JPH02268475A - Gas laser device - Google Patents

Gas laser device

Info

Publication number
JPH02268475A
JPH02268475A JP8799289A JP8799289A JPH02268475A JP H02268475 A JPH02268475 A JP H02268475A JP 8799289 A JP8799289 A JP 8799289A JP 8799289 A JP8799289 A JP 8799289A JP H02268475 A JPH02268475 A JP H02268475A
Authority
JP
Japan
Prior art keywords
discharge
cathode
gas laser
discharge space
anode
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
JP8799289A
Other languages
Japanese (ja)
Other versions
JPH0716047B2 (en
Inventor
Noboru Okamoto
昇 岡本
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.)
National Institute of Advanced Industrial Science and Technology AIST
Original Assignee
Agency of Industrial Science and Technology
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 Agency of Industrial Science and Technology filed Critical Agency of Industrial Science and Technology
Priority to JP8799289A priority Critical patent/JPH0716047B2/en
Publication of JPH02268475A publication Critical patent/JPH02268475A/en
Publication of JPH0716047B2 publication Critical patent/JPH0716047B2/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
    • 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 enable sufficient pre-ionization and to stabilize laser output by providing a mesh electrode body inside a dielectric to pre-ionize a discharge space between a cathode and an anode. CONSTITUTION:When a high voltage power source 5 is operated, discharge produces between a metal line 23 and an edge section of an inner periphery of each opening 9 of a cathode 3, and a discharge space is pre-ionized. Through this proceeding, main stroke produces between the cathode 3 and an anode 4 to carry out laser oscillation. A field strength of main stroke which produces between the edge section of the inner periphery of the opening 9 and the metal line 23 increases, thereby carrying out sufficient pre-ionization. Main stroke and laser output are stabilized in this way.

Description

【発明の詳細な説明】 [発明の目的] (産業上の利用分野) この発明はガスレーザ媒質を放電エネルギで励起してレ
ーザ光を放出するガスレーザ装置に関する。
DETAILED DESCRIPTION OF THE INVENTION [Object of the Invention] (Industrial Application Field) The present invention relates to a gas laser device that excites a gas laser medium with discharge energy to emit laser light.

(従来の技術) 一般に、TEACO2レーザやエキシマレーザなどのが
スレーザ装置はガスレーザ媒質が収容されたレーザ管内
に主放電電極を構成する陰極と陽極とが離間対向して配
置され、これらの間に主放電を発生させることによって
上記ガスレーザ媒質を励起してレーザ光を放出するよう
になっている。
(Prior Art) In general, in a laser device such as a TEACO2 laser or an excimer laser, a cathode and an anode, which constitute a main discharge electrode, are placed in a laser tube containing a gas laser medium, separated from each other and facing each other. By generating a discharge, the gas laser medium is excited to emit laser light.

上記陰極と陽極との間に主放電を発生させるに先立ち、
陰極と陽極との間の空間、つまり放電空間を予備電離手
段によって予備電離し、レーザ発振が効率よく行なえる
ようにしている。予備電離手段としては種々のタイプの
ものがあり、その1つとしてコロナ電極を用いてコロナ
放電を発生させて予備電離する手段がある。
Prior to generating the main discharge between the cathode and anode,
The space between the cathode and the anode, that is, the discharge space, is pre-ionized by the pre-ionization means so that laser oscillation can be performed efficiently. There are various types of pre-ionization means, one of which is a means for pre-ionizing by generating corona discharge using a corona electrode.

従来、コロナ電極を用いて放電空間を予fWl電離する
ガスレーザ装置としては、第3図に示す構造のものがあ
った。すなわち、同図中1は密閉容器としてのレーザ管
で、このレーザ管1内にはC02、N 2 、Heなど
のガスを混合したガスレーザ媒質が収容されている。ま
た、レーザ管1内には一対の保持板2が離間対向して配
設されている。各保持板2の対向する面にはそれぞれ主
放電電極を構成する陰極3と陽極4とが電気的に導通し
た状態で保持固定されている。これら陰極3と陽極4と
は高圧電源5に接続されているとともに上記陰極3はア
ースされている。
Conventionally, there has been a gas laser device having a structure shown in FIG. 3, which uses a corona electrode to preliminarily ionize a discharge space by fWl. That is, in the figure, reference numeral 1 denotes a laser tube as a closed container, and a gas laser medium containing a mixture of gases such as CO2, N2, and He is housed in the laser tube 1. Further, a pair of holding plates 2 are arranged in the laser tube 1 so as to be spaced apart from each other and facing each other. A cathode 3 and an anode 4 constituting a main discharge electrode are held and fixed on opposing surfaces of each holding plate 2 in an electrically conductive state. These cathode 3 and anode 4 are connected to a high voltage power source 5, and the cathode 3 is grounded.

1上記一対の保持板2間には波形整形のためのピーキン
グコンデンサ6が接続され、さらにレーザ管1内にはガ
スレーザ媒質を矢示方向に循環させるファン7と、この
ファン7の上流側に熱交換器8とが配設されている。
1 A peaking capacitor 6 for waveform shaping is connected between the pair of holding plates 2, and a fan 7 for circulating the gas laser medium in the direction of the arrow is provided in the laser tube 1, and a heat source is provided upstream of the fan 7. An exchanger 8 is provided.

上記陰極3は、多数の開口9を有するたとえばパンチン
グメタルやメツシュなどの開口金属板によって形成され
、その内部には予備電離手段としてのコロナ電極11が
収容されている。このコロナ電極11は石英ガラスやマ
イカ板などの誘電体12内に帯状の銅板13が設けられ
てなり、上記銅板13は上記高圧電源5に接続されてい
る。
The cathode 3 is formed of an open metal plate, such as punched metal or mesh, having a large number of openings 9, and a corona electrode 11 as a pre-ionization means is housed inside the cathode 3. This corona electrode 11 is made up of a strip-shaped copper plate 13 provided within a dielectric 12 such as quartz glass or mica plate, and the copper plate 13 is connected to the high voltage power source 5.

このような構成のガスレーザ装置においては、高圧電源
5が作動して電気エネルギが供給されると、まず銅板1
3と陰極3の開口9の内周縁のエツジ部とでコロナ放電
が発生し、それによって陰極3と陽極4との間の放電空
間が予備電離される。
In the gas laser device having such a configuration, when the high voltage power supply 5 is activated and electrical energy is supplied, first the copper plate 1 is
3 and the edge of the inner periphery of the opening 9 of the cathode 3, a corona discharge occurs, thereby pre-ionizing the discharge space between the cathode 3 and the anode 4.

そして、放電空間の予fil電離が進むと、陰極3と陽
極4との間で主放電が起こり、この主放電によって生じ
る分子発生光が図示しない光共振器で共振されてレーザ
光が発振されることになる。
Then, as the prefil ionization of the discharge space progresses, a main discharge occurs between the cathode 3 and the anode 4, and the molecular generated light generated by this main discharge is resonated in an optical resonator (not shown) to oscillate laser light. It turns out.

しかしながら、コロナ電極11の銅板13の平面と陰極
3の開口9のエツジ部との間で生じるコーロナ放電は電
界極度が十分に高くならないので、放電空間の予備電離
電子密度も低くなってしまう。
However, in the corona discharge that occurs between the plane of the copper plate 13 of the corona electrode 11 and the edge portion of the opening 9 of the cathode 3, the electric field strength is not sufficiently high, and the density of pre-ionized electrons in the discharge space also becomes low.

そのため、上記放電空間が十分に予(ii電離されする
い状態となるため、陰極3と陽極4との間に生じる主放
電が不安定な状態となり、安定した出力でレーザ発振さ
せることができないということがあった。
As a result, the discharge space becomes sufficiently pre-ionized, and the main discharge generated between the cathode 3 and the anode 4 becomes unstable, making it impossible to oscillate the laser with a stable output. Something happened.

このように、従来の予備電離手段は放電空間を十分に予
備電離することができなかったので、陰極と陽極との間
の主放電が安定せず、それによってレーザ出力も不安定
になるということがあった。
As described above, the conventional pre-ionization means could not sufficiently pre-ionize the discharge space, so the main discharge between the cathode and the anode was not stable, and the laser output was also unstable. was there.

この発明は上記事情にもとずきなされたもので、その目
的とするところは、予備電離による電界強度を十分に強
くして安定したレーザ出力が得られるようにしたガスレ
ーザ装置を提供することにある。
This invention was made based on the above-mentioned circumstances, and its purpose is to provide a gas laser device that can obtain stable laser output by sufficiently increasing the electric field strength caused by pre-ionization. be.

[発明の構成] (課題を解決するための手段及び作用)上記課題を解決
するためにこの発明は、ガスレーザ媒質を封入した密閉
容器と、この密閉容器1、内に相対向して設けられる少
な(とも一対の主放電電極と、これら主放電電極間の放
電空間を予備電離する予備電離手段と、上記主放電電極
の放電によって生じた上記放電空間における分子発生光
を共振する光共振器とを備えたガスレーザ発振装置にお
いて、上記予備電離手段は上記主放電電極の少なくとも
一方の放電面のほぼ全域にわたって形成された複数の開
口と、これら開口を有する上記放電面の反対側に設けら
れかつ誘電体で被覆された電極体とを具備し、上記電極
体を網目状に形成する。
[Structure of the Invention] (Means and Effects for Solving the Problems) In order to solve the above problems, the present invention includes a hermetic container in which a gas laser medium is sealed, and a container provided oppositely in the hermetic container 1. (Both include a pair of main discharge electrodes, a pre-ionization means for pre-ionizing the discharge space between these main discharge electrodes, and an optical resonator that resonates the light generated by molecules in the discharge space caused by the discharge of the main discharge electrodes. In the gas laser oscillation device, the pre-ionization means includes a plurality of openings formed over almost the entire discharge surface of at least one of the main discharge electrodes, and a dielectric material provided on the opposite side of the discharge surface having these openings. The electrode body is formed into a mesh shape.

このようにすることで、放電空間を十分な電界強度とな
るよう予備電離できるようにした。
By doing so, it was possible to pre-ionize the discharge space so that the electric field strength was sufficient.

(実施例) 以下、この発明の一実施例を第1図と第2図を参照して
説明する。なお、第3図に示す構成と同一部分には同一
記号を付して説明を省略する。
(Embodiment) An embodiment of the present invention will be described below with reference to FIGS. 1 and 2. Incidentally, the same parts as those in the configuration shown in FIG. 3 are given the same symbols and the explanation will be omitted.

すなわち、この発明における予備電離手段としてのコロ
ナ電極21は、石炭ガラスやマイカなどの読本正接が少
ない材料からなる誘電体22内に電極体として細い金属
線23を網目状に配設して構成されている。上記金属線
23は、たとえば直径が0.1mm程度の細いピアノ線
が用いられている。
That is, the corona electrode 21 as a preliminary ionization means in the present invention is constructed by disposing thin metal wires 23 as an electrode body in a mesh shape within a dielectric body 22 made of a material with a low reading tangent such as coal glass or mica. ing. The metal wire 23 is, for example, a thin piano wire with a diameter of about 0.1 mm.

このような構成のガスレーザ装置において、高圧電源5
を作動させると、金属線23と陰極3のそれぞれの開口
9の内周縁のエツジ部との間で放電が発生し、放電空間
が予6fHft離される。そして、このようにして放電
空間の予備電離が進むと、陰極3と陽極4との間で主放
電が発生し、それによってレーザ発振が行われることに
なる。
In the gas laser device having such a configuration, the high voltage power supply 5
When activated, a discharge occurs between the metal wire 23 and the edge portion of the inner peripheral edge of each opening 9 of the cathode 3, and the discharge space is separated by 6fHft. As the preliminary ionization of the discharge space progresses in this manner, a main discharge occurs between the cathode 3 and the anode 4, thereby causing laser oscillation.

ところで、陰極3の開口9の内周縁のエツジ部と金属線
23との間に生じる放電は、上記開口9の内周縁のエツ
ジ部と金属線23とがともに鋭利であるから、これらの
間に発生する放電の電界強度が高くなる。したがって、
放電空間の予fil電離電子密度が高くなり、十分に予
備電離されることになるから、陰極3と陽極4との間に
生じる主放電が安定し、レーザ出力も安定することにな
る。
By the way, the discharge that occurs between the inner peripheral edge of the opening 9 of the cathode 3 and the metal wire 23 is caused by the discharge occurring between the inner peripheral edge of the opening 9 and the metal wire 23, which are both sharp. The electric field strength of the generated discharge increases. therefore,
Since the pre-fil ionized electron density in the discharge space becomes high and the electrons are sufficiently pre-ionized, the main discharge generated between the cathode 3 and the anode 4 is stabilized, and the laser output is also stabilized.

しかも、上記コロナ電極21の金属線23は網目状に設
けられているから、上記金属線23を単に並列に配置し
た場合に比べて陰極3との対向面積が増大する。したが
って、電界強度が高くなるとともに電界の分布状態が均
一になるから、そのことによっても予備電M電子密度が
高くなり、レザ出力が安定化する。
Moreover, since the metal wires 23 of the corona electrode 21 are provided in a mesh shape, the area facing the cathode 3 is increased compared to a case where the metal wires 23 are simply arranged in parallel. Therefore, the electric field strength increases and the electric field distribution becomes uniform, which also increases the preliminary electric M electron density and stabilizes the laser output.

なお、上記一実施例ではコロナ電極を陰極の背面側に設
置した場合について説明したが、陽極の背面側に設置す
るようにしてもよい。また、誘電体を筒状に形成し、そ
の内部に金属線を収容するようにしてもよい。
In the above embodiment, the corona electrode was installed on the back side of the cathode, but it may be installed on the back side of the anode. Alternatively, the dielectric material may be formed into a cylindrical shape, and the metal wire may be housed inside the dielectric material.

[発明の効果] 以上述べたようにこの発明は、陰極と陽極との間の放電
空間を予備電離する予備電離手段として誘電体内に網目
状の電極体を設けたものを用いるようにした。したがっ
て、誘電体内に銅板を設けた従来のコロナ電極に比べて
電界強度の強いコロナ放電を発生させることができるか
ら、放電空間の予6ii電離電子密度が高くなって十分
に予備電離され、レーザ出力を安定させることができる
[Effects of the Invention] As described above, the present invention uses a mesh-shaped electrode body provided within a dielectric body as a pre-ionization means for pre-ionizing the discharge space between the cathode and the anode. Therefore, since it is possible to generate a corona discharge with a stronger electric field strength than the conventional corona electrode with a copper plate provided in the dielectric, the pre-ionized electron density in the discharge space becomes high and is sufficiently pre-ionized, resulting in laser output. can be stabilized.

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

第1図はこの発明の一実施例を示すガスレーザ装置の断
面図、第2図は同じくコロナ電極の斜視図、第3図は従
来のガスレーザ装置の断面図である。 1・・・レーザ管(密閉容器)、3・・・陰極、4・・
・陽極、 5・・・高圧電源、 1・・・コロナ電極、 22・・・ 誘電体、 3・・・金属線 (電極体)
FIG. 1 is a sectional view of a gas laser device showing an embodiment of the present invention, FIG. 2 is a perspective view of a corona electrode, and FIG. 3 is a sectional view of a conventional gas laser device. 1... Laser tube (closed container), 3... Cathode, 4...
・Anode, 5... High voltage power supply, 1... Corona electrode, 22... Dielectric, 3... Metal wire (electrode body)

Claims (1)

【特許請求の範囲】[Claims] ガスレーザ媒質を封入した密閉容器と、この密閉容器内
に相対向して設けられる少なくとも一対の主放電電極と
、これら主放電電極間の放電空間を予備電離する予備電
離手段と、上記主放電電極の放電によって生じた上記放
電空間における分子発生光を共振する光共振器とを備え
たガスレーザ発振装置において、上記予備電離手段は上
記主放電電極の少なくとも一方の放電面のほぼ全域にわ
たって形成された複数の開口と、これら開口を有する上
記放電面の反対側に設けられかつ誘電体で被覆された電
極体とを具備し、上記電極体を網目状に形成したことを
特徴とするガスレーザ装置。
A sealed container enclosing a gas laser medium, at least a pair of main discharge electrodes provided opposite each other in the sealed container, a pre-ionization means for pre-ionizing a discharge space between these main discharge electrodes, and a pre-ionization means for pre-ionizing the discharge space between the main discharge electrodes; In the gas laser oscillation device, the pre-ionization means includes a plurality of optical resonators that resonate molecularly generated light in the discharge space generated by discharge, and the pre-ionization means includes a plurality of laser beams formed over almost the entire discharge surface of at least one of the main discharge electrodes. 1. A gas laser device comprising: apertures; and an electrode body provided on the opposite side of the discharge surface having these apertures and covered with a dielectric, the electrode body being formed in a mesh shape.
JP8799289A 1989-04-10 1989-04-10 Gas laser equipment Expired - Lifetime JPH0716047B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8799289A JPH0716047B2 (en) 1989-04-10 1989-04-10 Gas laser equipment

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8799289A JPH0716047B2 (en) 1989-04-10 1989-04-10 Gas laser equipment

Publications (2)

Publication Number Publication Date
JPH02268475A true JPH02268475A (en) 1990-11-02
JPH0716047B2 JPH0716047B2 (en) 1995-02-22

Family

ID=13930304

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8799289A Expired - Lifetime JPH0716047B2 (en) 1989-04-10 1989-04-10 Gas laser equipment

Country Status (1)

Country Link
JP (1) JPH0716047B2 (en)

Also Published As

Publication number Publication date
JPH0716047B2 (en) 1995-02-22

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