JPH04283976A - Gas laser oscillation device - Google Patents

Gas laser oscillation device

Info

Publication number
JPH04283976A
JPH04283976A JP4714891A JP4714891A JPH04283976A JP H04283976 A JPH04283976 A JP H04283976A JP 4714891 A JP4714891 A JP 4714891A JP 4714891 A JP4714891 A JP 4714891A JP H04283976 A JPH04283976 A JP H04283976A
Authority
JP
Japan
Prior art keywords
discharge
gas laser
flow
laser medium
paths
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.)
Granted
Application number
JP4714891A
Other languages
Japanese (ja)
Other versions
JP3065681B2 (en
Inventor
Koji Kakizaki
弘司 柿崎
Katsuya Omura
大村 克也
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 JP4714891A priority Critical patent/JP3065681B2/en
Publication of JPH04283976A publication Critical patent/JPH04283976A/en
Application granted granted Critical
Publication of JP3065681B2 publication Critical patent/JP3065681B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Abstract

PURPOSE:To enable a discharge product to be discharged outside a location near a discharge portion and a stable pulse discharge to be performed repeatedly by branching from an input/output path near a discharge side of a gas laser medium at a main discharge electrode toward a discharging direction and at the same time forming a discharge path so that it merges circulation. CONSTITUTION:A gas laser medium which flows toward a discharge portion is divided into two parts, namely those passing an input/output path 30 along guide bodies 22 and 23 and those flowing to first paths 28a and 28b after entering through flow entrances 29a and 29b. Flow is rapid since the flow entrances 29a and 29b are wide and the flow is constricted inside in the first flow paths 28a and 28b, thus enabling a flow which is suctioned to a side of the first paths 28a and 28b to be generated at second paths 30a and 30b. The sucked gas merges the gas laser medium passing the discharge portion at a circulation flow path again.

Description

【発明の詳細な説明】[Detailed description of the invention]

[発明の目的] [Purpose of the invention]

【0001】0001

【産業上の利用分野】本発明は横励起方式のガスレーザ
発振装置に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a transverse excitation type gas laser oscillation device.

【0002】0002

【従来の技術】パルス発振が行われるエキシマレーザや
TEACO2 ガスレーザ発振装置などのパルスレーザ
では、レーザ出力は1パルス当りのジュール数とパルス
発振の繰返し数の積から算出される。このことから高出
力を得るために、従来より主放電の繰返し数を増加させ
る種々の提案がなされている。主放電の繰返し数を上げ
るためには、主放電時に発生した放電生成物や放電電極
の電極面に滞留している負イオンを放電空間外の遠くに
排除することが重要で、この排除が効果的に行われない
状態で繰返し数を上げても、放電部においてガスレーザ
媒質の排出側にレーザ発振に寄与しないアーク放電が発
生してしまうことになる。図5は特開平1ー24688
1号公報に開示された上記提案に係わるものひとつであ
る。すなわち、ガスレーザ媒質を所定圧力で封入した放
電管(1)内には2枚の保持板(2),(3) が平行
状態に所定の間隔をおき、さらに放電管(1) に対し
て電気的に絶縁状態に上下に設けられている。保持板(
2),(3) の対向される面には放電管(1) の軸
方向に沿って長尺の陰極(4),陽極(5) がそれぞ
れに結合され、これらによって主放電電極が構成されて
いる。陰極(4),陽極(5) の左右側部に近接して
複数の予備電離電極(6) が所定ピッチで保持板(2
),(3) 上に設けられている。各予備電離電極(6
) の中途部にはピーキングコンデンサ(7) がそれ
ぞれ設けられている。さらに、放電管(1) 内には上
記ガスレーザ媒質を循環させるファン(8) および熱
交換器(9) が設けられているとともに、ファン(8
) で起こされた風を上記主放電電極間に導くための第
1、第2の風ガイド(10),(11) が設けられて
いる。上記第1の風ガイド(10)は放電管(1) の
内面に沿うように延長され、矢印Aで示すように、上記
ガスレーザ媒質が保持板(2),(3) の縁部間を通
り、陰極(4),陽極(5) のそれぞれの電極面にほ
ぼ平行に流れるように形成されている。一方、第2の風
ガイド(11)は陽極(5) 側の保持板(3) を貫
通し、陽極(5) とガス流の上流側に位置する予備電
離電極(6) との間に開口して設けられ、矢印Bで示
すように、ガスレーザ媒質を陰極(4) の電極面に交
差する方向へ流すようになっている。
2. Description of the Related Art In a pulsed laser such as an excimer laser or a TEACO2 gas laser oscillator that performs pulse oscillation, the laser output is calculated from the product of the number of joules per pulse and the number of repetitions of pulse oscillation. For this reason, in order to obtain high output, various proposals have been made to increase the number of repetitions of the main discharge. In order to increase the number of repetitions of main discharge, it is important to remove discharge products generated during main discharge and negative ions that remain on the electrode surface of the discharge electrode far outside the discharge space, and this removal is effective. Even if the number of repetitions is increased without being carried out properly, arc discharge that does not contribute to laser oscillation will occur on the discharge side of the gas laser medium in the discharge section. Figure 5 is Japanese Patent Publication No. 1-24688.
This is one of the proposals related to the above proposal disclosed in Publication No. 1. In other words, two holding plates (2) and (3) are placed parallel to each other at a predetermined distance within a discharge tube (1) in which a gas laser medium is sealed at a predetermined pressure, and an electric current is applied to the discharge tube (1). They are placed one above the other in an insulated state. Holding plate (
A long cathode (4) and an anode (5) are connected to the facing surfaces of the discharge tube (1) along the axial direction of the discharge tube (1), and these constitute the main discharge electrode. ing. A plurality of pre-ionization electrodes (6) are arranged at a predetermined pitch on the left and right sides of the cathode (4) and anode (5), respectively, on the holding plate (2).
), (3) are provided above. Each pre-ionization electrode (6
) A peaking capacitor (7) is provided in the middle of each. Furthermore, a fan (8) for circulating the gas laser medium and a heat exchanger (9) are provided in the discharge tube (1).
) are provided for guiding the wind generated between the main discharge electrodes. The first wind guide (10) extends along the inner surface of the discharge tube (1), and as shown by arrow A, the gas laser medium passes between the edges of the holding plates (2) and (3). , the cathode (4), and the anode (5). On the other hand, the second wind guide (11) passes through the holding plate (3) on the anode (5) side and has an opening between the anode (5) and the preionization electrode (6) located upstream of the gas flow. As shown by arrow B, the gas laser medium is caused to flow in a direction intersecting the electrode surface of the cathode (4).

【0003】0003

【発明が解決しようとする課題】上記の構成では矢印A
の流れと矢印Bの流れが交差することになるので、互い
の流れの状態によっては、放電空間への流入間際で流れ
が乱され、放電生成物や負イオンを放電空間からより遠
くへ排除することが難しくなる場合も生じていた。また
、第2の風ガイド(11)を無くし、第1の風ガイド(
10)のみでガスレーザ媒質を流す場合、ファン(8)
を大型のものにして風量を増大することで効果的な排除
が可能にはなるが、装置を少しでも小形化しようとする
要望には反することになる。
[Problem to be solved by the invention] In the above configuration, the arrow A
Since the flow shown by arrow B intersects with the flow shown by arrow B, depending on the state of each flow, the flow is disturbed just before it enters the discharge space, and discharge products and negative ions are expelled further from the discharge space. There were times when this became difficult. Also, the second wind guide (11) is eliminated and the first wind guide (
When flowing the gas laser medium only with 10), the fan (8)
Although effective removal becomes possible by increasing the air volume by making the device larger, this goes against the desire to make the device as small as possible.

【0004】本発明はこのような事情に鑑みてなされた
もので、ファンなどの送風手段を大型化せずにパルス発
振の繰返し数を上げ、レーザの高出力化を可能にするガ
スレーザ発振装置を提供することを目的とする。 [発明の構成]
The present invention has been made in view of the above circumstances, and provides a gas laser oscillation device that can increase the number of pulse oscillation repetitions and increase the output of the laser without increasing the size of the blowing means such as a fan. The purpose is to provide. [Structure of the invention]

【0005】[0005]

【課題を解決するための手段】ガスレーザ媒質を所定の
圧力で封入した気密容器と、この気密容器内に主放電空
間を形成して設けられた少なくとも一対の主放電電極と
、上記ガスレーザ媒質を上記気密容器内で循環させる循
環手段と、循環されたガスレーザ媒質を上記主放電電極
の間に導き排出する入出路を形成するガイド体と、上記
主放電電極における上記ガスレーザ媒質の排出側近傍に
なる入出路から排出方向に向けられて分岐するとともに
上記循環に合流するように形成された排出路とを備えた
ことを特徴とする。
[Means for Solving the Problems] An airtight container in which a gas laser medium is sealed at a predetermined pressure; at least a pair of main discharge electrodes provided to form a main discharge space within the airtight container; A circulation means for circulating the gas laser medium in the airtight container, a guide body forming an input/output path for guiding and discharging the circulated gas laser medium between the main discharge electrodes, and an input/output path near the discharge side of the gas laser medium in the main discharge electrode It is characterized by comprising a discharge passage which is formed to branch from the outlet passage in the discharge direction and join the circulation.

【0006】[0006]

【作用】電極のガスレーザ媒質の排出側近傍に生じる渦
流で滞留しがちな放電生成物が瞬時に放電部近傍外へ排
出される。
[Operation] The discharge products that tend to stay due to the vortex generated near the discharge side of the gas laser medium of the electrode are instantly discharged outside the vicinity of the discharge section.

【0007】[0007]

【実施例】以下,実施例を示す図面に基づいて説明する
。図1は本発明のー実施例で放電部およびその近傍部分
を拡大して示したものである。すなわち、保持板(20
),(21) を有し、これらの互いの対向面にはほぼ
同形状で、ふっ素樹脂の成形体になるガイド体(22)
,(23) が対称的に設けられている。ガイド体(2
2),(23) は横断面が緩やかな山状に形成され、
図2に示すように紙面垂直方向になる管軸方向側に長尺
で、また、頂部部分(22a),(23a) と本体(
22b).(23b) の二つに分かれる分割体に形成
されている。頂部部分(22a),(23a) には長
尺の凹溝が形成され主放電電極を構成する陰極(24)
および陽極(25)がそれぞれ埋設されている。また、
本体(22b),(23b) には、図3に示すように
頂部部分(22a),(23a) を所定ピッチで貫通
して設けられた予備電離電極の一方をなす複数のピン電
極(26a),(26b) にそれぞれ接続されるピー
キングコンデンサ(27)が埋設されている。また、本
体(22b),(23b)の内部には上記長尺方向の幅
員に比べてやや狭い幅のスリット状の第1の通路(28
a),(28b) が形成されている。この第1の通路
(28a),(28b) のガスレーザ媒質の放電部へ
の流入側は大きく開いた流入口(29a),(29b)
 に形成されている。また、第1の通路(28a),(
28b) に連通する細穴状の複数の第2の通路(30
a),(30b) がそれぞれ頂部部分(22a),(
23a) と本体(22b).(23b) を貫通し、
頂部部分(22a),(23a) において、ガスレー
ザ媒質の放電部からの排出側に開口して形成されている
。ここで、上記第1の通路(28a),(28b) 側
がガイド体(22),(23) で形成される入出路(
31)の放電部に箇所に比べ、上記循環中圧力が低くな
る条件になるように形成されている。
[Embodiment] Hereinafter, an embodiment will be explained based on the drawings. FIG. 1 shows an enlarged view of a discharge portion and its vicinity in an embodiment of the present invention. That is, the holding plate (20
), (21), and on their mutually opposing surfaces there is a guide body (22) which has almost the same shape and is a molded body of fluororesin.
, (23) are provided symmetrically. Guide body (2
2) and (23) have a gentle mountain-like cross section;
As shown in FIG. 2, it is long in the tube axis direction, which is perpendicular to the plane of the paper, and the top portions (22a) and (23a) and the main body (
22b). (23b) It is formed into a divided body divided into two parts. A cathode (24) with long grooves formed in the top portions (22a) and (23a) and constituting the main discharge electrode.
and an anode (25) are buried respectively. Also,
The main bodies (22b), (23b) are provided with a plurality of pin electrodes (26a), which form one side of the pre-ionization electrodes, which are provided through the top portions (22a), (23a) at a predetermined pitch, as shown in FIG. , (26b), respectively, are buried therein. In addition, inside the main bodies (22b) and (23b), there is a first passage (28) in the form of a slit, which is slightly narrower than the width in the longitudinal direction.
a) and (28b) are formed. The first passages (28a), (28b) have large inflow ports (29a), (29b) on the inflow side of the gas laser medium into the discharge section.
is formed. In addition, the first passage (28a), (
28b) A plurality of small hole-shaped second passages (30
a) and (30b) are the top portions (22a) and (30b), respectively.
23a) and the main body (22b). (23b) through
The top portions (22a) and (23a) are formed to be open on the discharge side from the discharge section of the gas laser medium. Here, the entrance/exit path (28a), (28b) side is formed by the guide bodies (22), (23).
The discharge part 31) is formed so that the pressure during circulation is lower than that in the discharge part 31).

【0008】次に上記構成の作用について説明する。す
なわち、図示せぬ循環手段によって放電部に向かって流
されたガスレーザ媒質はガイド体(22),(23) 
に沿って入出路(30)を通過するものと、流入口(2
9a),(29b) から入って第1の通路(28a)
,(28b)に流れるものとに分かれる。第1の通路(
28a),(28b) においては流入口(29a),
(29b) が広いため内部では絞り込まれて高速に流
れ、そのため第2の通路(30a),(30b) にお
いては第1の通路(28a),(28b) 側に吸引さ
れる流れが生じる。吸引されたガスは第1の通路(28
a),(28b) を経て放電部の排出側になる循環流
路で放電部を通過したガスレーサ媒質と再び合流する。
Next, the operation of the above structure will be explained. That is, the gas laser medium flowed toward the discharge section by a circulation means (not shown) flows through the guide bodies (22), (23).
The one that passes through the inlet/outlet (30) along the inlet and the inlet (2)
9a), (29b) and the first passage (28a)
, (28b). The first passage (
28a), (28b), the inlet (29a),
Since (29b) is wide, it is narrowed inside and flows at high speed, so that in the second passages (30a) and (30b), a flow is generated that is sucked toward the first passages (28a) and (28b). The sucked gas passes through the first passage (28
a) and (28b), it joins again with the gas laser medium that has passed through the discharge section in the circulation flow path which becomes the discharge side of the discharge section.

【0009】図4は本発明の他の実施例で、上記実施例
における第1の通路に相当する部分を無くし、第2の通
路とほぼ同じような排出作用をする排出路(35a),
(35b) を形成した例である。排出路(35a),
(35b)は陰極(24), 陽極(25)側が小径に
形成され、排出側にいくに従って拡大した流路にないる
。この実施例においても排出路(35a),(35b)
 が負圧となり、上記実施例と同様にガスレーザ媒質の
排出作用が生じる。
FIG. 4 shows another embodiment of the present invention, in which the part corresponding to the first passage in the above embodiment is eliminated, and a discharge passage (35a) having almost the same discharge function as the second passage,
(35b) This is an example in which the following is formed. Discharge path (35a),
(35b) is formed to have a small diameter on the cathode (24) and anode (25) sides, and is in a flow path that expands toward the discharge side. Also in this embodiment, the discharge passages (35a), (35b)
becomes a negative pressure, and the gas laser medium is discharged similarly to the above embodiment.

【0010】0010

【発明の効果】以上説明したように、陰極(24), 
陽極(25)間の放電によって生じ、ガスレーザ媒質の
排出側になるこれら電極の近傍に滞留している放電生成
物や負イオンがガスレーザ媒質の一部とともに瞬時に第
2の通路(30a),(30b) もしくは排出路(3
5a),(35b) に吸引されガイド体で形成される
入出路を流れるガスレーザ媒質と合流するので、特にガ
ス流速を高速にすることなく、放電部を通過するガスレ
ーザの排出側に発生するアーク放電の放電原因を除去す
ることができた。その結果、安定したパルス放電の高繰
返し化が可能となり、レーザ出力を高めることができた
[Effect of the invention] As explained above, the cathode (24),
Discharge products and negative ions generated by the discharge between the anodes (25) and staying in the vicinity of these electrodes on the discharge side of the gas laser medium instantly flow into the second path (30a), ( 30b) or discharge channel (3
5a), (35b) and merges with the gas laser medium flowing through the inlet/outlet path formed by the guide body, the arc discharge generated on the discharge side of the gas laser passing through the discharge part can be avoided without particularly increasing the gas flow velocity. We were able to eliminate the cause of the discharge. As a result, it became possible to achieve a high repetition rate of stable pulse discharge and increase the laser output.

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

【図1】本発明のー実施例を示す要部の断面図である。FIG. 1 is a sectional view of essential parts showing an embodiment of the present invention.

【図2】同じく本発明のー実施例を示す要部の平面図で
ある。
FIG. 2 is a plan view of essential parts showing an embodiment of the present invention.

【図3】同じく本発明のー実施例を示す要部の断面図で
ある。
FIG. 3 is a sectional view of a main part showing an embodiment of the present invention.

【図4】本発明の他の実施例を示す断面図である。FIG. 4 is a sectional view showing another embodiment of the present invention.

【図5】従来例を示す断面図である。FIG. 5 is a sectional view showing a conventional example.

【符号の説明】[Explanation of symbols]

(22),(23) …ガイド体、(24)…陰極、(
25)…陽極、(28a),(28b) …第1の通路
(排出路)、(30a),(30b) …第2の通路(
排出路)、(31)…入出路。
(22), (23)...Guide body, (24)...Cathode, (
25)...Anode, (28a), (28b)...First passage (exhaust passage), (30a), (30b)...Second passage (
(discharge path), (31)...input/output path.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】  ガスレーザ媒質を所定の圧力で封入し
た気密容器と、この気密容器内に主放電空間を形成して
設けられた少なくとも一対の主放電電極と、上記ガスレ
ーザ媒質を上記気密容器内で循環させる循環手段と、循
環されたガスレーザ媒質を上記主放電電極の間に導き排
出する入出路を形成するガイド体と、上記主放電電極に
おける上記ガスレーザ媒質の排出側近傍になる入出路か
ら排出方向に向けられて分岐するとともに上記循環に合
流するように形成された排出路とを備えたことを特徴と
するガスレーザ発振装置。
1. An airtight container in which a gas laser medium is sealed at a predetermined pressure, at least a pair of main discharge electrodes provided to form a main discharge space within the airtight container, and the gas laser medium is enclosed within the airtight container. a circulation means for circulating; a guide body forming an input/output path for guiding and discharging the gas laser medium that has been circulated between the main discharge electrodes; A gas laser oscillation device comprising: a discharge path formed to branch toward the circulation and join the circulation.
JP4714891A 1991-03-13 1991-03-13 Gas laser oscillation device Expired - Fee Related JP3065681B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4714891A JP3065681B2 (en) 1991-03-13 1991-03-13 Gas laser oscillation device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4714891A JP3065681B2 (en) 1991-03-13 1991-03-13 Gas laser oscillation device

Publications (2)

Publication Number Publication Date
JPH04283976A true JPH04283976A (en) 1992-10-08
JP3065681B2 JP3065681B2 (en) 2000-07-17

Family

ID=12767017

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4714891A Expired - Fee Related JP3065681B2 (en) 1991-03-13 1991-03-13 Gas laser oscillation device

Country Status (1)

Country Link
JP (1) JP3065681B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP1039592A1 (en) * 1999-03-23 2000-09-27 Cinema Magnetique Communication ( C.M.C.) Method and device for the excitation of a high frequency electric discharge in a gas laser

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP1039592A1 (en) * 1999-03-23 2000-09-27 Cinema Magnetique Communication ( C.M.C.) Method and device for the excitation of a high frequency electric discharge in a gas laser

Also Published As

Publication number Publication date
JP3065681B2 (en) 2000-07-17

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