JPS63229875A - Excimer laser device - Google Patents

Excimer laser device

Info

Publication number
JPS63229875A
JPS63229875A JP6492487A JP6492487A JPS63229875A JP S63229875 A JPS63229875 A JP S63229875A JP 6492487 A JP6492487 A JP 6492487A JP 6492487 A JP6492487 A JP 6492487A JP S63229875 A JPS63229875 A JP S63229875A
Authority
JP
Japan
Prior art keywords
laser
laser beam
oscillation
stage
mirror
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
JP6492487A
Other languages
Japanese (ja)
Other versions
JP2673510B2 (en
Inventor
Yasuo Itakura
板倉 康夫
Noriaki Itou
伊藤 仙聡
Junichi Fujimoto
准一 藤本
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.)
Komatsu Ltd
Original Assignee
Komatsu Ltd
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 Komatsu Ltd filed Critical Komatsu Ltd
Priority to JP62064924A priority Critical patent/JP2673510B2/en
Publication of JPS63229875A publication Critical patent/JPS63229875A/en
Application granted granted Critical
Publication of JP2673510B2 publication Critical patent/JP2673510B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime 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

Landscapes

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

Abstract

PURPOSE:To output a high-energy laser beam by using a simplified structure without synchronous control by a method wherein laser oscillation is initiated on a discharge electrode common to an oscillation stage and amplification stage and thereafter the output is amplified in an optical resonance element. CONSTITUTION:A laser beam induced by an arc discharge between discharge electrodes 9a and 9b is thrown into resonance by an etalon 4 and mirrors 5 and 10, and the resultant laser beam is amplified by a spherical mirror 13 and front mirror 14 before being outputted.

Description

【発明の詳細な説明】 〔産業上の利用分野) 本発明はエキシマレーザ装置に関するものである。[Detailed description of the invention] [Industrial application field] The present invention relates to an excimer laser device.

〔従来の技術〕[Conventional technology]

KrFなどの気体をレーザ物質として用いるエキシマレ
ーザ装置においては、第5図に示すように、発振段のレ
ーザ管1と増幅段のレーザ管2を設け、発振段の放電電
極3aと3bとの間に)(rFなどの気体を図示の矢印
方向に環流させながら放?1113aと3b間のアーク
放電によってレーザ光を誘起し、そのレーザ光をリアミ
ラー5.フロントミラー6、およびエタロン4などの光
学共振素子で共振させ、ミラー7.8によってその光路
を曲げてm@段のレーザf!2内に導き、放電電極9a
、9bとの間のアーク放電によって発振段からのレーザ
光を増幅し、ミラー10とリアミラー11とによって共
振させて外部に出力するように構成したものがある。
In an excimer laser device that uses a gas such as KrF as a laser substance, as shown in FIG. 2) (While circulating gas such as rF in the direction of the arrow shown in the figure, a laser beam is induced by an arc discharge between the radiator 1113a and 3b, and the laser beam is transmitted to the optical resonance of the rear mirror 5, front mirror 6, etalon 4, etc.) The element resonates, and the optical path is bent by the mirror 7.8 and guided into the m@stage laser f!2, and the discharge electrode 9a
, 9b, the laser beam from the oscillation stage is amplified by arc discharge, and the laser beam is resonated by the mirror 10 and rear mirror 11 and output to the outside.

この構成は大きなパワーを持つレーザ光を必要とする時
に多用されるもので、注入同期法と呼ばれている。
This configuration is often used when a laser beam with high power is required, and is called injection locking.

この注入同期法を利用したエキシマレーザ装置としては
、第5図の構成の他に、第6図に示すように発振段の放
電電極3bと増幅段の放電電極9aとを共通化し、第5
図に示したのと同様にしてレーザ発振を行うように構成
したものもある。
As an excimer laser device using this injection locking method, in addition to the configuration shown in FIG. 5, as shown in FIG.
Some devices are configured to perform laser oscillation in the same manner as shown in the figure.

なお、第6図に示す構成においても第5図の構成と同様
に発振段と増幅段の気体は別々に環流するように構成さ
れている。
Note that in the configuration shown in FIG. 6 as well, the gases in the oscillation stage and the amplification stage are configured to circulate separately, similar to the configuration in FIG.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

ところが、第5図および第6図の構成では、発振段と増
幅段のレーザ発振を放電電極3a、3bと9a、9bの
2つの放電回路中で行うため、2つのレーザ管を必要と
する他、発振段と増幅段での発振に同期関係を持たゼな
ければならず、その制御回路が複雑になるという問題が
ある。
However, in the configurations shown in FIGS. 5 and 6, since the laser oscillations in the oscillation stage and the amplification stage are performed in two discharge circuits of the discharge electrodes 3a, 3b and 9a, 9b, two laser tubes are required. However, there is a problem in that the oscillations in the oscillation stage and the amplification stage must be synchronized, which makes the control circuit complicated.

本発明の目的は、簡単な構成でパワーの大きいレーザ光
を取出すことができるエキシマレーザ装置を提供するこ
とにある。
SUMMARY OF THE INVENTION An object of the present invention is to provide an excimer laser device that has a simple configuration and can extract a high-power laser beam.

〔問題点を解決するための手段〕[Means for solving problems]

本発明は、発振段と増幅段のレーザ発振を同一レーザ管
内の同一放電回路中で行うように光学バ振素子を配置し
たものである。
In the present invention, optical vibration elements are arranged so that the laser oscillations of the oscillation stage and the amplification stage are performed in the same discharge circuit within the same laser tube.

〔作用〕[Effect]

発振段と増幅段に共通の放電電極によって発振段のレー
ザ発振が開始され、その出力がミラーなどの光学共振素
子によって増幅段に導かれ、ここで増幅されて出力され
る。
Laser oscillation in the oscillation stage is started by a discharge electrode common to the oscillation stage and the amplification stage, and its output is guided to the amplification stage by an optical resonant element such as a mirror, where it is amplified and output.

〔実施例] 第1図は本発明の第1の実施例を示す断面構成図であり
、レーザ管の内部には敢雷電ff19aと9bが対向配
置され、これら電極間にはKrFなどの気体が環流され
ている。
[Embodiment] FIG. 1 is a cross-sectional configuration diagram showing a first embodiment of the present invention. Inside the laser tube, a pair of thunderbolts ff19a and 9b are arranged facing each other, and a gas such as KrF is placed between these electrodes. It is circulating.

2つの放電電極9a、9bのうち9bに近いレーザ管の
端部にはエタロン4とミラー5.10が一直線状に配置
され、これらエタロン4およびミラー5,10によって
発振段のレーザ光を発振させるように構成されている。
An etalon 4 and a mirror 5.10 are arranged in a straight line at the end of the laser tube near 9b of the two discharge electrodes 9a and 9b, and the etalon 4 and mirrors 5 and 10 oscillate the laser beam of the oscillation stage. It is configured as follows.

ここで、ミラー10はその中心軸が傾斜して取付けられ
ており、ミラー5.10とエタロン4で発振さゼたレー
ザ光を増幅段の球面ミラー13に入射し、この球面ミラ
ー13とフロントミラー14との間で増幅させるように
構成されている。
Here, the mirror 10 is installed with its central axis inclined, and the laser beam oscillated by the mirror 5.10 and the etalon 4 is incident on the spherical mirror 13 of the amplification stage, and the spherical mirror 13 and the front mirror 14.

この構成においては、放電電極9aと9bのアーク放電
によって誘起したレーザ光をエタロン4゜ミラー5,1
0によって共振させることにより、この共振によって発
生されたレーザ光は球面ミラー13とフロントミラー1
4によって増幅されて出力される。
In this configuration, the laser beam induced by the arc discharge of the discharge electrodes 9a and 9b is transmitted to the etalon 4° mirrors 5 and 1.
0, the laser beam generated by this resonance is transmitted to the spherical mirror 13 and the front mirror 1.
4 and output.

すなわち、同一の放電回路中で発振段と増幅段のレーザ
発振を行うことができる。この結果、レーザ管は1個の
みでよくなり、また同期制御も行う必要がなくなる。ま
た、同一放電回路中を2つのレーザ光が通過するので、
放M領域を有効に活用することができる。
That is, laser oscillation can be performed in the oscillation stage and the amplification stage in the same discharge circuit. As a result, only one laser tube is required, and there is no need for synchronous control. Also, since two laser beams pass through the same discharge circuit,
The emission area can be effectively utilized.

この場合、第2図の第2の実施例の構成に示すように、
プロアポンプ1:6を有する補機15を設け、レーザ管
内の気体をプロアポンプ16によって配管17を介して
矢印方向に強制環流させるようにし、かつ放電電極9a
にその気体流を通過させる多数のスリット(図示せず)
を設けるようにしてもよい。
In this case, as shown in the configuration of the second embodiment in FIG.
An auxiliary machine 15 having a proa pump 1:6 is provided so that the gas in the laser tube is forced to circulate in the direction of the arrow through the pipe 17 by the proa pump 16, and the discharge electrode 9a
a number of slits (not shown) that allow the gas flow to pass through the
may be provided.

第3図は本光明の第3の実施例を示す断面構成図であり
、発振段のレーザ光の光路Xおよび発振段から増幅段へ
の入射光路Y、さらに増幅段の光路Zが第3図(b)に
示す第3図(a)のA−A断面図に示すように別々の光
路となるように、ミラー5および10.エタロン42球
面ミラー13を配置したものである。
FIG. 3 is a cross-sectional configuration diagram showing a third embodiment of the present invention. Mirrors 5 and 10. An etalon 42 and a spherical mirror 13 are arranged.

この構成においても第1図の実施例と同様な効果を得る
ことができたうえ、放電電極9aと、9b′間のギャッ
プをさらに小さくすることができる。
In this configuration as well, the same effects as in the embodiment shown in FIG. 1 can be obtained, and the gap between the discharge electrodes 9a and 9b' can be further reduced.

また、第4図の第4の実施例の構成に示すように気体の
強制環流を行なわせる補IF115を組合せることもで
きる。
Furthermore, as shown in the configuration of the fourth embodiment shown in FIG. 4, an auxiliary IF 115 for forced gas circulation may be combined.

(発明の効果〕 以上のように本発明によれば、1つのレーザ管のみの簡
単な構成で、かつ同期制御を行うことなくパワーの大き
いレーザ光を取出すことができる。
(Effects of the Invention) As described above, according to the present invention, a high-power laser beam can be extracted with a simple configuration of only one laser tube and without performing synchronous control.

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

第1図は本発明の第1の実施例を示す断面構成図、第2
図〜第4図は第2〜第4の実施例を示す断面構成図、第
5図は従来の1キシマレーザ装置の第1の例を示す断面
構成図、第6図は従来の1キシマレーザ装置の第2の例
を示す断面構成図である。 1.2・・・レーザ管、4・・・エタロン、5,10・
・・ミラー、9a、9b・・・放電電極、13・・・球
面ミラ−11499,フロントミラー、15・・・補■
、16・°゛ブロアポンプ 第1図・ fベ ロ 第2図
FIG. 1 is a cross-sectional configuration diagram showing the first embodiment of the present invention, and FIG.
4 are cross-sectional configuration diagrams showing second to fourth embodiments, FIG. 5 is a cross-sectional configuration diagram showing a first example of a conventional 1-ximer laser device, and FIG. 6 is a sectional configuration diagram of a conventional 1-ximer laser device. FIG. 7 is a cross-sectional configuration diagram showing a second example. 1.2...Laser tube, 4...Etalon, 5,10.
...Mirror, 9a, 9b...Discharge electrode, 13...Spherical mirror 11499, front mirror, 15...Supplementary ■
, 16・°゛Blower pump Fig. 1・F tongue Fig. 2

Claims (1)

【特許請求の範囲】 発振段と増幅段との2つのレーザ管を有し、発振段で発
振されたレーザ光を増幅段で増幅して出力するエキシマ
レーザ装置において、 発振段と増幅段のレーザ発振を同一レーザ管内の同一放
電回路中で行うように光学共振素子を配置して成るエキ
シマレーザ装置。
[Scope of Claims] An excimer laser device having two laser tubes, an oscillation stage and an amplification stage, in which a laser beam oscillated by the oscillation stage is amplified and outputted by the amplification stage, comprising: An excimer laser device in which optical resonant elements are arranged so that oscillation occurs in the same discharge circuit within the same laser tube.
JP62064924A 1987-03-19 1987-03-19 Excimer laser device Expired - Lifetime JP2673510B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62064924A JP2673510B2 (en) 1987-03-19 1987-03-19 Excimer laser device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62064924A JP2673510B2 (en) 1987-03-19 1987-03-19 Excimer laser device

Publications (2)

Publication Number Publication Date
JPS63229875A true JPS63229875A (en) 1988-09-26
JP2673510B2 JP2673510B2 (en) 1997-11-05

Family

ID=13272076

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62064924A Expired - Lifetime JP2673510B2 (en) 1987-03-19 1987-03-19 Excimer laser device

Country Status (1)

Country Link
JP (1) JP2673510B2 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2010021518A (en) * 2008-06-12 2010-01-28 Komatsu Ltd Slab type laser apparatus
JP5657139B2 (en) * 2011-12-07 2015-01-21 三菱電機株式会社 CO2 laser device and CO2 laser processing device

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6181685A (en) * 1984-09-28 1986-04-25 Mitsubishi Electric Corp Laser apparatus
JPS61284981A (en) * 1985-06-06 1986-12-15 レーザー コーポレーション オブ アメリカ Gas laser unit having thermally stable optical mount base

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6181685A (en) * 1984-09-28 1986-04-25 Mitsubishi Electric Corp Laser apparatus
JPS61284981A (en) * 1985-06-06 1986-12-15 レーザー コーポレーション オブ アメリカ Gas laser unit having thermally stable optical mount base

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2010021518A (en) * 2008-06-12 2010-01-28 Komatsu Ltd Slab type laser apparatus
JP5657139B2 (en) * 2011-12-07 2015-01-21 三菱電機株式会社 CO2 laser device and CO2 laser processing device
US9059567B2 (en) 2011-12-07 2015-06-16 Mitsubishi Electric Corporation CO2 laser device and CO2 laser processing device

Also Published As

Publication number Publication date
JP2673510B2 (en) 1997-11-05

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