JPH04306891A - Gas laser oscillator - Google Patents

Gas laser oscillator

Info

Publication number
JPH04306891A
JPH04306891A JP7073291A JP7073291A JPH04306891A JP H04306891 A JPH04306891 A JP H04306891A JP 7073291 A JP7073291 A JP 7073291A JP 7073291 A JP7073291 A JP 7073291A JP H04306891 A JPH04306891 A JP H04306891A
Authority
JP
Japan
Prior art keywords
dielectrics
dielectric
discharge electrode
discharge
laser oscillator
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
JP7073291A
Other languages
Japanese (ja)
Inventor
Takaaki Murata
隆昭 村田
Kiyohisa Terai
清寿 寺井
Koichi Nishida
西田 公一
Yukihiro Mikuni
幸宏 三国
Akira Moriguchi
森口 晃
Hirokatsu Suzuki
鈴木 博勝
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 JP7073291A priority Critical patent/JPH04306891A/en
Publication of JPH04306891A publication Critical patent/JPH04306891A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To eliminate a dead space from a discharge space between discharge electrodes so as to miniaturize a gas laser oscillator by a method wherein dielectric flat plates provided with a discharge electrode are laminated. CONSTITUTION:Dielectric flat plates 11a, 11b, 12a, 12b, 13a, 12b, 14a, and 14b formed in U-shaped in cross section by bending both the ends of them are divided in the lengthwise direction and laminated in two stages. The dielectric plates 11a, 11b, 12a, 12b, 13a, 12b, 14a, and 14b are provided so as to enable them to confront each other respectively, and metal discharge electrodes 15a, 15b, 16a, 16b, 17a, 17b, 18a, and 18b formed by frame spraying are provided to the rear sides of the electric plates opposite to the confronting sides. Furthermore, the dielectrics 11a and 11b and the dielectrics 13a and 13b are separated from each other by a barrier 19, and also the dielectrics 12a and 12b and the dielectrics 14a and 14b are separated from each other by a barrier 19, whereby discharges occurring in regions are prevented from interfering with each other.

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、高周波電圧を放電電極
間に印加してレーザ光を発振させるガスレーザ発振器に
関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a gas laser oscillator that oscillates laser light by applying a high frequency voltage between discharge electrodes.

【0002】0002

【従来の技術】高周波電源を用いた従来のガスレーザ発
振器の一例を図3に示した。外部風洞1内には、内部が
外気に通じた断面U型のステンレス製またはアルミニウ
ム製の内部風洞2が設けられている。
2. Description of the Related Art An example of a conventional gas laser oscillator using a high frequency power source is shown in FIG. Inside the external wind tunnel 1, an internal wind tunnel 2 made of stainless steel or aluminum and having a U-shaped cross section and communicating with the outside air is provided.

【0003】また、外部風洞1の上部中央にはセラミッ
クなどから成る第1の誘電体3aが気密に取付けられ、
同様に前記内部風洞2の上部には、前記1の誘電体3a
と対向する位置に第2の誘電体3bが取付けられている
。そして、この第2の誘電体3bによって前記断面U型
の内部風洞2の開口部が閉じられている。さらに、前記
第1の誘電体3aの中央上面には第1の放電電極4aが
、また、前記第2の誘電体3bの中央下面には第2の放
電電極4bが取付けられている。また、前記第1の放電
電極4aは高周波電源5の片側に接続され、第2の放電
電極4bは接地された高周波電源の他側に接続されてい
る。そして、前記誘電体3a,3bの内面間で放電させ
て、紙面垂直方向にレーザ光6を発生させている。
[0003] Furthermore, a first dielectric body 3a made of ceramic or the like is airtightly attached to the center of the upper part of the external wind tunnel 1.
Similarly, in the upper part of the internal wind tunnel 2, the first dielectric 3a is
A second dielectric 3b is attached at a position opposite to. The opening of the internal wind tunnel 2 having a U-shaped cross section is closed by the second dielectric 3b. Furthermore, a first discharge electrode 4a is attached to the upper center surface of the first dielectric 3a, and a second discharge electrode 4b is attached to the lower center surface of the second dielectric 3b. Further, the first discharge electrode 4a is connected to one side of the high frequency power source 5, and the second discharge electrode 4b is connected to the other side of the grounded high frequency power source. A discharge is caused between the inner surfaces of the dielectrics 3a and 3b to generate laser light 6 in a direction perpendicular to the plane of the paper.

【0004】なお、前記外部風洞1と内部風洞2の間に
は、約60torrの圧力で封入されたレーザガスが風
洞の内部に配設された送風機7によって矢印Aのように
図中時計方向に循環され、冷却器(図示せず)によって
冷却されている。
Note that between the external wind tunnel 1 and the internal wind tunnel 2, a laser gas sealed at a pressure of about 60 torr is circulated clockwise in the figure as shown by arrow A by a blower 7 disposed inside the wind tunnel. and is cooled by a cooler (not shown).

【0005】[0005]

【発明が解決しようとする課題】しかし、従来のガスレ
ーザ発振器において、大容量化を図るために放電部を大
型化すると、放電電極間のデッドスペースがあるので、
装置自体が大型化してしまい、市場のニーズである小型
化に対応できず、極めて致命的な問題となっている。
[Problems to be Solved by the Invention] However, in conventional gas laser oscillators, when the discharge section is enlarged in order to increase the capacity, there is a dead space between the discharge electrodes.
The device itself has become large and cannot meet the market's need for miniaturization, which has become an extremely fatal problem.

【0006】そこで、本発明のガスレーザ発振器は、上
記問題点に鑑み、放電部の大型化に対しても放電電極間
のデッドスペースを有効に活用し、装置自体を大型化さ
せることなく、市場ニーズに対応したガスレーザ発振器
を提供することを目的とする。 [発明の構成]
Therefore, in view of the above-mentioned problems, the gas laser oscillator of the present invention effectively utilizes the dead space between the discharge electrodes even when the discharge section is enlarged, and meets market needs without increasing the size of the device itself. The purpose is to provide a gas laser oscillator that is compatible with the following. [Structure of the invention]

【0007】[0007]

【課題を解決するための手段】上記目的を達成するため
に、本発明のガスレーザ発振器は、所定部位に金属を溶
射して形成された放電電極を有する対向配置された誘電
体と、前記放電電極に高周波電圧を印加する高周波電源
と、前記対向配置された誘電体の間隙にレーザ媒質を送
風する送風手段と、複数のミラーを組合せて構成された
共振手段とを備え、前記対向配置された誘電体を複数段
積層することを特徴とするものである。
[Means for Solving the Problems] In order to achieve the above object, a gas laser oscillator of the present invention includes a dielectric body having a discharge electrode formed by thermally spraying metal on a predetermined portion, and a dielectric body disposed facing each other, and a high-frequency power supply that applies a high-frequency voltage to the dielectrics disposed opposite to each other; a blowing means for blowing a laser medium into a gap between the dielectrics disposed opposite to each other; and a resonance means configured by combining a plurality of mirrors; It is characterized by stacking the bodies in multiple stages.

【0008】[0008]

【作用】このように構成された本発明のガスレーザ発振
器においては、金属を溶射して形成された放電電極を有
する平板状の誘電体を複数段積層するように構成したの
で、従来存在していた放電電極間のデッドスペースが存
在せず装置の小型化が図れる。
[Function] The gas laser oscillator of the present invention constructed in this manner is constructed by stacking a plurality of flat dielectrics each having a discharge electrode formed by spraying metal, which is different from conventional gas laser oscillators. Since there is no dead space between the discharge electrodes, the device can be made smaller.

【0009】[0009]

【実施例】以下、本発明の一実施例を図面を用いて説明
する。
DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the present invention will be described below with reference to the drawings.

【0010】図1に示すように、本実施例のガスレーザ
発振器は両端部を折曲げ、断面形状をU形とした平板状
の誘電体11a,11b,12a,12b,13a,1
3b,14a,14bが長手方向に二分割され、さらに
二段に積層されている。また、誘電体11aと11b,
12aと12b,13aと13b,14aと14bとは
各々対向するように設けられ、その対向面の裏面には各
々金属を溶射して形成された放電電極15a,15b,
16a,16b,17a,17b,18a,18bを有
している。
As shown in FIG. 1, the gas laser oscillator of this embodiment has flat dielectric members 11a, 11b, 12a, 12b, 13a, 1 with bent ends and a U-shaped cross section.
3b, 14a, and 14b are divided into two in the longitudinal direction and further stacked in two stages. Moreover, the dielectrics 11a and 11b,
12a and 12b, 13a and 13b, and 14a and 14b are provided to face each other, and discharge electrodes 15a, 15b, 15a and 15b are respectively formed by spraying metal on the back surface of the opposing surface.
It has 16a, 16b, 17a, 17b, 18a, and 18b.

【0011】さらに、誘電体11a,11bと13a,
13b及び誘電体12a,12bと14a,14bとは
バリア19で仕切られており、各領域で発生する放電が
干渉しないようにされている。
Furthermore, dielectrics 11a, 11b and 13a,
13b and the dielectrics 12a, 12b and 14a, 14b are separated by a barrier 19 to prevent discharges generated in each area from interfering with each other.

【0012】このように構成された4つの各放電部には
、各々高周波電源20,21,22,23が設けられて
いる。すなわち、放電電極15aは高周波電源20の片
側に接続され、他方の放電電極15bは接地された高周
波電源20の他側に接続され、放電電極16aは高周波
電源21の片側に接続され他方の放電電極16bは接地
された高周波電源21の他側に接続され、放電電極17
a,18aは各々高周波電源22,23の片側に接続さ
れ、他方の放電電極17b,18bは各々高周波電源2
2,23の他側に接続されている。
[0012] Each of the four discharge sections configured as described above is provided with a high frequency power source 20, 21, 22, and 23, respectively. That is, the discharge electrode 15a is connected to one side of the high frequency power source 20, the other discharge electrode 15b is connected to the other side of the grounded high frequency power source 20, and the discharge electrode 16a is connected to one side of the high frequency power source 21 and the other discharge electrode 16b is connected to the other side of the grounded high frequency power source 21, and the discharge electrode 17
a, 18a are each connected to one side of the high frequency power source 22, 23, and the other discharge electrode 17b, 18b is connected to the high frequency power source 2, respectively.
2 and 23 are connected to the other side.

【0013】そして、各放電電極15a,15b間、1
6a,16b間、17a,17b間、18a,18b間
に高周波電圧を印加することにより、対向した各誘電体
11aと11b,12aと12b,13aと13b,1
4aと14bを介してグロー放電を生成し、レーザを発
生させる。また、誘電体11a,11b,13a13b
と誘電体12a,12b,14a,14bは各々同一風
洞24,25内に気密に設けられ、それらの風洞24,
25内には各々誘電体11a,13aの上部及び誘電体
12b,14bの下部に軸流ファン26,27が設けら
れ、このファン26,27によりレーザガスが各誘電体
11a,11b間12a,12b間13a,13b間1
4a,14b間に矢印A方向に循環され加熱されたガス
はファン26,27の上流にある冷却器28,29によ
り冷却される。
[0013] Between each discharge electrode 15a and 15b, 1
By applying a high frequency voltage between 6a and 16b, between 17a and 17b, and between 18a and 18b, each of the opposing dielectrics 11a and 11b, 12a and 12b, 13a and 13b, 1
A glow discharge is generated through 4a and 14b to generate a laser. In addition, dielectrics 11a, 11b, 13a13b
and dielectrics 12a, 12b, 14a, 14b are airtightly provided in the same wind tunnels 24, 25, respectively.
Axial fans 26 and 27 are provided in the upper part of the dielectric bodies 11a and 13a and the lower part of the dielectric bodies 12b and 14b, respectively, in the interior of the dielectric body 25. 1 between 13a and 13b
The heated gas circulated in the direction of arrow A between fans 26 and 14b is cooled by coolers 28 and 29 located upstream of fans 26 and 27.

【0014】なお、誘電体11a,11b間と13a,
13b間に流れるガス流方向と誘電体12a,12b間
14a,14b間に流れるガス流方向とは逆方向である
。また、各誘電体の一端部にはミラー30,31,32
,33が設けられており、ミラー30,31の光軸に対
し、ミラー32,33の光軸は45°傾けられている。
Note that between the dielectrics 11a and 11b and between the dielectrics 13a and 13a,
The direction of the gas flow between the dielectrics 12a and 12b and the direction of the gas flow between the dielectrics 12a and 12b and between the dielectrics 14a and 14b are opposite directions. Further, mirrors 30, 31, 32 are provided at one end of each dielectric.
, 33 are provided, and the optical axes of the mirrors 32 and 33 are inclined at 45 degrees with respect to the optical axes of the mirrors 30 and 31.

【0015】以上述べたように、本実施例によれば、放
電電極及び誘電体にて形成される放電部を二層構造とし
たので、装置の小型化が図れる。また、上層,下層のガ
ス流方向を逆方向としたので、ガス密度勾配によるレー
ザ光のゆがみを解消でき、さらに、上層,下層のミラー
を45°ずらし45°偏光面としたので、円偏光ユニッ
トが不要となりコストの低減及び装置の小型化が図れる
。なお、本実施例においては、放電部を二層構造とした
が、これに限定される必要はなく、三層,四層等の構造
としてもよい。
As described above, according to this embodiment, since the discharge section formed by the discharge electrode and the dielectric has a two-layer structure, the device can be made smaller. In addition, since the gas flow directions in the upper and lower layers are opposite, distortion of the laser beam due to gas density gradient can be eliminated.Furthermore, the mirrors in the upper and lower layers are shifted by 45 degrees to create a 45 degree polarization plane, so the circularly polarized light unit This eliminates the need for cost reduction and miniaturization of the device. In this embodiment, the discharge section has a two-layer structure, but it is not limited to this, and may have a three-layer, four-layer, etc. structure.

【0016】[0016]

【発明の効果】以上述べたように、本発明によれば、対
向配置した誘電体、すなわち放電部を複数段積層する構
造としたので、大容量出力が可能でかつ装置自体の小型
化が図れるという極めて有用な効果を奏する。
[Effects of the Invention] As described above, according to the present invention, a structure is adopted in which a plurality of dielectric bodies, that is, discharge parts, are stacked in a plurality of stages, which are arranged opposite to each other, so that a large capacity output is possible and the device itself can be miniaturized. This has an extremely useful effect.

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

【図1】本発明のガスレーザ発振器の一実施例を示す左
断面図である。
FIG. 1 is a left sectional view showing an embodiment of a gas laser oscillator of the present invention.

【図2】図1に示した一実施例の斜視図である。FIG. 2 is a perspective view of the embodiment shown in FIG. 1;

【図3】従来のガスレーザ発振器の概要を示す断面図で
ある。
FIG. 3 is a cross-sectional view showing an outline of a conventional gas laser oscillator.

【符号の説明】[Explanation of symbols]

11a,11b,12a,12b,13a,13b,1
4a,14b…誘電体 15a,15b,16a,16b,17a,17b,1
8a,18b…放電電極 20,21,22,23…高周波電源 26,27…軸流ファン 30,31,32,33…ミラー
11a, 11b, 12a, 12b, 13a, 13b, 1
4a, 14b...Dielectric 15a, 15b, 16a, 16b, 17a, 17b, 1
8a, 18b...Discharge electrode 20, 21, 22, 23...High frequency power source 26, 27...Axial flow fan 30, 31, 32, 33...Mirror

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】  所定部位に金属を溶射して形成された
放電電極を有する対向配置された誘電体と、前記放電電
極に高周波電圧を印加する高周波電源と、前記対向配置
された誘導体の間隙にレーザ媒質を送風する送風手段と
、複数のミラーを組合わせて構成された共振手段とを具
備し、前記対向配置された誘電体を複数段積層したこと
を特徴とするガスレーザ発振器。
1. A dielectric material disposed opposite to each other having a discharge electrode formed by spraying metal on a predetermined portion, a high frequency power source for applying a high frequency voltage to the discharge electrode, and a dielectric material disposed opposite to each other in a gap between the dielectric materials disposed oppositely to each other and having a discharge electrode formed by spraying metal on a predetermined portion. 1. A gas laser oscillator comprising a blowing means for blowing a laser medium and a resonating means configured by combining a plurality of mirrors, and comprising a plurality of stacked dielectrics arranged facing each other.
JP7073291A 1991-04-03 1991-04-03 Gas laser oscillator Pending JPH04306891A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP7073291A JPH04306891A (en) 1991-04-03 1991-04-03 Gas laser oscillator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7073291A JPH04306891A (en) 1991-04-03 1991-04-03 Gas laser oscillator

Publications (1)

Publication Number Publication Date
JPH04306891A true JPH04306891A (en) 1992-10-29

Family

ID=13440001

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7073291A Pending JPH04306891A (en) 1991-04-03 1991-04-03 Gas laser oscillator

Country Status (1)

Country Link
JP (1) JPH04306891A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2015223591A (en) * 2014-05-26 2015-12-14 住友重機械工業株式会社 Laser processor and laser oscillation method

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2015223591A (en) * 2014-05-26 2015-12-14 住友重機械工業株式会社 Laser processor and laser oscillation method

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