JPH03225978A - Gas laser oscillation apparatus - Google Patents

Gas laser oscillation apparatus

Info

Publication number
JPH03225978A
JPH03225978A JP1927190A JP1927190A JPH03225978A JP H03225978 A JPH03225978 A JP H03225978A JP 1927190 A JP1927190 A JP 1927190A JP 1927190 A JP1927190 A JP 1927190A JP H03225978 A JPH03225978 A JP H03225978A
Authority
JP
Japan
Prior art keywords
gas laser
main discharge
laser medium
flow
discharge space
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
JP1927190A
Other languages
Japanese (ja)
Inventor
Shigeyuki Takagi
茂行 高木
Saburo Sato
三郎 佐藤
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 JP1927190A priority Critical patent/JPH03225978A/en
Publication of JPH03225978A publication Critical patent/JPH03225978A/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 obtain a smooth gas flow speed by a method wherein individual side faces on the side of a main discharge space part are arranged on nearly the same face and are formed on the face which regulates the flow of a gas laser medium. CONSTITUTION:Peaking capacitors (15) of a nearly rectangular parallelepiped are arranged. The peaking capacitors (15) are formed on slopes (16) in such a way that one face of a hexahedron becomes a regulating face of the flow of a gas laser medium. Since the peaking capacitors (15) come into contact with each other and the slopes (16) are arranged to be nearly the same face, the slopes act in the same manner as a wind guide (10) and regulates the flow of the gas laser medium; the medium flows into a main discharge space. Since the slope (16) of the peaking capacitor (15) on the downstream side is directed to the diverging direction, the gas laser medium which has flowed into is discharged quickly from the main discharge space (4).

Description

【発明の詳細な説明】 [発明の目的] (産業上の利用分野) 本発明はガスレーザ発振装置に関する。[Detailed description of the invention] [Purpose of the invention] (Industrial application field) The present invention relates to a gas laser oscillation device.

(従来技術) レーザ光に対して主放電方向が直交するTEACO2レ
ーザやエキシマレーザなどのパルスレーザでは、その応
用上、高繰返し動作が望まれている。この種の従来のレ
ーザ発振装置について第4図を参照して説明する。すな
わち、レーザ管(1)を有し、内部に陰極(2)および
陽極(3)からなる一対の主放電電極が所定の主放電空
間(4)を形成して設けられている。なお、図示せぬが
主放電空間(4)を間にして紙面垂直方向において共振
器ミラーが配置されている。また、主放電空間(4)の
近傍に、主放電を安定に点弧させるための予備電離用の
ピン電極(5)が紙面垂直方向になるレーザ光軸に沿っ
て複数対設けられている。これらピン電極(5)はそれ
ぞれ波形成形のためのピーキングコンデンサ(6)を介
し主電源(7)に接続されている。レーザ管(1)の内
部には上記主放電電極の他に封入されているガスレーザ
媒質を冷却して循環させる熱交換器(8)、送風機(9
)および風ガイドCl0)が設けられている。
(Prior Art) In pulse lasers such as TEACO2 lasers and excimer lasers whose main discharge direction is orthogonal to the laser beam, high repetition rate operation is desired for their applications. A conventional laser oscillation device of this type will be explained with reference to FIG. That is, it has a laser tube (1), inside which a pair of main discharge electrodes consisting of a cathode (2) and an anode (3) are provided to form a predetermined main discharge space (4). Although not shown, a resonator mirror is arranged in the direction perpendicular to the plane of the paper with the main discharge space (4) in between. Further, in the vicinity of the main discharge space (4), a plurality of pairs of pin electrodes (5) for pre-ionization for stably igniting the main discharge are provided along the laser optical axis perpendicular to the plane of the paper. These pin electrodes (5) are each connected to a main power source (7) via a peaking capacitor (6) for waveform shaping. Inside the laser tube (1), in addition to the main discharge electrode, there are a heat exchanger (8) that cools and circulates the enclosed gas laser medium, and a blower (9).
) and a wind guide C10) are provided.

(発明が解決しようとする課題) 上記の構成になるガスレーザ発振装置では、主放電時に
陰極(2)および陽極(3)に多量の電気エネルギが注
入され、放電過程で発生するイオンや電子が例えばCC
I  SN I F 2などの放電生成物が発生する。
(Problems to be Solved by the Invention) In the gas laser oscillator having the above configuration, a large amount of electrical energy is injected into the cathode (2) and the anode (3) during main discharge, and ions and electrons generated during the discharge process are e.g. C.C.
Discharge products such as I SN IF 2 are generated.

これら放電生成物はガスレーザ媒質の流れにのって主放
電空間から速やかに排除される。ところで、ピーキング
コンデンサ(6)はレーザ発振装置以外にも使用されて
いる汎用性の円板状のものが使われ、第4図および第5
図に示すように、円形面を陰極(2)の両側面に接し光
共振方向に沿って複数配置されていた。このため、ピキ
ングコンデンサ(6)間の透き間や円弧部で描かれる波
状部分がガスレーザ媒質の流れを妨げ、上記放電生成物
の排除が不十分となっていた。放電生成物が不十分であ
ると主放電を妨げ、レーザの高繰返し化が困難になる問
題があった。
These discharge products are quickly removed from the main discharge space by the flow of the gas laser medium. By the way, the peaking capacitor (6) is a general-purpose disk-shaped capacitor that is used in other applications than laser oscillation devices, and is shown in Figures 4 and 5.
As shown in the figure, a plurality of circular surfaces were placed in contact with both side surfaces of the cathode (2) along the optical resonance direction. For this reason, the gaps between the picking capacitors (6) and the wavy portions drawn by the circular arc portions obstruct the flow of the gas laser medium, resulting in insufficient removal of the discharge products. If the discharge products are insufficient, there is a problem in that the main discharge is hindered, making it difficult to increase the repetition rate of the laser.

本発明は主放電部のインダクタンスを増すことなく、円
滑なガス流速が得られるガスレーザ発振装置を提供する
ことを目的とする。
An object of the present invention is to provide a gas laser oscillation device that can obtain a smooth gas flow rate without increasing the inductance of the main discharge section.

[発明の構成] (課題を解決するための手段と作用) ガスレーザ媒質を封入したレーザ管と、このレーザ管内
に対向して設けられた主放電電極と、上記主放電電極の
近傍に設けられた複数のピン電極と、これらピン電極に
それぞれ取付けられ放電波形を整形するピーキングコン
デンサと、主放電空間で発生したレーザ光を共振する光
共振器と、上記レーザ管内に設けられ上記ガスレーザ媒
質を循環させる循環手段とを備えたガスレーザ発振装置
において、上記各ピーキングコンデンサはほぼ直方体に
なり隣接する側面どうしが近接または当接して配置され
、上記主放電空間部側の各側面をほぼ同一面上に配置し
上記ガスレーザ媒質の流れを規制する規制面に形成した
もので、ガスレーザ媒質は規制面に案内されて主放電空
間を流れていく。
[Structure of the invention] (Means and effects for solving the problem) A laser tube enclosing a gas laser medium, a main discharge electrode provided oppositely within the laser tube, and a main discharge electrode provided near the main discharge electrode. A plurality of pin electrodes, a peaking capacitor attached to each of these pin electrodes to shape the discharge waveform, an optical resonator that resonates the laser light generated in the main discharge space, and a plurality of pin electrodes provided in the laser tube to circulate the gas laser medium. In the gas laser oscillation device, each of the peaking capacitors has a substantially rectangular parallelepiped shape, and adjacent side surfaces are arranged in close proximity or in contact with each other, and each side surface on the main discharge space side is arranged on substantially the same plane. It is formed on a regulating surface that regulates the flow of the gas laser medium, and the gas laser medium is guided by the regulating surface and flows through the main discharge space.

(実施例) 以下、実施例を示す図面に基づいて本発明を説明する。(Example) EMBODIMENT OF THE INVENTION Hereinafter, the present invention will be described based on drawings showing examples.

第1図は本発明の一実施例で、第3図と共通する部分に
は同一符号を付している。すなわち、第3図に示した従
来例と異なる点は、はぼ直方体のピーキングコンデンサ
(15)を配置した点にある。ピーキングコンデンサ(
15)は第2図に示すように、6面体の一面がガスレー
ザ媒質の流れの規制面となる傾斜面(16)に形成され
た形になり、第3図に示すように、傾斜面(16)を光
共振方向に沿ってほぼ同一面にし、互いに当接して配置
されている。この配置では、傾斜面(16)はガスレー
ザ媒質の流れの上流側では主放電空間(4)に対して上
記流れを絞り込むように規制する方向に揃えられ、同じ
く下流側では上記流れを発散する方向に揃えられている
FIG. 1 shows one embodiment of the present invention, and parts common to those in FIG. 3 are given the same reference numerals. That is, the difference from the conventional example shown in FIG. 3 is that a peaking capacitor (15) shaped like a rectangular parallelepiped is arranged. Peaking capacitor (
15) has a shape in which one side of the hexahedron is formed as an inclined surface (16) that serves as a regulating surface for the flow of the gas laser medium, as shown in FIG. 3, and as shown in FIG. ) are arranged on substantially the same plane along the optical resonance direction and in contact with each other. In this arrangement, the inclined surface (16) is aligned in a direction that restricts and restricts the flow of the gas laser medium with respect to the main discharge space (4) on the upstream side, and in a direction that diverges the flow on the downstream side. are arranged.

次に上記構成の作用について説明する。ピーキングコン
デンサ(15)は互いに当接し、また、傾斜面(16)
がほぼ同一面に揃えられているので、これら傾斜面が風
ガイド(10)と同様な作用をなしてガスレーザ媒質の
流れを規制して主放電空間に流入させる。また、下流側
はピーキングコンデンサ(15)の傾斜面(16)が発
散する方向に向いていているので、上記流入したガスレ
ーザ媒質は速やかに主放電空間(4)から排除される。
Next, the operation of the above configuration will be explained. The peaking capacitors (15) are in contact with each other and are also in contact with the inclined surface (16).
Since they are arranged substantially on the same plane, these inclined surfaces function similarly to the wind guide (10), regulating the flow of the gas laser medium and causing it to flow into the main discharge space. Furthermore, since the downstream side faces in the direction in which the slope (16) of the peaking capacitor (15) diverges, the gas laser medium that has flowed in is quickly removed from the main discharge space (4).

なお、上記実施例では規制面を傾斜面(16)としたが
、ガスレーザ媒質の流れに沿うような水平面に形成して
もよく、陰極(2)を間にして規制面を形成したピーキ
ングコンデンサ(15)をガスレーザ媒質の上流側、下
流側の両側に設けたが、上流側のみに設けてガスレーザ
媒質の流れを規制するようにしてもよい。また、傾斜面
(16)は平面に限らず曲面でも形成できる。さらに、
上記実施例ではピーキンクコンデンサ(15)を陰極(
2)側でなく、陽極(3)側あるいは両極側に取付ける
中間電位方式に適用してもよい。
In the above embodiment, the regulating surface is an inclined surface (16), but it may be formed on a horizontal surface along the flow of the gas laser medium. 15) are provided on both the upstream and downstream sides of the gas laser medium, but they may be provided only on the upstream side to regulate the flow of the gas laser medium. Further, the inclined surface (16) is not limited to a flat surface, but can also be formed as a curved surface. moreover,
In the above embodiment, the peak-ink capacitor (15) is connected to the cathode (
It may also be applied to an intermediate potential method in which it is attached to the anode (3) side or both electrodes instead of the 2) side.

[発明の効果コ 以上のように、従来ピーキンクコンデンサがガスレーザ
媒質の流れを阻害していたものが、本発明ではピーキン
グコンデンサがガスレーザ媒質の流れを円滑にし、流路
抵抗を著しく低下させたため、循環しているガス流速を
20〜50%も早めることが可能になった。したがって
、放電時に発生した放電生成物は主放電空間(4)から
速やかに排除されるので、主放電の間隔を早められ、レ
ザの高繰返しを向上させることを達成することができた
[Effects of the Invention] As described above, in the past, peaking capacitors obstructed the flow of the gas laser medium, but in the present invention, the peaking capacitor smoothes the flow of the gas laser medium and significantly reduces the flow path resistance. It has become possible to increase the circulating gas flow rate by 20 to 50%. Therefore, the discharge products generated during discharge are quickly removed from the main discharge space (4), so that the interval between main discharges can be shortened and high repetition rate of the laser can be improved.

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

第1図は本発明の一実施例を示す要部正面図、第2図は
ピーキンクコンデンサの拡大斜視図、第3図は上記一実
施例を示す要部側面図、第4図および第5図は従来例を
示す断面図および側面図である。 2)・・・陰極 3)・・・陽極 5)・・・ピン電極 15)・・・ピーキングコンデンサ 16)・・・傾斜面(規制面)
FIG. 1 is a front view of main parts showing an embodiment of the present invention, FIG. 2 is an enlarged perspective view of a peaking capacitor, FIG. 3 is a side view of main parts showing the above embodiment, and FIGS. The figures are a sectional view and a side view showing a conventional example. 2)...Cathode 3)...Anode 5)...Pin electrode 15)...Peaking capacitor 16)...Slanted surface (regulating surface)

Claims (1)

【特許請求の範囲】[Claims] ガスレーザ媒質を封入したレーザ管と、このレーザ管内
に対向して設けられた主放電電極と、上記主放電電極の
近傍に設けられた複数のピン電極と、これらピン電極に
それぞれ取付けられ放電波形を整形するピーキングコン
デンサと、主放電空間で発生したレーザ光を共振する光
共振器と、上記レーザ管内に設けられ上記ガスレーザ媒
質を循環させる循環手段とを備えたガスレーザ発振装置
において、上記各ピーキングコンデンサはほぼ直方体に
なり隣接する側面どうしが近接または当接して配置され
、上記主放電空間部側の各側面をほぼ同一面上に配置し
上記ガスレーザ媒質の流れを規制する規制面に形成した
ことを特徴とするガスレーザ発振装置。
A laser tube enclosing a gas laser medium, a main discharge electrode provided facing inside the laser tube, a plurality of pin electrodes provided in the vicinity of the main discharge electrode, and a plurality of pin electrodes each attached to each of these pin electrodes to control the discharge waveform. In a gas laser oscillation device comprising a peaking capacitor for shaping, an optical resonator for resonating laser light generated in a main discharge space, and a circulation means provided in the laser tube for circulating the gas laser medium, each of the peaking capacitors is It is characterized in that it has a substantially rectangular parallelepiped shape, and adjacent side surfaces are arranged close to each other or in contact with each other, and each side surface on the side of the main discharge space is arranged on substantially the same plane, and is formed as a regulating surface that regulates the flow of the gas laser medium. Gas laser oscillation device.
JP1927190A 1990-01-31 1990-01-31 Gas laser oscillation apparatus Pending JPH03225978A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1927190A JPH03225978A (en) 1990-01-31 1990-01-31 Gas laser oscillation apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1927190A JPH03225978A (en) 1990-01-31 1990-01-31 Gas laser oscillation apparatus

Publications (1)

Publication Number Publication Date
JPH03225978A true JPH03225978A (en) 1991-10-04

Family

ID=11994782

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1927190A Pending JPH03225978A (en) 1990-01-31 1990-01-31 Gas laser oscillation apparatus

Country Status (1)

Country Link
JP (1) JPH03225978A (en)

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