JP2584949Y2 - CO2 laser oscillator - Google Patents

CO2 laser oscillator

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Publication number
JP2584949Y2
JP2584949Y2 JP3370893U JP3370893U JP2584949Y2 JP 2584949 Y2 JP2584949 Y2 JP 2584949Y2 JP 3370893 U JP3370893 U JP 3370893U JP 3370893 U JP3370893 U JP 3370893U JP 2584949 Y2 JP2584949 Y2 JP 2584949Y2
Authority
JP
Japan
Prior art keywords
cathode
inner diameter
axial direction
laser oscillator
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.)
Expired - Fee Related
Application number
JP3370893U
Other languages
Japanese (ja)
Other versions
JPH0686361U (en
Inventor
達也 大東
保 上埜
幸治 伊藤
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.)
Daihen Corp
Original Assignee
Daihen 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 Daihen Corp filed Critical Daihen Corp
Priority to JP3370893U priority Critical patent/JP2584949Y2/en
Publication of JPH0686361U publication Critical patent/JPH0686361U/en
Application granted granted Critical
Publication of JP2584949Y2 publication Critical patent/JP2584949Y2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Description

【考案の詳細な説明】[Detailed description of the invention]

【0001】[0001]

【産業上の利用分野】本考案は、炭酸ガスレーザ発振器
に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a carbon dioxide laser oscillator.

【0002】[0002]

【従来の技術】炭酸ガスレーザ発振器は、レーザ共振器
内にCO2 、N2 、He等の混合ガスを所定圧力で封入
し、これに高電圧を印加してグロー放電を発生させ、こ
の放電によってCO2 分子から放出される光を光共振器
によって増幅して、エネルギー密度の高いレーザビーム
を得るものである。図3は、高速軸流形と呼ばれる方式
の炭酸ガスレーザ発振器の構造を示す、一部断面正面図
である。同図において1a,1bは石英や強化ガラス等
の電気絶縁材から形成された放電管、2は放電管1a,
1bと同様の材質から成る絶縁管、3a,3bは直流高
圧電源、4a,4bは放電管1a,1bと絶縁管2とを
連結するアルミ等の導電材から形成されたホルダ、5
a,5bはホルダ4a,4b内に設けられた円筒形状の
高電位の陰極、6a,6bは放電管1a,1b内に設け
られた陽極であり、それぞれ高圧電源3a,3bに連結
される。なお、安全上各陽極6a,6bは電気的に接地
されている。放電管1aのX1 側端部には全反射鏡7が
設けられると共に、放電管1bのX2 側端部には部分透
過鏡8が設けられている。9は作動ガスを循環させるた
めのブロア、10aは放電によって温度上昇したガスの
熱を除去するための電気的に接地された熱交換器、10
bはブロア9の圧縮熱によって温度上昇したガスの熱を
除去するための熱交換器である。放電管1a、1bには
作動ガス循環用の配管11a,11bが連結され、配管
11a,11bの他端は熱交換器10bに連結されてい
る。13a,13bはセラミック等の絶縁物から形成さ
れたホルダである。以上により構成される炭酸ガスレー
ザ発振器において、陽極6aと陰極5aおよび陽極6b
と陰極5bとの間に夫々高電圧を印加することにより、
陽極6aと陰極5aおよび陽極6aと陰極6bとの間に
夫々グロー放電が発生する。他方,CO2 、N2 、He
等から成る作動ガスは夫々陽極6a,6bから陰極5
a,5bに向かって符号12で示す矢印の方向に高速で
流される。このようにグロー放電を発生してレーザの励
起が行われる。すなわち、全反射鏡7と部分透過鏡8と
の間で繰り返して増幅された後、レーザ光13が部分透
過鏡8を透過して外部に放出される。
2. Description of the Related Art In a carbon dioxide gas laser oscillator, a mixed gas of CO 2 , N 2 , He, etc. is sealed at a predetermined pressure in a laser resonator, and a high voltage is applied thereto to generate a glow discharge. The light emitted from the CO 2 molecule is amplified by an optical resonator to obtain a laser beam having a high energy density. FIG. 3 is a partially sectional front view showing a structure of a carbon dioxide laser oscillator of a system called a high-speed axial flow type. In the figure, reference numerals 1a and 1b denote discharge tubes formed of an electrically insulating material such as quartz or tempered glass, and 2 denotes discharge tubes 1a and 1b.
Insulating tubes made of the same material as 1b, 3a and 3b are DC high-voltage power supplies, 4a and 4b are holders made of a conductive material such as aluminum for connecting the discharge tubes 1a and 1b and the insulating tube 2;
Reference numerals a and 5b denote cylindrical high-potential cathodes provided in the holders 4a and 4b, and reference numerals 6a and 6b denote anodes provided in the discharge tubes 1a and 1b, which are connected to the high-voltage power supplies 3a and 3b, respectively. In addition, each anode 6a, 6b is electrically grounded for safety. The X 1 side end portion of the discharge tube 1a with a total reflection mirror 7 is provided, on the X 2 side end portion of the discharge tube 1b are is provided partially transmitting mirror 8. 9 is a blower for circulating the working gas, 10a is an electrically grounded heat exchanger for removing the heat of the gas whose temperature has been raised by the discharge, 10a
b denotes a heat exchanger for removing the heat of the gas whose temperature has increased due to the compression heat of the blower 9. The discharge tubes 1a, 1b are connected to pipes 11a, 11b for circulating working gas, and the other ends of the pipes 11a, 11b are connected to a heat exchanger 10b. 13a and 13b are holders formed of an insulator such as ceramic. In the carbon dioxide laser oscillator configured as described above, the anode 6a, the cathode 5a, and the anode 6b
By applying a high voltage between the cathode and the cathode 5b, respectively,
A glow discharge is generated between the anode 6a and the cathode 5a and between the anode 6a and the cathode 6b. On the other hand, CO 2 , N 2 , He
The working gas composed of the anode 6a, 6b and the cathode 5
It is made to flow at high speed in the direction of the arrow indicated by reference numeral 12 toward a and 5b. Thus, glow discharge is generated to excite the laser. That is, after being repeatedly amplified between the total reflection mirror 7 and the partial transmission mirror 8, the laser light 13 is transmitted through the partial transmission mirror 8 and emitted to the outside.

【0003】[0003]

【考案が解決しようとする課題】ところが、図3に示さ
れる従来の装置では、陰極と陽極間、即ち5aー6a、
及び5bー6b間のグロー放電によって発生したイオン
はそれぞれ陰極5a、5bにかかる電位傾度により加速
され高エネルギーとなって陰極5a,5bの表面に衝突
し、陰極物質がスパッタとして放出される。ここで従来
の要部拡大図4により、陰極5aの近傍の放電状態を説
明する。
However, in the conventional apparatus shown in FIG. 3, between the cathode and the anode, that is, 5a-6a,
Ions generated by the glow discharge between the electrodes 5b and 6b are accelerated by the potential gradient applied to the cathodes 5a and 5b, become high energy, collide with the surfaces of the cathodes 5a and 5b, and the cathode material is emitted as sputter. Here, a discharge state near the cathode 5a will be described with reference to FIG.

【0004】図4において、14aはグロー放電の形状
を示している。絶縁材よりなるホルダ13aに支持され
た放電管1aと、導電材よりなるホルダ4aに支持され
た陰極5aとは、軸方向に間隙を設けて配置される。一
方陰極5aは、レーザ光の共振領域を制限して、モード
形状を良くするために、陰極の内径が、放電管1aの内
径より小さい円筒形状に形成されている。このよう
に、軸方向に間隙があり、さらに、陰極5aの角が放電
空間に突出しているために、陰極5aの陽極側、即ちX
1方向の端部に電界の集中が起き、放電管内を広った
グロー放電14aは、電流を増加しても、陰極全体に広
がることなく、陰極5aの端部に集中する。ここで、放
出されるスパッタの量は、陰極部における放電密度にほ
ぼ比例する。即ち、電極間5a−6aに印加される電力
量にほぼ比例し、また、陰極部における放電面積にほぼ
反比例する。こうしてスパッタとして放出された陰極物
質、例えばニッケルスパッタは発振器内部を高速で循環
しているガス流によって下流側へと流され、その一部は
絶縁管2の内壁面に付着する。
In FIG. 4, reference numeral 14a denotes a glow discharge shape. The discharge tube 1a supported by the holder 13a made of an insulating material and the cathode 5a supported by the holder 4a made of a conductive material are arranged with a gap in the axial direction. On the other hand, the cathode 5a is formed in a cylindrical shape in which the inside diameter of the cathode is smaller than the inside diameter of the discharge tube 1a in order to limit the resonance region of the laser beam and improve the mode shape. like this
There is a gap in the axial direction, and the corner of the cathode 5a is discharged.
Since it protrudes into the space, the anode side of the cathode 5a, that is, X
1 direction end concentration of the electric field occurs in the glow discharge 14a to the wide discharge tube but was Tsu, even if increasing the current, without spreading over the entire cathode, concentrated on the edge portion of the cathode 5a. Here, the amount of sputter released is substantially proportional to the discharge density in the cathode portion. That is, it is almost proportional to the amount of electric power applied between the electrodes 5a-6a, and almost inversely proportional to the discharge area in the cathode portion. The cathode material, such as nickel sputter, released as sputter in this way is caused to flow downstream by the gas flow circulating at high speed inside the oscillator, and a part thereof adheres to the inner wall surface of the insulating tube 2.

【0005】図3に示すされる装置では、スパッタが絶
縁管2の内面に付着するにつれて、絶縁管2の絶縁特性
が低下する。この絶縁管2の絶縁特性が低下すると、陰
極5aと接地された熱交換器10aとの間に異常放電が
起こり、予期するグロー放電が得られなくなる。このた
め、レーザ出力が不安定になり、ひいては、レーザ出力
が低下する。
In the apparatus shown in FIG. 3, as the sputter adheres to the inner surface of the insulating tube 2, the insulating characteristics of the insulating tube 2 deteriorate. If the insulation characteristics of the insulating tube 2 deteriorate, abnormal discharge occurs between the cathode 5a and the grounded heat exchanger 10a, and the expected glow discharge cannot be obtained. For this reason, the laser output becomes unstable, and as a result, the laser output decreases.

【0006】さらに、スパッタの一部が反射鏡7および
部分透過鏡8の内面に付着してレーザー出力を低下させ
ていた。このため、絶縁管1a,1b,2、反射鏡7お
よび部分透過鏡8等を定期的に補修する必要があり、コ
スト高となっていた。
Further, a part of the sputter adheres to the inner surfaces of the reflecting mirror 7 and the partially transmitting mirror 8 to reduce the laser output. For this reason, it is necessary to periodically repair the insulating tubes 1a, 1b, 2, the reflecting mirror 7, the partially transmitting mirror 8, and the like, resulting in an increase in cost.

【0007】また、絶縁管2の絶縁特性を維持する方法
として、絶縁管2のX方向の長さを長くすることが考え
られるが、発振器が大形化するという欠点があった。
As a method for maintaining the insulating properties of the insulating tube 2, it is conceivable to increase the length of the insulating tube 2 in the X direction, but there is a disadvantage that the oscillator becomes large.

【0008】本考案の目的は、発振器を大形化すること
なく、またレーザ出力の低下を可及的に小さくすること
ができ、かつメンテナンス周期の長い高速軸流形炭酸ガ
スレーザ発振器を提供することである。
SUMMARY OF THE INVENTION An object of the present invention is to provide a high-speed axial-flow type carbon dioxide laser oscillator which has a long maintenance cycle without increasing the size of the oscillator and can minimize a decrease in laser output. It is.

【0009】[0009]

【課題を解決するための手段】本第1の考案は、電気絶
縁材よりなる放電管に、軸方向に離間する陽極と陰極と
からなる電極を配設し、該電極間に直流高電圧を印加す
る炭酸ガスレーザ発振器に適用される。その特徴とする
ところは、陰極を円筒状とすると共に、円筒状陰極の陽
極方向の端部側に、該端部から陰極の軸方向に縮径する
テーパー部を形成し、放電管の端部と陰極のテーパー部
の開口端部とを軸方向に実質的に突き合わせ、かつ放電
管の端部の内径を、陰極のテーパー部の開口端の内径よ
りも小さく形成したことである。本第2の考案は、電気
絶縁材よりなる放電管に、軸方向に離間する陽極と陰極
とからなる電極を配設し、該電極間に直流高電圧を印加
する炭酸ガスレーザ発振器に適用される。その特徴とす
るところは、陰極を円筒状とすると共に、円筒状陰極の
陽極方向の端部側に、該端部から陰極の軸方向に縮径す
るテーパー部を形成し、放電管の端部を支持する電気絶
縁材よりなる絶縁ホルダの端部と陰極のテーパー部の開
口端部とを軸方向に実質的に突き合わせ、かつ絶縁ホル
ダの陰極側端部の内径を、陰極のテーパー部の開口端の
内径よりも小さく形成したことである。
According to a first aspect of the present invention, a discharge tube made of an electrically insulating material is provided with an electrode consisting of an anode and a cathode spaced apart in the axial direction, and a high DC voltage is applied between the electrodes. It is applied to a carbon dioxide laser oscillator to be applied. The feature is that the cathode is cylindrical, and a tapered portion is formed at the end of the cylindrical cathode in the anode direction, the diameter of which is reduced in the axial direction of the cathode from the end. And the opening end of the tapered portion of the cathode substantially abuts in the axial direction, and the inside diameter of the end of the discharge tube is formed smaller than the inside diameter of the opening end of the tapered portion of the cathode. This second invention is applied to a carbon dioxide laser oscillator in which electrodes consisting of an anode and a cathode which are spaced apart in the axial direction are arranged on a discharge tube made of an electrically insulating material, and a high DC voltage is applied between the electrodes. . The feature is that the cathode is cylindrical, and a tapered portion is formed at the end of the cylindrical cathode in the anode direction, the diameter of which is reduced in the axial direction of the cathode from the end. The end of the insulating holder made of an electrically insulating material supporting the end of the insulating taper and the opening end of the tapered portion of the cathode substantially abut each other in the axial direction, and the inner diameter of the end of the insulating holder on the cathode side is changed to the opening of the tapered portion of the cathode. That is, it was formed smaller than the inner diameter of the end.

【0010】[0010]

【実施例】以下、本考案を図示の実施例により、詳細に
説明する。図1は、本考案の実施例の要部拡大図であっ
て、図4に相当する図である。なお、図4と同じ構成部
品には、同じ符号を付してある。図1において、陰極5
aの内径は、放電管laの内径より小さく、断面が陽極
側、即ちX1 方向側に拡径するテーパー状に形成されて
いる。さらに、テーパー部の開口端の内径は、絶縁材か
らなるホルダ13aの内径よりも大きい円筒状に形成さ
れている。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS The present invention will be described below in detail with reference to the illustrated embodiments. FIG. 1 is an enlarged view of a main part of an embodiment of the present invention, and corresponds to FIG. The same components as those in FIG. 4 are denoted by the same reference numerals. In FIG. 1, the cathode 5
the inner diameter of a is smaller than the inner diameter of the discharge tube la, it is formed in a tapered shape whose cross section is enlarged to the anode side, i.e. X 1 direction. Further, the inner diameter of the opening end of the tapered portion is formed in a cylindrical shape larger than the inner diameter of the holder 13a made of an insulating material.

【0011】レーザ発振器の稼動は、図3に示す従来技
と同様であって、ブロア9により作動ガスを循環させ
るとともに、電極5a−6aおよび5b−6b間に高電
圧を印加してグロー放電を発生させる。ところで、図
に示されるごとく、陰極5aのテーパー状の端部の内径
が、絶縁材よりなるホルダ13aの内径よりも小さく、
かつホルダ13aの端部と陰極5aの端部とは軸方向に
実質的に間隙を有しないため、陰極端の電界集中が緩和
される。しかも、グロー放電14aは陰極のテーパー状
部に広がって発生する。
The operation of the laser oscillator is based on the prior art shown in FIG.
It is similar to the operator, together with the circulating working gas by a blower 9, a high voltage is applied to generate glow discharge between the electrodes 5a-6a and 5b-6b. By the way, as shown in FIG. 2
As shown in, the inner diameter of the tapered end of the cathode 5a is rather smaller than the inner diameter of the holder 13a made of an insulating material,
In addition, since the end of the holder 13a and the end of the cathode 5a have substantially no gap in the axial direction, the electric field concentration at the cathode end is reduced. In addition, the glow discharge 14a is generated by spreading over the tapered portion of the cathode .

【0012】すなわち、グロー放電14aは、陰極5a
のテーパー状部に広がって発生するため、陰極に着目す
れば、放電密度が低下することになる。
That is, the glow discharge 14a is connected to the cathode 5a
Therefore, if attention is paid to the cathode, the discharge density decreases.

【0013】このように、陰極部における放電密度の低
下により、放出されるスパッタの量が大幅に減少した。
このため、絶縁管2の内壁に付着するスパッタの量は、
著しく低減される。すなわち、絶縁管2の絶縁特性の低
下を防ぐことができ、異常放電が起こりにくく、レーザ
出力の低下の度合いが極めて緩やかとなる。
As described above, the amount of sputter released is greatly reduced due to the decrease in the discharge density in the cathode portion.
Therefore, the amount of spatter adhering to the inner wall of the insulating tube 2 is
It is significantly reduced. That is, it is possible to prevent the insulation characteristics of the insulating tube 2 from being deteriorated, and it is difficult for abnormal discharge to occur, and the degree of reduction in the laser output becomes extremely gentle.

【0014】勿論、スパッタ量が著しく低減することに
より、絶縁管1a,1b,2、反射鏡7および部分透過
鏡8等の補修周期が長くなるため、補修費用を低減する
ことができる。さらに絶縁管2のX方向の長さを長尺に
する必要がなく、レーザ発振器を小型化することができ
る。
Of course, when the amount of spatter is remarkably reduced, the repair cycle of the insulating tubes 1a, 1b, 2, the reflecting mirror 7, the partially transmitting mirror 8, and the like becomes longer, so that the repair cost can be reduced. Further, it is not necessary to make the length of the insulating tube 2 in the X direction long, and the laser oscillator can be downsized.

【0015】図2は、本考案の他の実施例を示したもの
で、放電管laを、陰極5aに密接し、陰極5aのテー
パー部の開口端の内径が放電管laの内径よりも大きく
形成されている。この場合も、陰極5aの端部の電界集
中が緩和され、グロー放電14aは陰極5aのテーパー
部に広がり、スパッタの量を大幅に低減させることがで
きた。
FIG. 2 shows another embodiment of the present invention, in which the discharge tube la is closely contacted with the cathode 5a, and the inner diameter of the opening end of the tapered portion of the cathode 5a is larger than the inner diameter of the discharge tube la. Is formed. Also in this case, the concentration of the electric field at the end of the cathode 5a was reduced, and the glow discharge 14a spread over the tapered portion of the cathode 5a, so that the amount of sputtering could be greatly reduced.

【0016】以上の説明は、ガス流の方向を陽極から陰
極に流した場合を示したが、陰極から陽極へガスを流す
こともできる。また、陰極の内径を放電管の内径よりも
大きくしても、モード形状が悪化することとなるが、ス
パッタの量を低減させることに関して実効がある。
In the above description, the case where the direction of the gas flow is from the anode to the cathode is shown. However, the gas may flow from the cathode to the anode. Further, if the inner diameter of the cathode is larger than the inner diameter of the discharge tube, the mode shape is deteriorated, but it is effective in reducing the amount of sputtering.

【0017】[0017]

【考案の効果】以上の説明で明らかなように、本考案に
よれば、高エネルギーのイオンの衝突で陰極5a、5b
の表面から放出されるスパッタは、発振器内部を高速で
循環しているガス流によって下流側へと流されるが、円
筒状陰極の陽極方向の端部から、陰極の軸方向に縮径す
るテーパー部を形成し、放電管の陰極側の内径を、前記
テーパー部の開口端の内径よりも小さく形成することに
より、スパッタ量が著しく低減され、絶縁管の絶縁特性
の低下を防ぐことができ、異常放電が起こりにくく、レ
ーザ出力の低下の度合いが極めて緩やかとなる。勿論、
スパッタ量が著しく低減することにより、絶縁管、反射
鏡および部分透過鏡等の補修周期が長くなるため、補修
費用を低減することができる。さらに絶縁管のX方向の
長さを長尺にする必要がなく、レーザ発振器を小型化す
ることができる。
As is clear from the above description, according to the present invention, the cathodes 5a, 5b
The sputter emitted from the surface of the cylindrical cathode is caused to flow downstream by the gas flow circulating at high speed inside the oscillator, but from the end in the anode direction of the cylindrical cathode, the tapered part which reduces in diameter in the axial direction of the cathode By forming the inner diameter of the discharge tube on the cathode side smaller than the inner diameter of the opening end of the tapered portion, the amount of spatter can be significantly reduced, and the insulation characteristics of the insulating tube can be prevented from deteriorating. Discharge does not easily occur, and the degree of decrease in laser output becomes extremely moderate. Of course,
When the amount of spatter is remarkably reduced, the repair cycle of the insulating tube, the reflecting mirror, the partially transmitting mirror, and the like becomes longer, so that the repair cost can be reduced. Further, it is not necessary to make the length of the insulating tube in the X direction long, and the laser oscillator can be downsized.

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

【図1】本考案の実施例の要部拡大断面図FIG. 1 is an enlarged sectional view of a main part of an embodiment of the present invention.

【図2】本考案の他の実施例の要部拡大断面図FIG. 2 is an enlarged sectional view of a main part of another embodiment of the present invention.

【図3】従来例を示す一部断面正面図FIG. 3 is a partial cross-sectional front view showing a conventional example.

【図4】図3の要部拡大断面図FIG. 4 is an enlarged sectional view of a main part of FIG. 3;

【符号の説明】[Explanation of symbols]

1a 放電管 3a 直流高圧電源 4a 陰極ホルダ 5a 陰極 6a 陽極1a Discharge tube 3a DC high voltage power supply 4a Cathode holder 5a Cathode 6a Anode

Claims (3)

(57)【実用新案登録請求の範囲】(57) [Scope of request for utility model registration] 【請求項1】 電気絶縁材よりなる放電管に、軸方向に
離間する陽極と陰極とからなる電極を配設し、該電極間
に直流高電圧を印加する炭酸ガスレーザ発振器におい
て、前記陰極を円筒状とすると共に、前記円筒状陰極の
前記陽極方向の端部側に、該端部から陰極の軸方向に縮
径するテーパー部を形成し、放電管の端部と前記陰極の
テーパー部の開口端部とを軸方向に対向させ、かつ前記
放電管の端部の内径を、前記陰極のテーパー部の開口端
の内径よりも小さく形成して、グロー放電を前記陰極の
テーパー部に拡大させた炭酸ガスレーザ発振器。
1. A carbon dioxide laser oscillator in which a discharge tube made of an electrically insulating material is provided with an electrode consisting of an anode and a cathode spaced apart in an axial direction, and a high DC voltage is applied between the electrodes. Along with the end of the cylindrical cathode in the anode direction, a tapered portion is formed from the end to reduce the diameter in the axial direction of the cathode. The end of the discharge tube and the opening of the tapered portion of the cathode are formed. The end portion is opposed to the axial direction, and the inner diameter of the end portion of the discharge tube is formed smaller than the inner diameter of the open end of the tapered portion of the cathode, so that glow discharge is performed on the cathode.
Carbon dioxide laser oscillator expanded to the tapered part .
【請求項2】 電気絶縁材よりなる放電管に、軸方向に
離間する陽極と陰極とからなる電極を配設し、該電極間
に直流高電圧を印加する炭酸ガスレーザ発振器におい
て、前記陰極を円筒状とすると共に、前記円筒状陰極の
前記陽極方向の端部側に、該端部から陰極の軸方向に縮
径するテーパー部を形成し、放電管の端部を支持する電
気絶縁材よりなる絶縁ホルダの端部と前記陰極のテーパ
ー部の開口端部とを軸方向に突き合わせ、かつ前記絶縁
ホルダの陰極側端部の内径を、前記陰極のテーパー部の
開口端の内径よりも小さく形成して、グロー放電を前記
陰極のテーパー部に拡大させた炭酸ガスレーザ発振器。
2. A carbon dioxide laser oscillator in which a discharge tube made of an electrically insulating material is provided with an electrode consisting of an anode and a cathode spaced apart in the axial direction, and a DC high voltage is applied between the electrodes. The cylindrical cathode is formed on the end side in the anode direction of the cylindrical cathode with a tapered portion which is reduced in diameter in the axial direction of the cathode from the end, and is made of an electrically insulating material for supporting the end of the discharge tube. an open end of the tapered portion of the cathode and the end portion of the insulating holder fit can impact in the axial direction and the inner diameter of the cathode-side end portion of the insulating holder, smaller than the inner diameter of the open end of the tapered portion of the cathode Forming a glow discharge
Carbon dioxide laser oscillator expanded to the tapered part of the cathode .
【請求項3】 前記陰極の円筒部の内径が、放電管の内
径よりも大きく形成してなる請求項1または請求項2に
記載の炭酸ガスレーザ発振器。
Wherein the inner diameter of the cylindrical portion of the cathode, formed by the size rather than the inner diameter of the discharge tube according to claim 1 or a carbon dioxide gas laser oscillator according to claim 2.
JP3370893U 1993-05-28 1993-05-28 CO2 laser oscillator Expired - Fee Related JP2584949Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP3370893U JP2584949Y2 (en) 1993-05-28 1993-05-28 CO2 laser oscillator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP3370893U JP2584949Y2 (en) 1993-05-28 1993-05-28 CO2 laser oscillator

Publications (2)

Publication Number Publication Date
JPH0686361U JPH0686361U (en) 1994-12-13
JP2584949Y2 true JP2584949Y2 (en) 1998-11-11

Family

ID=12393920

Family Applications (1)

Application Number Title Priority Date Filing Date
JP3370893U Expired - Fee Related JP2584949Y2 (en) 1993-05-28 1993-05-28 CO2 laser oscillator

Country Status (1)

Country Link
JP (1) JP2584949Y2 (en)

Also Published As

Publication number Publication date
JPH0686361U (en) 1994-12-13

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