JPS63228772A - Highly repetitive pulsed laser electrode - Google Patents

Highly repetitive pulsed laser electrode

Info

Publication number
JPS63228772A
JPS63228772A JP6325887A JP6325887A JPS63228772A JP S63228772 A JPS63228772 A JP S63228772A JP 6325887 A JP6325887 A JP 6325887A JP 6325887 A JP6325887 A JP 6325887A JP S63228772 A JPS63228772 A JP S63228772A
Authority
JP
Japan
Prior art keywords
discharge
ionization
electrode
insulator
groove sections
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
JP6325887A
Other languages
Japanese (ja)
Inventor
Eiji Kaneko
英治 金子
Toru Tamagawa
徹 玉川
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 JP6325887A priority Critical patent/JPS63228772A/en
Publication of JPS63228772A publication Critical patent/JPS63228772A/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
    • H01S3/038Electrodes, e.g. special shape, configuration or composition

Landscapes

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

Abstract

PURPOSE:To stabilize pre-ionization and laser oscillation characteristics by forming a plurality of grooves orthogonal in the direction of discharge to the creeping surface of an insulator between counter electrodes for a pre-ionizing electrode. CONSTITUTION:Groove sections 6C orthogonal in the direction of discharge are shaped at two positions in the direction of discharge of an insulator 6. Since the breakdown voltage of space is acquired in the groove sections 6C at two positions while creeping surfaces except the groove sections 6C are exposed to the discharge of the groove sections 6C on pre-ionization, voltage is hardly obtained. Consequently, the breakdown voltage of the groove sections 6C is determined by the discharge distances of the groove sections 6C, and is not fluctuated by discharge. Accordingly, pre-ionization is conducted by stable breakdown voltage at all times regardless of the number of repetition and repeating frequency of discharge, thus acquiring stable laser oscillation characteristics.

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、高繰返しパルスレーザ装置に使用される高繰
返しパルスレーザ電極に関するものであり、特に予備放
電を行う予備電離電極部分に改良を施した高繰返しパル
スレーザ電極に係る。
[Detailed Description of the Invention] [Object of the Invention] (Industrial Application Field) The present invention relates to a high repetition pulse laser electrode used in a high repetition pulse laser device, and in particular to a pre-ionization electrode that performs preliminary discharge. It relates to a high repetition pulse laser electrode with improved parts.

(従来の技術) 近年、CO2レーデ、エキシマレーザ等の各種高繰返し
パルスレーザ“装置における技術の著しい進歩に伴い、
これらの各種高繰返しパルスレーザ装置の−・層の小型
化、高性能化が要求されている。
(Prior art) In recent years, with the remarkable progress in the technology of various high repetition pulse laser devices such as CO2 radar and excimer laser,
There is a demand for smaller layers and higher performance of these various high repetition pulse laser devices.

この様な高繰返しパルスレーザ装置としては、例えば、
第3図に承り様な実開昭55−65875〕号のζ案が
存在している。
As such a high repetition pulse laser device, for example,
As shown in Fig. 3, there is an acceptable proposal of ζ of Utility Model Application No. 55-65875.

第3図において、レーザキャビティ1内には、主放電電
極2,3か対向配置され、この主成電電4JJ2,3の
側方の近接位置には、予備電離電極4か配置されている
。予備電離電極4は、主成電電)※2,3に並べて配設
されたビーキングコンデン1す5に直列接続された電極
部材4A、4Bと、この間に配設されたレラミックチッ
プ等の絶縁物6から崩成されている。パルス電源装置か
ら放電部へのパルス電圧の供給は、給電導体7を介して
なされる様になっている。また、レーザキVビティ1の
壁面には、主放電電極2,3の長手方向両端に出力ミラ
ー8と全反射ミラー9とが配設され、この構成によって
主放電電極2,3間にグロー放電を生じた際、励起され
たレーザガスを共撮させてレーザ発売を71い、図中1
0に示す方向にレーザ光を取出す様になっている。
In FIG. 3, within the laser cavity 1, main discharge electrodes 2 and 3 are arranged facing each other, and a preliminary ionization electrode 4 is arranged at a position close to the side of the main discharge electrodes 4JJ2 and 3. The pre-ionization electrode 4 consists of electrode members 4A and 4B that are connected in series to beaking condensers 1 and 5 that are arranged side by side in the main ionizing electrodes)*2 and 3, and an insulator such as a relamic chip that is arranged between them. It is composed of object 6. The pulse voltage is supplied from the pulse power supply device to the discharge section via the power supply conductor 7. Furthermore, an output mirror 8 and a total reflection mirror 9 are disposed on the wall surface of the laser cutter V bit 1 at both ends of the main discharge electrodes 2 and 3 in the longitudinal direction. When this occurs, the excited laser gas is photographed together and the laser is released.
Laser light is emitted in the direction indicated by 0.

ところで、高繰返しパルスレーザ装置においては、主放
電電極2,3間に安定したグロー放電を発生するために
予め予備電離がなされるか、第3図の高繰返しパルスレ
ーザ装置における予(li?l電離は、予備電離電極4
の電4TI部材4A、48間に配置された絶縁物6の沿
面を放電ざぜて、紫外線光を発生させることで行なわれ
る。なお、第4図は、第3図の装置の予備電離電極4を
示す斜視図でおる。
By the way, in a high repetition pulse laser device, preliminary ionization is performed in advance to generate a stable glow discharge between the main discharge electrodes 2 and 3, or pre-ionization is performed in the high repetition pulse laser device in FIG. Ionization is carried out using the preliminary ionization electrode 4.
This is carried out by generating ultraviolet light by discharging the creeping surface of the insulator 6 disposed between the 4TI members 4A and 48. Incidentally, FIG. 4 is a perspective view showing the pre-ionization electrode 4 of the apparatus shown in FIG. 3.

しかしながら、この様に絶縁物6の沿面を放電させた場
合、放電や、電極スパッタリングで沿面か汚損されて、
沿面放電特性が変化すると、予備電離電極4の放電開始
電圧が変化してしまい、安定した紫外線光が得られなく
なる。この様に予備電離の条件か不安定c必るとレーザ
発振特性が安定Uず、特に繰返し数の多い場合や、繰返
し周液数の高い場合に、動作が著しく不安定となってし
にう。
However, when the creeping surface of the insulator 6 is discharged in this way, the creeping surface is contaminated by the discharge and electrode sputtering.
When the creeping discharge characteristics change, the discharge starting voltage of the pre-ionization electrode 4 changes, making it impossible to obtain stable ultraviolet light. If the pre-ionization conditions are unstable in this way, the laser oscillation characteristics will not be stable, and the operation will become extremely unstable, especially when the number of repetitions is large or the number of cycles is high. .

ざらに、絶縁物の沿面を放電ざぜるタイプの予備電離電
極4どしでは、第4図に示した様な単純形状の乙のの他
に、第5図に示す様に、絶縁物6の沿面に放電方向に沿
って溝部6Aを有し、この)jへ部6Aで放電を行なわ
けるものも存在している。
In general, in the pre-ionization electrode 4 of the type that causes discharge to occur along the creeping surface of an insulator, in addition to the simple shape shown in FIG. There is also a device that has a groove portion 6A along the discharge direction along the creeping surface and performs discharge at this portion 6A.

この様に、絶縁物6の溝部6Aで放電を行なわける場合
には、ぞれだけ紫外線光が強くなる利点をイjしている
反面、紫外線光が強力になるに従い絶縁物の沿面の1目
傷が多くなり、前記の様な予W1電離の不安定化が助長
されてしまう。
In this way, when discharging is carried out in the grooves 6A of the insulator 6, the advantage is that the ultraviolet light becomes stronger in each case. This increases the number of scratches and promotes the instability of pre-W1 ionization as described above.

(発明が解決しようとする問題点) 上記の様に、従来、絶縁物の沿面を放電させて予備電w
i@行なわせるタイプの高繰返しパルスレーザ装置にお
いては、放電や電極スパッタリングで放電開始電圧が変
化してしまい、この結果安定した条件の予備電離が不可
能となる問題点が存在していた。
(Problems to be Solved by the Invention) As mentioned above, conventionally, the creeping surface of an insulator is discharged to generate a preliminary
In the i@ type high repetition pulse laser device, there is a problem in that the firing voltage changes due to discharge and electrode sputtering, and as a result, pre-ionization under stable conditions is impossible.

本発明は、この様な従来技術の問題点を解決するために
提案されたものであり、その目的は、放電や電極スパッ
タリングによっても放電開始電圧が変化しない様にする
ことにより、常に安定した予備電離を行え、安定したレ
ーザ発振特性を得られる様な優れた高繰返しパルスレー
ザ電極を提供することである。
The present invention was proposed in order to solve the problems of the prior art, and its purpose is to maintain a stable reserve at all times by ensuring that the discharge starting voltage does not change due to discharge or electrode sputtering. An object of the present invention is to provide an excellent high repetition pulse laser electrode that can perform ionization and obtain stable laser oscillation characteristics.

[発明の構成] (問題点を解決するための手段) 本発明による高繰返しパルスレーザ電極は、予備電離電
極の対向電極の間に配置された絶縁物の沿面に、放電方
向と直交する複数の溝部を説けることを構成の特徴とし
ている。
[Structure of the Invention] (Means for Solving the Problems) The high repetition pulse laser electrode according to the present invention has a plurality of insulators disposed between the opposing electrodes of the pre-ionization electrode, along which a plurality of A feature of the composition is that it can explain the grooves.

(作用) 以上の様な構成を有する本発明においては、溝部にて空
間の絶縁破壊電圧を1qられる一方、溝部の放電に晒さ
れる他の沿面部では絶縁破壊電圧をほとんど得られない
ため、予備放電の放電開始電圧が複数の溝部の放電開始
電圧の総計にほぼ等しくなる。この場合、溝部の放電開
始電圧は、溝部の放電方向距離にて決定されるため、放
電や電極スパッタリングにJ、っても放電特性が変化す
ることはなく、従って、常に安定した予備電離を行え、
安定したレーリ゛光(辰特性を1qられる。
(Function) In the present invention having the above configuration, while the dielectric breakdown voltage of the space can be reduced by 1q in the groove, almost no dielectric breakdown voltage can be obtained in other creeping areas exposed to the discharge in the groove. The firing voltage of the discharge becomes approximately equal to the total of the firing voltages of the plurality of grooves. In this case, the discharge starting voltage of the groove is determined by the distance of the groove in the discharge direction, so the discharge characteristics do not change even if the discharge or electrode sputtering occurs. Therefore, stable pre-ionization can always be performed. ,
Stable ray light (1q of dragon characteristics).

(実施例) 以上説明した様な本発明による高繰返しパルスレーザ装
置極の実施例を以下に説明する。なお、第3図乃至第5
Nに示した従来技術と同一部分には同一?”]号を付し
、説明を省略する。
(Example) An example of the high repetition pulse laser apparatus pole according to the present invention as described above will be described below. In addition, Figures 3 to 5
Is the same part the same as the conventional technology shown in N? ”] and the explanation will be omitted.

第1図の実施例は、絶縁物6の放電方向の2箇所に放電
方向に直交する溝部6C@設【プたものである。この実
施例において、予備電離の際には、2箇所の溝部6Cに
て空間の絶縁破壊電圧が得られる一方、絶縁物6の溝部
6C以外の沿面においては、渦部6Cの放電に晒される
ためにほとんど電圧が19られない。従って、同実施例
において、予備放電の放電開始電圧は2箇所の溝部6C
の放電開始電圧の総計にほぼ等しくなる。この場合、溝
部6Cの放電開始電圧は、溝部6Cの放電方向距離にて
決定されるため、従来技術の様に放電やN極スパッタリ
ングによって絶縁物6の放電開始電圧が変化する問題は
ない。従って、本実施例においては、放電の繰返し数や
繰返し周波数の高さに拘らず、常時安定した放電開始電
圧を得られるため、常に安定した予備電離を行え、安定
したレーザ発(膜特性を得られる。
In the embodiment shown in FIG. 1, grooves 6C are provided at two locations in the discharge direction of the insulator 6, which are perpendicular to the discharge direction. In this embodiment, during pre-ionization, a spatial breakdown voltage is obtained at the two grooves 6C, while the creeping surface of the insulator 6 other than the grooves 6C is exposed to the discharge of the vortex 6C. Almost no voltage is applied. Therefore, in the same embodiment, the discharge starting voltage of the preliminary discharge is at the two groove portions 6C.
is approximately equal to the total discharge starting voltage. In this case, the firing voltage of the groove 6C is determined by the distance in the discharge direction of the groove 6C, so there is no problem that the firing voltage of the insulator 6 changes due to discharge or N-pole sputtering as in the prior art. Therefore, in this example, a stable discharge starting voltage can always be obtained regardless of the number of discharge repetitions or the height of the repetition frequency, so stable pre-ionization can always be performed, and stable laser emission (film characteristics can be obtained). It will be done.

第2図の実施例は放電方向に溝部6Aを有する絶縁物6
に本発明を施したものであり、絶縁物6の放電方向の溝
部6Aの構成面には、放電方向の2箇所に放電方向に直
交する溝部6Bが設けられている。本実施例においても
第1図の実施例と同様の作用効果を得られる。
The embodiment shown in FIG. 2 is an insulator 6 having a groove 6A in the discharge direction.
The present invention is applied to the groove portion 6A of the insulator 6 in the discharge direction, and groove portions 6B that are orthogonal to the discharge direction are provided at two locations in the discharge direction. In this embodiment as well, the same effects as in the embodiment shown in FIG. 1 can be obtained.

なお、本発明は前記実施例に限定されるものではなく、
例えば、放電方向と直交方向の溝部を3箇所以上に設(
プることも可能である。また、本発明は、全ての予備層
lit電極間に絶縁物を配置する構成と、一部の予備電
離電極間のみに絶縁物を配置する構成のいずれも可能で
ある。さらに、本発明は、予備電離電極部分の特に絶縁
物の形状の改良に係る発明であるため、その他の構成、
即ら、主成電電(〜やピーキングコンデンサ等の形状、
配置構成等は適宜選択可能である。
Note that the present invention is not limited to the above embodiments,
For example, grooves in the direction orthogonal to the discharge direction may be installed at three or more locations (
It is also possible to Furthermore, the present invention is capable of either a configuration in which an insulator is disposed between all of the pre-layer lit electrodes, or a configuration in which an insulator is disposed only between some pre-ionization electrodes. Furthermore, since the present invention relates to an improvement in the shape of the insulator of the pre-ionization electrode portion, other configurations,
That is, the shape of the main power source (~, peaking capacitor, etc.),
The arrangement and configuration can be selected as appropriate.

[発明の効果] 以」−説明した様に、本発明においては、予備電離電極
間に配設される絶縁物に、放電方向と直交づる溝部を設
けるという簡単な構成により、従来問題となっていた経
時的な絶縁物沿面の汚損の影響をほとんど受けることな
く、溝部の空間放電にで常に安定した放電開始電圧を得
られるため、安定したレーザ発振特性を得られる様な優
れた高繰返しパルスレーザ電極を提供できる。
[Effects of the Invention] - As explained above, the present invention solves the conventional problem by providing a simple structure in which a groove section perpendicular to the discharge direction is provided in the insulator disposed between the pre-ionization electrodes. This is an excellent high-repetition pulse laser that can obtain stable laser oscillation characteristics because it is almost unaffected by dirt on the creeping surface of the insulator over time and can always obtain a stable firing voltage due to the space discharge in the groove. Can provide electrodes.

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

第1図は本発明による高繰返しパルスレーザ電極の一実
施例を示す斜視図、第2図は本発明の他の実施例を示す
斜視図、第3図は従来の高繰返しパルスレーザ発振装置
を示す斜視図、第4図及び第5図はそれぞれ従来の異な
るパルスレーザ電(伽を示す斜視図である。 1・・・レーザキャビティ、2,3・・・主放電電極、
4・・・予備電離電極、4A、4B・・・電極部材、5
・・・ピーキングコンデンサ、6・・・絶縁物、6A〜
6C・・・絶縁物、7・・・給電導体、8・・・出力ミ
ラー、9・・・全反射ミラー、10・・・レーザ光。
Fig. 1 is a perspective view showing one embodiment of a high repetition pulse laser electrode according to the present invention, Fig. 2 is a perspective view showing another embodiment of the invention, and Fig. 3 is a perspective view showing a conventional high repetition pulse laser oscillation device. The perspective views shown, FIGS. 4 and 5, are respectively perspective views showing different conventional pulsed laser electrodes. 1... Laser cavity, 2, 3... Main discharge electrode,
4...Preliminary ionization electrode, 4A, 4B... Electrode member, 5
...Peaking capacitor, 6...Insulator, 6A~
6C... Insulator, 7... Power supply conductor, 8... Output mirror, 9... Total reflection mirror, 10... Laser light.

Claims (2)

【特許請求の範囲】[Claims] (1)対向配置された主放電電極の側方に主放電電極の
放電に先立って予備放電を行う予備電離電極を備え、こ
の予備電離電極の対向電極の間に絶縁物を配置して成る
高繰返しパルスレーザ電極において、 前記絶縁物の沿面に放電方向と直交する複数の溝部が設
けられたことを特徴とする高繰返しパルスレーザ電極。
(1) A high-pressure high-voltage device is equipped with a pre-ionization electrode on the side of the main discharge electrode arranged oppositely to perform a preliminary discharge prior to the discharge of the main discharge electrode, and an insulator is arranged between the counter electrode of the pre-ionization electrode. A high repetition pulse laser electrode, characterized in that a plurality of grooves perpendicular to the discharge direction are provided along the creeping surface of the insulator.
(2)絶縁物が、その放電方向に溝部を有するものであ
る特許請求の範囲第1項記載の高繰返しパルスレーザ電
極。
(2) The high repetition pulse laser electrode according to claim 1, wherein the insulator has a groove in the discharge direction.
JP6325887A 1987-03-18 1987-03-18 Highly repetitive pulsed laser electrode Pending JPS63228772A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6325887A JPS63228772A (en) 1987-03-18 1987-03-18 Highly repetitive pulsed laser electrode

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6325887A JPS63228772A (en) 1987-03-18 1987-03-18 Highly repetitive pulsed laser electrode

Publications (1)

Publication Number Publication Date
JPS63228772A true JPS63228772A (en) 1988-09-22

Family

ID=13224060

Family Applications (1)

Application Number Title Priority Date Filing Date
JP6325887A Pending JPS63228772A (en) 1987-03-18 1987-03-18 Highly repetitive pulsed laser electrode

Country Status (1)

Country Link
JP (1) JPS63228772A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0294486A (en) * 1988-09-29 1990-04-05 Komatsu Ltd Excimer laser device

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0294486A (en) * 1988-09-29 1990-04-05 Komatsu Ltd Excimer laser device

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