JP2598007B2 - Pulse gas laser device - Google Patents
Pulse gas laser deviceInfo
- Publication number
- JP2598007B2 JP2598007B2 JP62012712A JP1271287A JP2598007B2 JP 2598007 B2 JP2598007 B2 JP 2598007B2 JP 62012712 A JP62012712 A JP 62012712A JP 1271287 A JP1271287 A JP 1271287A JP 2598007 B2 JP2598007 B2 JP 2598007B2
- Authority
- JP
- Japan
- Prior art keywords
- main discharge
- electrodes
- discharge electrode
- gas laser
- laser medium
- 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.)
- Expired - Lifetime
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES 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
- H01S3/00—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
- H01S3/02—Constructional details
- H01S3/03—Constructional details of gas laser discharge tubes
- H01S3/038—Electrodes, 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)
Description
【発明の詳細な説明】 [発明の目的] (産業上の利用分野) 本発明は横励起形のパルスガスレーザ装置に関する。DETAILED DESCRIPTION OF THE INVENTION [Purpose of the Invention] (Industrial application field) The present invention relates to a laterally pumped pulse gas laser device.
(従来の技術) 第5図はパルスガスレーザ装置としてのエキシマレー
ザ装置の断面構成図であって、外側円筒容器1および内
側円筒容器2を有し、これら容器1、2の間にパルスレ
ーザ光を発生する放電部3、熱交換器4および送風機5
が備えられている。これにより、各容器1、2の間に封
入されたガスレーザ媒質が放電部3に流れて熱を吸収す
ると、熱交換器4において冷却されて送風機5で再び放
電部3に送られている。ところで、放電部3は第6図お
よび第7図に示す如く長方形状の一対の主放電電極6、
7(すなわち第1の主放電電極6、第2の主放電電極
7)が対向配置されるとともにこれら主放電電極6、7
の長手方向に沿って円柱状の予備電離用電極(以下、予
備電極と省略する)8〜17がそれぞれ対向配置されてい
る。なお、第7図は主放電電極6側から見た主放電電極
7側の配置構成を示している。また各予備電極8〜17の
一方の電極はピーキングコンデンサ18、19を通して主放
電電極6と電気的に接続されている。(Prior Art) FIG. 5 is a cross-sectional view of an excimer laser device as a pulse gas laser device, which has an outer cylindrical container 1 and an inner cylindrical container 2, and applies a pulse laser beam between these containers 1 and 2. Discharge part 3, heat exchanger 4 and blower 5 generated
Is provided. Thereby, when the gas laser medium enclosed between the containers 1 and 2 flows into the discharge unit 3 and absorbs heat, it is cooled in the heat exchanger 4 and sent to the discharge unit 3 again by the blower 5. By the way, as shown in FIGS. 6 and 7, the discharge portion 3 has a pair of rectangular main discharge electrodes 6,
7 (i.e., the first main discharge electrode 6 and the second main discharge electrode 7) are opposed to each other, and the main discharge electrodes 6, 7
Are arranged opposite to each other along the longitudinal direction of the column. FIG. 7 shows the arrangement on the main discharge electrode 7 side as viewed from the main discharge electrode 6 side. One of the spare electrodes 8 to 17 is electrically connected to the main discharge electrode 6 through peaking capacitors 18 and 19.
このような構成で放電部3に高圧電源20からパルス高
電圧(20〜50kV)が印加されると、各予備電極8〜17間
にアーク放電が発生して紫外線が放出される。これによ
り、主放電電極6、7の間が予備電離され、この後、主
放電電極6、7の間で主放電が発生する。かくして、主
放電電極6、7の長手方向側に配置された共振器(不図
示)の間にパルスレーザ光が誘起される。When a pulse high voltage (20 to 50 kV) is applied from the high voltage power supply 20 to the discharge unit 3 in such a configuration, an arc discharge occurs between the spare electrodes 8 to 17 and ultraviolet rays are emitted. As a result, preliminary ionization occurs between the main discharge electrodes 6 and 7, and thereafter, a main discharge occurs between the main discharge electrodes 6 and 7. Thus, a pulsed laser beam is induced between the resonators (not shown) arranged on the longitudinal sides of the main discharge electrodes 6 and 7.
ところが、以上のような構成のレーザ装置ではパルス
繰返し数を次第に高くすると、レーザ光出力がそれほど
高くない繰返し数で飽和状態となる。この原因は次の通
りである。放電部3にはガスレーザ媒質が送風機5によ
って高速に流されているが、このガスレーザ媒質は放電
部3,特に主放電電極6、7の間で一様な状態で流れるこ
とが要求される。ところが、ガスレーザ媒質の流れは第
7図に示すように各予備電極8〜17の形状が円柱状とな
っているためにガスレーザ媒質の流れの抵抗となって流
速を低下させたり、また粗密を生じさせたりしている。
このため、主放電が主放電電極6、7の間で一様に発生
することが阻害され、逆にアーク放電の発生の確率が高
くなる。従って、パルス繰返し数が高くなるに従って主
放電電極6、7間のガスレーザ媒質が一様な状態となら
ずにレーザ光出力が飽和状態となってしまう。However, when the pulse repetition rate is gradually increased in the laser device having the above-described configuration, the laser light output is saturated at a repetition rate that is not so high. The cause is as follows. The gas laser medium is passed through the discharge section 3 at a high speed by the blower 5, and the gas laser medium is required to flow in a uniform state between the discharge section 3, particularly between the main discharge electrodes 6 and 7. However, the flow of the gas laser medium, as shown in FIG. 7, has a columnar shape of each of the spare electrodes 8 to 17, which causes a resistance of the flow of the gas laser medium to reduce the flow velocity and to cause the density of the gas laser medium. Or let me do it.
For this reason, the main discharge is prevented from being uniformly generated between the main discharge electrodes 6 and 7, and conversely, the probability of occurrence of arc discharge is increased. Therefore, as the pulse repetition rate increases, the gas laser medium between the main discharge electrodes 6 and 7 does not become uniform, and the laser light output becomes saturated.
(発明が解決しようとする問題点) 以上のようにパルス繰返し数が高くなる前にレーザ光
出力が飽和状態となり十分に高いパルス繰返し数のパル
スガスレーザ光を得ることができなかった。(Problems to be Solved by the Invention) As described above, the laser beam output became saturated before the pulse repetition rate was increased, and it was not possible to obtain a pulse gas laser beam having a sufficiently high pulse repetition rate.
そこで本発明は、高いパルス繰返し数が得られるパル
スガスレーザ装置を提供することを目的とする。Therefore, an object of the present invention is to provide a pulse gas laser device capable of obtaining a high pulse repetition rate.
[発明の構成] (問題点を解決するための手段) 本発明は、ガスレーザ媒質の流れる放電容器内に第1
の主放電電極と第2の主放電電極とを対向配置するとと
もにこれらの主放電電極の長手方向に沿って予備電離を
発生するための複数の予備電極を配置して成るパルスガ
スレーザ装置において、 複数の予備電極は、平板状に形成され、この平板状の
板面を前記ガスレーザ媒質の流れ方向と同一方向に配置
し、かつそれぞれの先端部を前記第1の主放電電極と第
2の主放電電極との各対向面の位置よりも内側に突出さ
せて配置するとともに、これら第1の主放電電極側から
突出した予備電極と第2の主放電電極から突出した予備
電極とが第1の主放電電極及び前記第2の主放電電極の
長手方向から見て重なり合うように交互に配置したパル
スガスレーザ装置である。[Structure of the Invention] (Means for Solving the Problems) The present invention provides a first container in a discharge vessel in which a gas laser medium flows.
A pulse gas laser device comprising a main discharge electrode and a second main discharge electrode arranged opposite to each other and a plurality of preliminary electrodes for generating preionization along the longitudinal direction of the main discharge electrodes. Are formed in the shape of a flat plate, the flat plate surface is arranged in the same direction as the flow direction of the gas laser medium, and the respective tips are connected to the first main discharge electrode and the second main discharge electrode. The auxiliary electrode protruding from the first main discharge electrode side and the auxiliary electrode protruding from the second main discharge electrode are arranged so as to protrude inward from the position of each opposing surface with the electrode. A pulse gas laser device which is arranged alternately so as to overlap when viewed from the longitudinal direction of the discharge electrode and the second main discharge electrode.
(作用) このようなパルスガスレーザ装置であれば、ガスレー
ザ媒質が主放電電極間に一様に流れ、これら主放電電極
間に均一な主放電を発生することができる。これによっ
て、主放電電極間を狭くできるとともに装置自体をコン
パクト化できる。(Operation) With such a pulse gas laser device, the gas laser medium flows uniformly between the main discharge electrodes, and a uniform main discharge can be generated between these main discharge electrodes. Thereby, the space between the main discharge electrodes can be narrowed and the device itself can be made compact.
(実施例) 以下、本発明の一実施例について図面を参照して説明
する。なお、図5と同一部分には同一符号を付してその
詳しい説明は省略する。Hereinafter, an embodiment of the present invention will be described with reference to the drawings. The same parts as those in FIG. 5 are denoted by the same reference numerals, and detailed description thereof will be omitted.
第1図はパルスガスレーザ装置の断面構成図であり、
第2図は予備電極の配置図、第3図は予備電極の上方か
ら見た配置図である。FIG. 1 is a sectional configuration diagram of a pulse gas laser device,
FIG. 2 is a layout view of the spare electrode, and FIG. 3 is a layout view of the spare electrode as viewed from above.
各予備電極40〜48は、その横断面形状が流線形などの
平板状に形成され、この平板状の板面をガスレーザ媒質
の流れ方向と同一方向に配置されている。Each of the preliminary electrodes 40 to 48 is formed in a flat plate shape having a cross-sectional shape such as streamline, and the flat plate surface is arranged in the same direction as the flow direction of the gas laser medium.
又、これら予備電極40〜48の各先端部は、第1の主放
電電極6と第2の主放電電極6との各対向面の位置より
も内側に突出させて配置するとともに、これら第1の主
放電電極6側から突出した予備電極40、42、44、46と第
2の主放電電極7側から突出した予備電極41、43、45と
が各主放電電極6、7の長手方向から見て重なり合うよ
うに交互に配置されている。Further, each of the tips of the spare electrodes 40 to 48 is disposed so as to protrude inward from the position of each of the opposing surfaces of the first main discharge electrode 6 and the second main discharge electrode 6, and the first The preliminary electrodes 40, 42, 44, 46 projecting from the main discharge electrode 6 side and the preliminary electrodes 41, 43, 45 projecting from the second main discharge electrode 7 side are arranged in the longitudinal direction of each main discharge electrode 6, 7. They are arranged alternately so as to overlap when viewed.
このような構成であれば、高速で流れるカスレーザ媒
質は各予備電極40〜48間を通過しても一様な状態で各主
放電電極6、7の間に流れる。With such a configuration, the cas laser medium flowing at high speed flows between the main discharge electrodes 6 and 7 in a uniform state even when passing between the preliminary electrodes 40 to 48.
このような状態で高圧電源20から高圧のパルス電圧が
放電部に印加されると、各予備電極40〜48間でアーク放
電が発生して各主放電電極6、7の間の空間が、各主放
電電極6、7の長手方向において均一に予備電離され
る。When a high-voltage pulse voltage is applied to the discharge unit from the high-voltage power supply 20 in such a state, arc discharge occurs between the spare electrodes 40 to 48, and the space between the main discharge electrodes 6 and 7 becomes Pre-ionization is uniformly performed in the longitudinal direction of the main discharge electrodes 6 and 7.
この後、各主放電電極6、7の間で上記予備電離から
成長して主放電が一様に発生し、共振器(不図示)での
間でパルスレーザ光が誘起される。After that, the main discharges grow between the main discharge electrodes 6 and 7 from the preionization and the main discharge is uniformly generated, and a pulse laser beam is induced between the resonators (not shown).
このように上記一実施例においては、各予備電極40〜
48の先端位置の配置向きを主放電電極6、7の長手方向
に沿って交互に逆方向に変え、かつこれら予備電極40〜
48の先端位置を主放電電極6、7の長手方向から見て交
わるように配置したので、主放電電極6、7の間の空間
に、主放電電極6、7の長手方向において均一に予備電
離ができ、主放電を一様に発生でき、これによって、主
放電電極6、7間を狭くできるとともに装置自体をコン
パクト化できる。Thus, in the above embodiment, each of the spare electrodes 40 to
The arrangement direction of the tip positions of 48 is alternately changed in the opposite direction along the longitudinal direction of the main discharge electrodes 6 and 7, and these auxiliary electrodes 40 to
48 are arranged so as to intersect with each other when viewed from the longitudinal direction of the main discharge electrodes 6 and 7, so that the space between the main discharge electrodes 6 and 7 is uniformly pre-ionized in the longitudinal direction of the main discharge electrodes 6 and 7. Thus, the main discharge can be uniformly generated, whereby the space between the main discharge electrodes 6 and 7 can be narrowed and the device itself can be made compact.
すなわち、主放電電極6、7の間を流れるガスレーザ
媒質の流速の損失による低下が小さくかつ流速分布の乱
れが少ない一様な状態で流れる。しかもガスレーザ媒質
の流速をそれ程高速としなくても主放電電極6、7間の
ガスレーザ媒質を新しいものと直ぐに入れ替えできる。That is, the gas laser medium flowing between the main discharge electrodes 6 and 7 flows in a uniform state with a small decrease due to the loss of the flow velocity and with little disturbance of the flow velocity distribution. Moreover, the gas laser medium between the main discharge electrodes 6 and 7 can be immediately replaced with a new one without setting the flow velocity of the gas laser medium so high.
従って、アーク放電の発生確率が非常に小さくなると
ともに主放電電極6、7間で均一な放電が発生できる。
かくして、第4図に示すごとくパルス繰り返し数が高く
なってもガスレーザ媒質の流れは均一状態を保って安定
した状態でパルスレーザ光が発生できる。Accordingly, the probability of occurrence of arc discharge is extremely reduced, and uniform discharge can be generated between the main discharge electrodes 6 and 7.
Thus, as shown in FIG. 4, even when the pulse repetition rate is increased, the flow of the gas laser medium can be maintained in a uniform state and the pulse laser beam can be generated in a stable state.
なお、予備電極40〜48は、比較的表面積が大きいため
高速繰り返し数において先端部での発熱量が大きくなる
が、高速のガスレーザ媒質の流れによって確実に冷却で
きる。これにより、各予備電極40〜48が高温になり溶け
落ちることはない。The spare electrodes 40 to 48 have a relatively large surface area, so that the amount of heat generated at the tip portion increases at a high repetition rate. Thereby, each of the spare electrodes 40 to 48 is heated to a high temperature and does not melt off.
なお、本発明は、エキシマレーザの他にTEACO2レーザ
や高気圧封入TEACO2レーザに適用できることは言うまで
もない。It is needless to say that the present invention can be applied to a TEACO 2 laser and a high-pressure sealed TEACO 2 laser in addition to the excimer laser.
[発明の効果] 以上詳記したように本発明によれば、ガスレーザ媒質
の流速の損失による低下が小さくかつ流速分布の乱れが
少ない一様な状態でガスレーザ媒質が流れて均一な主放
電が発生でき、かつ主放電に先立って主放電電極の長手
方向において均一に予備電離ができ、そのうえガスレー
ザ媒質の流速をそれ程高速としなくても主放電電極間の
ガスレーザ媒質を新しいものと直ぐに入れ替えでき、さ
らに主放電電極間を狭くできるとともに装置自体をコン
パクト化でき、高いパルス繰り返し数が得られるパルス
ガスレーザ装置を提供できる。[Effects of the Invention] As described above in detail, according to the present invention, the gas laser medium flows in a uniform state with a small decrease due to the loss of the flow velocity of the gas laser medium and a small disturbance in the flow velocity distribution, thereby generating a uniform main discharge. Can be pre-ionized uniformly in the longitudinal direction of the main discharge electrode prior to the main discharge, and furthermore, the gas laser medium between the main discharge electrodes can be immediately replaced with a new one without having to make the flow rate of the gas laser medium so high. It is possible to provide a pulse gas laser device that can make the space between the main discharge electrodes narrow and can make the device itself compact, and can obtain a high pulse repetition rate.
第1図はパルスガスレーザ装置の断面構成図、第2図は
同装置の予備電極の配置図、第3図は同装置の予備電極
の上方から見た配置図、第4図は同装置のパルス繰り返
し数を示す図、第5図乃至第7図は従来装置の構成図で
ある。 1……外側円筒容器、2……外側円筒容器、6、7……
主放電電極、10,11……ピーキングコンデンサ、20……
高圧電源、40〜48……予備電極。FIG. 1 is a cross-sectional view of the pulse gas laser device, FIG. 2 is a layout diagram of spare electrodes of the device, FIG. 3 is a layout diagram of the device viewed from above the spare electrodes, and FIG. FIG. 5 to FIG. 7 show the number of repetitions, and FIG. 1 ... outer cylindrical container, 2 ... outer cylindrical container, 6, 7 ...
Main discharge electrode, 10,11 …… peaking capacitor, 20 ……
High voltage power supply, 40-48 …… A spare electrode.
Claims (1)
の主放電電極と第2の主放電電極とを対向配置するとと
もにこれらの主放電電極の長手方向に沿って予備電離を
発生するための複数の予備電極を配置して成るパルスガ
スレーザ装置において、 前記複数の予備電極は、平板状に形成され、この平板状
の板面を前記ガスレーザ媒質の流れ方向と同一方向に配
置し、かつそれぞれの先端部を前記第1の主放電電極と
前記第2の主放電電極との各対向面の位置よりも内側に
突出させて配置するとともに、これら第1の主放電電極
側から突出した前記予備電極と前記第2の主放電電極側
から突出した前記予備電極とが前記第1の主放電電極及
び前記第2の主放電電極の長手方向から見て重なり合う
ように交互に配置したことを特徴とするパルスガスレー
ザ装置。1. A first container in a discharge vessel in which a gas laser medium flows.
Wherein the main discharge electrode and the second main discharge electrode are arranged to face each other and a plurality of preliminary electrodes for generating preliminary ionization are arranged along the longitudinal direction of these main discharge electrodes. The plurality of spare electrodes are formed in a flat plate shape, the flat plate surface is arranged in the same direction as the flow direction of the gas laser medium, and the respective tips are formed by the first main discharge electrode and the second main discharge electrode. The auxiliary electrodes protruding from the first main discharge electrode side and the auxiliary electrodes protruding from the second main discharge electrode side are arranged so as to protrude inward from the positions of the respective opposing surfaces with the main discharge electrode. Wherein the first main discharge electrode and the second main discharge electrode are alternately arranged so as to overlap when viewed from the longitudinal direction.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP62012712A JP2598007B2 (en) | 1987-01-22 | 1987-01-22 | Pulse gas laser device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP62012712A JP2598007B2 (en) | 1987-01-22 | 1987-01-22 | Pulse gas laser device |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS63181387A JPS63181387A (en) | 1988-07-26 |
JP2598007B2 true JP2598007B2 (en) | 1997-04-09 |
Family
ID=11813035
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP62012712A Expired - Lifetime JP2598007B2 (en) | 1987-01-22 | 1987-01-22 | Pulse gas laser device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JP2598007B2 (en) |
Families Citing this family (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH01191486A (en) * | 1988-01-27 | 1989-08-01 | Komatsu Ltd | Reserve ionizing electrode of laser |
JP2718623B2 (en) * | 1993-10-14 | 1998-02-25 | 浜松ホトニクス株式会社 | Gas laser device |
Family Cites Families (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6371562U (en) * | 1986-10-29 | 1988-05-13 |
-
1987
- 1987-01-22 JP JP62012712A patent/JP2598007B2/en not_active Expired - Lifetime
Also Published As
Publication number | Publication date |
---|---|
JPS63181387A (en) | 1988-07-26 |
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