JP2560366Y2 - High-speed axial-flow type carbon dioxide laser oscillator - Google Patents

High-speed axial-flow type carbon dioxide laser oscillator

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Publication number
JP2560366Y2
JP2560366Y2 JP1991011547U JP1154791U JP2560366Y2 JP 2560366 Y2 JP2560366 Y2 JP 2560366Y2 JP 1991011547 U JP1991011547 U JP 1991011547U JP 1154791 U JP1154791 U JP 1154791U JP 2560366 Y2 JP2560366 Y2 JP 2560366Y2
Authority
JP
Japan
Prior art keywords
discharge
laser oscillator
anodes
carbon dioxide
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 - Lifetime
Application number
JP1991011547U
Other languages
Japanese (ja)
Other versions
JPH0499856U (en
Inventor
直樹 浦井
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 JP1991011547U priority Critical patent/JP2560366Y2/en
Publication of JPH0499856U publication Critical patent/JPH0499856U/ja
Application granted granted Critical
Publication of JP2560366Y2 publication Critical patent/JP2560366Y2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

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、電極を改良した高速軸
流形炭酸ガスレ−ザ発振器に関するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a high-speed axial flow type carbon dioxide laser oscillator having improved electrodes.

【0002】[0002]

【従来の技術】高速軸流形炭酸ガスレ−ザ発振器におい
て、高出力を得る場合、一般的に放電管を複数個直列に
した共振器構成が採用される。図1は、上記構成を採用
した従来の分割放電式の高速軸流形炭酸ガスレ−ザ発振
器の概略構成図である。同図において、共振器1は例え
ば4個の第1乃至第4放電管2,3,4,5が直列に接
続されており、各放電管には各々第1乃至第4陰極2
a,3a,4a,5a及び第1乃至第4陽極2b,3
b,4b,5bが設けられ、放電管の長手方向に設けた
陰極及び陽極の対電極の極性を交互に異ならせて配設さ
れている。この第1乃至第4陰極2a〜5a及び第1乃
至第4陽極2b〜5b間には、各々第1乃至第4高圧直
流電源62,63,64,65が接続され、両電極間に
電圧を印加すると、グロ−放電7が発生する。また、第
1及び第4放電管2,5の端部には、反射鏡8及び出力
鏡9が配設されており、出力鏡9によりレ−ザ光10が
外部に取り出される。ガス通路11に設けたブロワ12
を駆動すると、放電管内に充填したガス媒体が矢印方向
に循環すると共に、放電によって温度上昇したガスの熱
とブロワ12の圧縮熱によって温度上昇したガスの熱
が、各々熱交換器13,14により除去される。
2. Description of the Related Art In a high-speed axial-flow type carbon dioxide laser oscillator, in order to obtain a high output, a resonator configuration in which a plurality of discharge tubes are connected in series is generally employed. FIG. 1 is a schematic configuration diagram of a conventional split discharge type high-speed axial flow type carbon dioxide laser oscillator employing the above configuration. In the figure, a resonator 1 has, for example, four first to fourth discharge tubes 2, 3, 4, and 5 connected in series, and each discharge tube has a first to fourth cathode 2 respectively.
a, 3a, 4a, 5a and first to fourth anodes 2b, 3
b, 4b, and 5b are provided, and the counter electrodes of the cathode and the anode provided in the longitudinal direction of the discharge tube are alternately provided with different polarities. First to fourth high-voltage DC power supplies 62, 63, 64, 65 are connected between the first to fourth cathodes 2a to 5a and the first to fourth anodes 2b to 5b, respectively. When applied, a glow discharge 7 is generated. A reflecting mirror 8 and an output mirror 9 are disposed at the ends of the first and fourth discharge tubes 2 and 5, and the output mirror 9 extracts the laser beam 10 to the outside. Blower 12 provided in gas passage 11
Is driven, the gas medium filled in the discharge tube circulates in the direction of the arrow, and the heat of the gas whose temperature has increased due to the discharge and the heat of the gas whose temperature has increased due to the compression heat of the blower 12 are respectively transferred by the heat exchangers 13 and 14. Removed.

【0003】[0003]

【考案が解決しようとする問題点】ところで、安全上の
見地から各陽極が接地されているために、隣接する陰極
を近づける構成にした場合、例えば第1放電管2が第2
放電管3よりも僅かにガス圧力が低く、放電開始をしや
すい状態となっていると、先に放電管2で放電が開始さ
れて、放電電流I1 は図2の実線に示すように、電源6
2→陽極2b→放電管2→陰極2a→第1電源62と流
れ、放電管2内にグロ−放電7が発生する。このとき、
第2電源63からの印加電圧が陽極3b及び陰極3a間
に加えられているが、放電管3に放電が発生することな
く、電源63による放電電流I2 は図2の点線に示すよ
うに、電源63→大地→陽極2b→放電管2→陰極3a
→電源63と流れ、放電管2内に新たな放電71が生じ
る。放電管2内放電は、電源62及び63の印加電圧に
より電流密度が増し、グロ−放電からア−ク放電へと移
行するので、正規のレ−ザ放電が得られないために、レ
−ザ出力が低下する。したがって、従来の分割放電式の
レ−ザ発振器においては、上記のような不正規のレ−ザ
放電を防止するために、隣接する各陰極間に適宜の絶縁
距離を設ける必要があり、これが共振器内の放電利用
率、すなわち全体の共振器空間に対する放電利用空間の
比率を下げる原因となっている。例えば、この比率が5
0%以下になることもあり、高出力を得ようとすれば、
レ−ザ発振器の長大化を招く欠点がある。
Problems to be Solved by the Invention Since each anode is grounded from a safety point of view, when the adjacent cathodes are arranged close to each other, for example, the first discharge tube 2 is connected to the second discharge tube.
When the gas pressure is slightly lower than that of the discharge tube 3 and the discharge is easily started, the discharge is started in the discharge tube 2 first, and the discharge current I1 is reduced as shown by the solid line in FIG. 6
2 → anode 2b → discharge tube 2 → cathode 2a → first power supply 62, and glow discharge 7 is generated in discharge tube 2. At this time,
Although the voltage applied from the second power supply 63 is applied between the anode 3b and the cathode 3a, no discharge occurs in the discharge tube 3, and the discharge current I2 from the power supply 63 is reduced as shown by the dotted line in FIG. 63 → ground → anode 2b → discharge tube 2 → cathode 3a
→ The current flows to the power source 63, and a new discharge 71 is generated in the discharge tube 2. In the discharge in the discharge tube 2, the current density is increased by the applied voltage of the power supplies 62 and 63, and the discharge is changed from glow discharge to arc discharge. Therefore, a regular laser discharge cannot be obtained. Output drops. Therefore, in the conventional split discharge type laser oscillator, it is necessary to provide an appropriate insulating distance between adjacent cathodes in order to prevent the above-mentioned irregular laser discharge. This causes a reduction in the discharge utilization rate in the vessel, that is, the ratio of the discharge utilization space to the entire resonator space. For example, if this ratio is 5
It may be 0% or less.
There is a disadvantage that the laser oscillator becomes longer.

【0004】[0004]

【問題点を解決するための手段】上記の問題点を解決す
るために、本考案においては、陰極及び陽極の対電極を
長手方向に設けた放電管を、対電極の極性を交互に異な
らせて放電管の長手方向に複数配設した分割放電式の高
速軸流形炭酸ガスレーザ発振器を対象とし、隣接する対
電極の陰極同士を各々共通にして、陰極間を同電位と
し、共通にした陰極と対になる陽極との間に、各々高圧
電源を接続するとともに、上記複数の陽極の内隣接する
陽極間を電気的に接続し、かつ上記陽極のいずれか1つ
のみを接地したことを特徴とする。
Means for Solving the Problems To solve the above problems, in the present invention, a discharge tube provided with a cathode and an anode counter electrode in the longitudinal direction is formed by alternately changing the polarity of the counter electrode. The target is a high-speed axial flow type carbon dioxide laser oscillator of the split discharge type arranged in the longitudinal direction of a plurality of discharge tubes.
High pressure between the common cathode and the paired anode.
Connect the power supply and adjoin adjacent one of the anodes
Electrically connect the anodes and any one of the above anodes
It is characterized in that only one is grounded .

【0005】[0005]

【実施例】図3は、本考案の実施例を示す共振器本体の
要部概略構成図である。同図において、第1共通陰極2
3aは図1に示す従来の第1及び第2陰極2a,3a間
に設けた適宜の絶縁距離をなくし、これらの陰極同士を
共通にして、同電位とするもので、また第2共通陰極4
5aは従来の第3及び第4陰極4a,5a間の絶縁距離
をなくし、陰極同士を共通にするものである。これに伴
って、第1放電管2と第2放電管3及び第3放電管4と
第4放電管5との間に設けた絶縁管が不要となる。第1
及び第2陽極2b,3bと第1共通陰極23aとの間
に、各々高圧直流電源62,63を接続し、第3及び第
4陽極4a,5aと第2共通陰極45aとの間に、各々
電源64,65を接続し、この第2及び第3陽極3b,
4b間を外部接続し、かつ上記陽極のどれか1つ、例え
ば第1陽極2bを接地する。放電に際しては、従来のよ
うに各陽極を接地したことによる回り回路が形成される
ことがないので、各陰極及び陽極間に正規のレ−ザ放電
(グロ−放電)7が発生し、また電源62,63による
電位差が相殺されて、第2(第3)陽極3b(,4b)
の電位が零となり、同様に第4陽極5bの電位も零とな
る。なお、放電として直流電源を用いての直流放電であ
るが、交流放電であってもよい。
FIG. 3 is a schematic diagram showing a main part of a resonator body according to an embodiment of the present invention. In the figure, the first common cathode 2
Reference numeral 3a designates a structure in which a proper insulating distance provided between the conventional first and second cathodes 2a and 3a shown in FIG.
Numeral 5a eliminates the conventional insulation distance between the third and fourth cathodes 4a and 5a, and makes the cathodes common. Accordingly, an insulating tube provided between the first discharge tube 2 and the second discharge tube 3 and between the third discharge tube 4 and the fourth discharge tube 5 becomes unnecessary. First
And high-voltage DC power supplies 62 and 63 are connected between the second anodes 2b and 3b and the first common cathode 23a, respectively, between the third and fourth anodes 4a and 5a and the second common cathode 45a. The power sources 64 and 65 are connected, and the second and third anodes 3b,
4b is externally connected, and one of the anodes, for example, the first anode 2b is grounded. At the time of discharge, since a circuit is not formed by grounding each anode as in the prior art, a regular laser discharge (glow discharge) 7 is generated between each cathode and anode, and The potential difference due to 62, 63 is canceled, and the second (third) anode 3b (, 4b)
Becomes zero, and similarly, the potential of the fourth anode 5b also becomes zero. The discharge is a DC discharge using a DC power supply, but may be an AC discharge.

【0006】[0006]

【考案の効果】以上のように、本考案によれば、一端を
接地することによって安全性を確保しつつ陰極間に絶縁
距離を設ける必要がなく、かつ回り回路が形成されるこ
とがないので、共振器内の放電利用率を向上させること
ができる。したがって、従来と同出力を得る場合、より
レーザ発振器の小形化が図られ、また高出力を得る場
合、発振器の長大化を防止することができる。
[Effect of the Invention] As described above, according to the present invention, one end
By grounding , there is no need to provide an insulation distance between the cathodes while ensuring safety , and a round circuit is formed.
Therefore , the discharge utilization rate in the resonator can be improved. Therefore, when the same output as that of the related art is obtained, the size of the laser oscillator can be further reduced. When a high output is obtained, the length of the oscillator can be prevented.

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

【図1】従来の分割放電式の高速軸流形炭酸ガスレ−ザ
発振器の概略構成図である。
FIG. 1 is a schematic configuration diagram of a conventional split discharge type high-speed axial flow type carbon dioxide laser oscillator.

【図2】従来の発振器における不正規のレ−ザ放電をす
る場合の説明図である。
FIG. 2 is an explanatory diagram in the case of performing an irregular laser discharge in a conventional oscillator.

【図3】本考案の実施例を示す共振器本体の要部概略構
成図である。
FIG. 3 is a schematic configuration diagram of a main part of a resonator main body showing an embodiment of the present invention.

【符号の説明】[Explanation of symbols]

2〜5 第1乃至第4放電管 2a〜5a 第1乃至第4陰極 2b〜5b 第1乃至第4陽極 23a 第1共通陰極 45a 第2共通陰2-5 the first to fourth discharge tube 2a~5a first to fourth cathode 2B-5b first to fourth anode 23a first co Tsukage electrode 45a second co Tsukage pole

Claims (1)

(57)【実用新案登録請求の範囲】(57) [Scope of request for utility model registration] 【請求項1】 陰極及び陽極の対電極を長手方向に設け
た放電管を、前記対電極の極性を交互に異ならせて前記
放電管の長手方向に複数配設した分割放電式の高速軸流
形炭酸ガスレーザ発振器において、隣接する前記対電極
の陰極同士を各々共通にして、前記陰極間を同電位と
し、前記共通にした陰極と対になる陽極との間に、各々
高圧電源を接続するとともに、前記複数の陽極の内隣接
する陽極間を電気的に接続し、かつ前記陽極のいずれか
1つのみを接地した高速軸流形炭酸ガスレーザ発振器。
1. A split discharge type high-speed axial flow in which a plurality of discharge tubes provided with a counter electrode of a cathode and an anode in the longitudinal direction are arranged in the longitudinal direction of the discharge tube by alternately changing the polarities of the counter electrodes. In the carbon dioxide laser oscillator, the cathodes of the adjacent counter electrodes are made common to each other, and the same potential is applied between the cathodes.
And between the common cathode and the paired anode,
Connect a high-voltage power supply, and adjacent to the plurality of anodes
The anodes to be electrically connected, and any one of the above anodes
High-speed axial flow CO2 laser oscillator with only one grounded .
JP1991011547U 1991-02-08 1991-02-08 High-speed axial-flow type carbon dioxide laser oscillator Expired - Lifetime JP2560366Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1991011547U JP2560366Y2 (en) 1991-02-08 1991-02-08 High-speed axial-flow type carbon dioxide laser oscillator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1991011547U JP2560366Y2 (en) 1991-02-08 1991-02-08 High-speed axial-flow type carbon dioxide laser oscillator

Publications (2)

Publication Number Publication Date
JPH0499856U JPH0499856U (en) 1992-08-28
JP2560366Y2 true JP2560366Y2 (en) 1998-01-21

Family

ID=31745057

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1991011547U Expired - Lifetime JP2560366Y2 (en) 1991-02-08 1991-02-08 High-speed axial-flow type carbon dioxide laser oscillator

Country Status (1)

Country Link
JP (1) JP2560366Y2 (en)

Family Cites Families (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS57139978A (en) * 1981-02-23 1982-08-30 Matsushita Electric Ind Co Ltd Gas laser oscillator
JPS57169287A (en) * 1981-04-10 1982-10-18 Toshiba Corp Gas laser oscillating tube device
JPS5893294A (en) * 1981-11-30 1983-06-02 Hitachi Ltd Laser oscillator
JPH06105803B2 (en) * 1985-02-18 1994-12-21 三菱電機株式会社 Axial gas laser oscillator
JPS6235589A (en) * 1985-08-08 1987-02-16 Matsushita Electric Ind Co Ltd Laser oscillator
JPH0221678A (en) * 1988-07-11 1990-01-24 Toshiba Corp Axial-flow type gas laser

Also Published As

Publication number Publication date
JPH0499856U (en) 1992-08-28

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