面に向くように保持されてい
る。また、予備放電電極(12)の基端にはそれぞれI
KΩ程度の抵抗器(13)の一端が接続され、その他端
は共通接続されている。一方、陽極、電極間にグロー放
電を起こすための直流電源(14)を備え、その正極が
IONΩ程度の抵抗器(15)を介して陽極(4)に、
負極は陰極(3)にそれぞれ接続されている。さらに、
陽極(0および陰極(3)間には10gFのコンデンサ
(16)が4個並列接続されている。また、予備放電電
極(11)および(12)間に電圧を印加するための直
流電源(17)を備え、その正極が予備放電電極(11
)と陰極(3)とに接続され、負極はINΩ程度の抵抗
器(18)およびlpF程度のコンデンサ(19)を介
して抵抗器(13)の相互接合点に接続されている。そ
して、予備放電を開始させるために7ノードが接地され
たサイリスタ(20)のカソードが抵抗器(18)およ
びコンデンサ(19)の相互接合点に接続され、このサ
イリスタ(10)にパルス電源(21)がゲートパルス
を与えるようになっている。
The number of pre-discharge electrodes (12) are pin-shaped and are held such that their tips face the side surfaces of the pre-discharge electrodes (11). Further, at the base end of the preliminary discharge electrode (12), I
One end of a resistor (13) of about KΩ is connected, and the other ends are commonly connected. On the other hand, it is equipped with a DC power source (14) for causing a glow discharge between the anode and the electrode, and the positive electrode is connected to the anode (4) via a resistor (15) of approximately IONΩ.
The negative electrodes are each connected to a cathode (3). moreover,
Four 10 gF capacitors (16) are connected in parallel between the anode (0) and the cathode (3). Also, a DC power supply (17) is used to apply voltage between the preliminary discharge electrodes (11) and (12). ), the positive electrode of which is a preliminary discharge electrode (11
) and a cathode (3), and the negative electrode is connected to the mutual junction of the resistors (13) via a resistor (18) of about INΩ and a capacitor (19) of about lpF. Then, the cathode of a thyristor (20) whose 7 nodes are grounded is connected to the mutual junction of the resistor (18) and the capacitor (19) in order to start a preliminary discharge, and the pulse power source (21) is connected to the thyristor (10). ) is designed to give a gate pulse.

なお、上述した陰極(3)、陽極(4)およびコンデン
サ(1B)は第1図に示すように一体構成になっている
。すなわち、陰極(3)および陽極(4)はともに板厚
が1.Os+で、直径2■の孔がピッチ2.6■であけ
られ、開孔率が52%の矩形状の多孔質鉄板でなり、板
幅中央部が船底状に曲げ成形されている。また、コンデ
ンサ(16)は直径60m層、高さ20m層程度の円筒
状に形成されたセラミックコンデンサでなっている。そ
して、これらのコンデンサ〔16〕は対向配置される陰
極(3)および陽極(4)の4つの間にそれぞれスペー
サとして固定され、ネジ(22)によって極板の隅を締
付けることによってこれらが一体化されると同時に電気
的にも接続される。なお、陰極(3)および陽極(4)
を外部接続するために、それぞれ極板の側方から陰極り
−1”(31)および陽極リード(41)が導出されて
いる。
Note that the above-mentioned cathode (3), anode (4), and capacitor (1B) are integrally constructed as shown in FIG. That is, both the cathode (3) and the anode (4) have a plate thickness of 1.5 mm. Os+ is made of a rectangular porous iron plate with holes of 2 mm diameter drilled at a pitch of 2.6 mm and a porosity of 52%, with the central part of the plate width bent to resemble the bottom of a ship. The capacitor (16) is a cylindrical ceramic capacitor with a diameter of 60 m and a height of about 20 m. These capacitors [16] are each fixed as a spacer between the cathode (3) and anode (4) that are arranged opposite each other, and are integrated by tightening the corners of the electrode plates with screws (22). At the same time, they are also electrically connected. In addition, the cathode (3) and the anode (4)
For external connection, a cathode lead (31) and an anode lead (41) are led out from the sides of the electrode plate, respectively.

上記のように構成されたレーザ励起装置の動作を以下に
説明する。
The operation of the laser excitation device configured as described above will be explained below.

まず、4個のコンデンサ(16)は直流電源(14)に
よって15〜20KV程度に充電され、この充電電圧が
常時陽極(4)および陰極(3)間に印加されている。
First, the four capacitors (16) are charged to about 15 to 20 KV by the DC power supply (14), and this charging voltage is constantly applied between the anode (4) and the cathode (3).

この状態でパルス電源(21)がサイリスク(20)に
ゲートパルスを与えてこれを瞬間的にオン状態にすると
、予備放電電極(12)の電位が上昇し、予備放電電極
(11)との間に火花放電を生じさせると共に、これが
発すると紫外線により陽極(4)および陰極(3)が対
向する主放電空間の002ガスを含む混合ガスを電離さ
せる。また、 ’1を敲によって両電極間になだれ放電
現象が誘起されてレーザ発振が起こる。
In this state, when the pulse power source (21) applies a gate pulse to the cyrisk (20) to turn it on momentarily, the potential of the pre-discharge electrode (12) rises, and the potential between the pre-discharge electrode (11) and the A spark discharge is generated, and when this is emitted, ultraviolet rays ionize the mixed gas containing 002 gas in the main discharge space where the anode (4) and cathode (3) face each other. Further, by tapping '1', an avalanche discharge phenomenon is induced between both electrodes and laser oscillation occurs.

この場合、4つのコンデンサ(1B)は主放電電極に直
接接続されるため、両者間の接続導線が最短になって放
電回路のインダクタンスが著しく小さくなり、これによ
って IJL秒以下の短時間放電が可能になると共に、
短パルス高波高値のレーザ出力が得られる。
In this case, the four capacitors (1B) are directly connected to the main discharge electrode, so the connecting conductor between them becomes the shortest and the inductance of the discharge circuit becomes significantly smaller, which allows short-time discharge of less than IJL seconds. Along with becoming
Laser output with short pulses and high peak values can be obtained.

また、陽極(4)および陰極(3)間の4隅にそれぞれ
スペーサが挿入されたがため長期間に亘って間隙を一定
に保持することができ、これによって放電およびレーザ
発振の安定化が図られる。
In addition, since spacers are inserted at each of the four corners between the anode (4) and cathode (3), the gap can be maintained constant over a long period of time, which helps stabilize discharge and laser oscillation. It will be done.

さらに、従来装設では主放電用のコンデンサを金属円筒
(1)の外側部に設置していたので装置全体の小型化に
限度があったが、この実施例では主放電用のコンデンサ
(16)を金属円筒の内部に収納したことになり、その
分だけ装置の小型化が容易になっている。
Furthermore, in conventional installations, the main discharge capacitor (16) was installed outside the metal cylinder (1), which limited the ability to miniaturize the entire device; however, in this embodiment, the main discharge capacitor (16) is housed inside the metal cylinder, making it easier to downsize the device.

なお、上記実施例では主放電用のコンデンサ(16)が
4個の場合について説明したが、陽8i(4)および陰
極(3)の形状、材質等に゛よってより多くのスペーサ
を介在させる必要がある場合には容量の小さい5個以上
のコンデンサをそれぞれスペーサとして固定するように
してもよい。
In the above embodiment, the case where there are four main discharge capacitors (16) was explained, but it may be necessary to use more spacers depending on the shape, material, etc. of the anode 8i (4) and the cathode (3). In some cases, five or more capacitors with small capacitances may be fixed as spacers.

なおまた、上記実施例ではTEA co2 レーザの場
合について述べたが、高圧力のレーザガスを用いたパル
ス放電励起によって発振を行なわせるエキシマレーザに
も本発明を適用し得ることは言うまでもない。
Furthermore, although the above embodiments have been described with respect to the case of a TEA co2 laser, it goes without saying that the present invention can also be applied to an excimer laser in which oscillation is performed by pulse discharge excitation using a high-pressure laser gas.

[発明の効果] 以上の説明によって明らかなように、この発明によれば
、放電電荷を蓄えるコンデンサを、放電電極間のスペー
サとして固定したので、高波高値のレーザ出力を長期間
に亘って安定的に取り出し得、しかも小型化が容易にな
るという効果がある。
[Effects of the Invention] As is clear from the above explanation, according to the present invention, the capacitor that stores the discharge charge is fixed as a spacer between the discharge electrodes, so that the laser output with a high wave peak value can be stably maintained over a long period of time. It has the effect that it can be taken out easily and can be easily miniaturized.

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

第1図はこの発明の一実施例の要部の構成を示す斜視図
、第2図は同実施例の電気回路図、第3図は従来のレー
ザ励起装置の斜視図である。 図において (3)は陰極、(4)は陽極、 (+2)、(13)は予備放電電極、(14)は直流電
源、(16)はコンデンサ。 なお、各図中、同一符号は同−又は相当部分を示す。 代  理  人   大  岩  増  雄第2図 3F  Pt本!=(fJ’Xtt本缶)4:P4樟(
・  ) 第3図
FIG. 1 is a perspective view showing the configuration of essential parts of an embodiment of the present invention, FIG. 2 is an electric circuit diagram of the same embodiment, and FIG. 3 is a perspective view of a conventional laser excitation device. In the figure, (3) is the cathode, (4) is the anode, (+2) and (13) are the preliminary discharge electrodes, (14) is the DC power supply, and (16) is the capacitor. In each figure, the same reference numerals indicate the same or corresponding parts. Agent Masuo Oiwa Figure 2 3F Pt book! = (fJ'Xtt book can) 4:P4 camphor (
・ ) Figure 3

Claims (2)

【特許請求の範囲】[Claims] (1)レーザ媒質ガスを供給するレーザ励起空間に一対
の放電電極を対向配置し、コンデンサの充電電圧を前記
放電電極間に印加してグロー放電を起こして前記レーザ
媒質ガスを励起するレーザ励起装置において、前記コン
デンサをスペーサとして前記放電電極間に配置して固定
したことを特徴とするレーザ励起装置。
(1) A laser excitation device that arranges a pair of discharge electrodes facing each other in a laser excitation space that supplies laser medium gas, and applies a charging voltage of a capacitor between the discharge electrodes to cause glow discharge and excite the laser medium gas. A laser excitation device according to the invention, wherein the capacitor is arranged and fixed between the discharge electrodes as a spacer.
(2)前記コンデンサは円筒状コンデンサを4個並列接
続したものでなり、この円筒状コンデンサをそれぞれ前
記放電電極の4つの隅部に配置したことを特徴とする特
許請求の範囲第1項記載のレーザ励起装置。
(2) The capacitor is composed of four cylindrical capacitors connected in parallel, and each of the cylindrical capacitors is arranged at four corners of the discharge electrode. Laser excitation device.
JP20108386A 1986-08-27 1986-08-27 Laser exciting device Pending JPS6356973A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP20108386A JPS6356973A (en) 1986-08-27 1986-08-27 Laser exciting device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP20108386A JPS6356973A (en) 1986-08-27 1986-08-27 Laser exciting device

Publications (1)

Publication Number Publication Date
JPS6356973A true JPS6356973A (en) 1988-03-11

Family

ID=16435109

Family Applications (1)

Application Number Title Priority Date Filing Date
JP20108386A Pending JPS6356973A (en) 1986-08-27 1986-08-27 Laser exciting device

Country Status (1)

Country Link
JP (1) JPS6356973A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02199883A (en) * 1989-01-30 1990-08-08 Mitsubishi Electric Corp Gas laser device

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02199883A (en) * 1989-01-30 1990-08-08 Mitsubishi Electric Corp Gas laser device

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