JPH04236474A - Discharge-exciting type laser - Google Patents

Discharge-exciting type laser

Info

Publication number
JPH04236474A
JPH04236474A JP500991A JP500991A JPH04236474A JP H04236474 A JPH04236474 A JP H04236474A JP 500991 A JP500991 A JP 500991A JP 500991 A JP500991 A JP 500991A JP H04236474 A JPH04236474 A JP H04236474A
Authority
JP
Japan
Prior art keywords
discharge
laser
electrodes
power supply
series
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
JP500991A
Other languages
Japanese (ja)
Inventor
Yasuhiro Ogura
靖弘 小倉
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 JP500991A priority Critical patent/JPH04236474A/en
Publication of JPH04236474A publication Critical patent/JPH04236474A/en
Pending legal-status Critical Current

Links

Landscapes

  • Lasers (AREA)

Abstract

PURPOSE:To provide a discharge-exciting type laser which can efficiently obtain a laser output and be composed compactly. CONSTITUTION:In a discharge-exciting type laser in which a plurality of discharge units 7 each having a pair of discharge electrodes 5a, 5b disposed oppositely through a discharge space 4 sealed with laser gas 8 and a power source 6 for applying a voltage to the electrodes 5a, 5b, are arranged axially of the space 4 to discharge-excite the gas 8 in each unit 7 to obtain a laser output, the waveforms and the phases of the power source voltages of the respective units 7 are brought in coincidence.

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】本発明は放電励起型レーザ装置に
係り、特に高い効率でレーザ出力を得ることができ、装
置をコンパクトに構成することが可能な放電励起型レー
ザ装置に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a discharge-excited laser device, and more particularly to a discharge-excited laser device that can obtain laser output with high efficiency and can be constructed compactly.

【0002】0002

【従来の技術】近年、放電励起により発振されるレーザ
光は、医療機器、金属加工機器、計測機器、計量機器な
どの広い分野で利用されている。特に炭酸ガスレーザ光
などのように出力が大きいレーザ光を発振するレーザ装
置は切断、溶接、焼入れ加工、表面処理などの加工分野
で利用されており、従来加工が困難であった小物部品や
脆性材料の加工を可能にし、さらに短時間で大量かつ高
精密に加工できる特色を活かして精密機械や電子機器の
製造に利用されている。
2. Description of the Related Art In recent years, laser light oscillated by discharge excitation has been used in a wide range of fields such as medical equipment, metal processing equipment, measuring equipment, and weighing equipment. In particular, laser devices that emit high-output laser beams such as carbon dioxide laser beams are used in processing fields such as cutting, welding, hardening, and surface treatment, and are used to process small parts and brittle materials that were previously difficult to process. It is used in the manufacture of precision machinery and electronic equipment, taking advantage of its ability to process large quantities with high precision in a short period of time.

【0003】上記のような各種レーザ加工機に使用され
る放電励起型レーザ装置として、例えば図5に示すもの
がある。すなわち図5に示す放電励起型レーザ装置は、
放電容器1に装着された誘電体2と、この誘電体2から
間隔をおいて放電容器1内に配設された誘電体3と、上
記誘電体2および誘電体3の間に形成された放電空間4
を挟むように対抗して設けられた一対の電極5a,5b
と、この電極5a,5b間に電圧を印加する電源6とか
ら成る放電ユニット7を放電空間の軸方向に2基並列に
配置して構成される。ここで図5に示すように2基の放
電ユニット7,7を説明上、A系列とB系列とに区別す
る。
An example of a discharge-excited laser device used in the various laser processing machines described above is shown in FIG. 5. That is, the discharge excited laser device shown in FIG.
A dielectric 2 attached to the discharge vessel 1, a dielectric 3 disposed within the discharge vessel 1 at a distance from the dielectric 2, and a discharge formed between the dielectric 2 and the dielectric 3. space 4
A pair of electrodes 5a and 5b are provided opposite to each other so as to sandwich the
and a power source 6 that applies a voltage between the electrodes 5a and 5b. Two discharge units 7 are arranged in parallel in the axial direction of the discharge space. Here, as shown in FIG. 5, the two discharge units 7, 7 are distinguished into an A series and a B series for the sake of explanation.

【0004】各放電ユニット7の容量は電源6の容量に
よって制約されるため、特に大出力のレーザ光を得るこ
とが必要なレーザ装置においては、上記のように個別に
電源回路を有する放電ユニット7を複数基並列に配置し
て構成される。
Since the capacity of each discharge unit 7 is limited by the capacity of the power supply 6, especially in a laser device that needs to obtain a high output laser beam, the discharge unit 7 having an individual power supply circuit as described above is used. It is constructed by arranging multiple units in parallel.

【0005】A,B各系列の放電ユニット7,7の電極
5a,5bに電源6,6よりそれぞれ電圧が印加される
ことにより、誘電体2,3間に放電が起こり、放電空間
4内に封入されたレーザガス8が励起され、高出力のレ
ーザ光が放出される。放出されたレーザ光は増幅された
後に、光路に配設された数枚の反射鏡で屈光され、レー
ザヘッド内に装填したレンズで被加工物表面の所定位置
に集光される。そしてレーザ光が照射された狭い領域に
エネルギが集中され、被加工物に穴を形成したり、切断
、溶接、表面処理を行なうために使用される。
When voltages are applied from the power supplies 6 and 6 to the electrodes 5a and 5b of the discharge units 7 and 7 of the A and B series, respectively, a discharge occurs between the dielectrics 2 and 3, and a discharge occurs in the discharge space 4. The enclosed laser gas 8 is excited and a high-power laser beam is emitted. After the emitted laser light is amplified, it is bent by several reflecting mirrors disposed in the optical path, and focused at a predetermined position on the surface of the workpiece by a lens installed in the laser head. Energy is concentrated in a narrow area irradiated with laser light, and is used to form holes in the workpiece, perform cutting, welding, and surface treatment.

【0006】[0006]

【発明が解決しようとする課題】しかしながら、上記の
ように個別に電源を装備した放電ユニットを複数基並列
に配設して構成された放電励起型レーザ装置においては
、各放電ユニットの電源回路の波形および位相が異なっ
ているため、隣接する電極間に電位差が生じ、隣接電極
間で異常放電を起こす場合が多い。
[Problems to be Solved by the Invention] However, in a discharge-excited laser device configured by arranging a plurality of discharge units each equipped with an individual power supply in parallel as described above, the power supply circuit of each discharge unit is Since the waveforms and phases are different, a potential difference occurs between adjacent electrodes, which often causes abnormal discharge between adjacent electrodes.

【0007】すなわちA系列およびB系列のそれぞれの
電源回路の電源6,6の出力電圧V10,V20の位相
が図6に示すように相互に異なるため、両系列の電極5
a,5b間に印加電圧V11およびV21も相互に異る
。このことは軸方向に隣接する電極間においても電位差
Vdを生じ、隣接電極間に異常放電を起こし易いことを
意味する。
That is, since the phases of the output voltages V10 and V20 of the power supplies 6 and 6 of the A series and B series power supply circuits are different from each other as shown in FIG.
The voltages V11 and V21 applied between a and 5b are also different from each other. This means that a potential difference Vd also occurs between electrodes adjacent in the axial direction, and abnormal discharge is likely to occur between the adjacent electrodes.

【0008】このような異常放電を抑止するため、従来
は軸方向に隣接する電極5a,5bおよび電極5a,5
bとの間を離し適当な絶縁距離dを確保することが余儀
なくされていた。しかしながら、レーザガス中では大気
中より絶縁性能が低いため、より効果的に異常放電を阻
止するためには、絶縁距離dを充分に大きく設定するこ
とが必要であり、装置が大型化してしまう欠点があった
。一方、電極が配置されておらず放電現象が起こらない
絶縁空間部に滞留するレーザガスは、発振したレーザ光
を吸収する性質があるため、この絶縁空間部によりレー
ザ発振器の出力効率が低下する問題があった。そしてこ
の欠点を補うためには、さらに容量が大きな電源を装備
する必要があり、いずれにしても装置構成が過大になっ
てしまう問題点があった。
In order to suppress such abnormal discharge, conventionally, the electrodes 5a, 5b adjacent to each other in the axial direction and the electrodes 5a, 5
It has been necessary to keep an appropriate insulation distance d apart from b. However, since the insulation performance is lower in laser gas than in the atmosphere, in order to more effectively prevent abnormal discharge, it is necessary to set the insulation distance d sufficiently large, which has the disadvantage of increasing the size of the device. there were. On the other hand, the laser gas that stays in the insulating space where no electrodes are placed and no discharge phenomenon occurs has the property of absorbing the oscillated laser light, so this insulating space can reduce the output efficiency of the laser oscillator. there were. In order to compensate for this drawback, it is necessary to equip a power supply with a larger capacity, and in any case, there is a problem that the device configuration becomes excessively large.

【0009】本発明は上記の問題点を解決するためにな
されたものであり、高い効率でレーザ出力を得ることが
でき、装置をコンパクトに構成することが可能な放電励
起型レーザ装置を提供することを目的とする。〔発明の
構成〕
The present invention has been made to solve the above problems, and provides a discharge-excited laser device that can obtain laser output with high efficiency and that can be configured compactly. The purpose is to [Structure of the invention]

【0010】0010

【課題を解決するための手段】上記目的を達成するため
本発明は、レーザガスを封入した放電空間を挟むように
対抗して配置された一対の放電電極と、この放電電極に
電圧を印加する電源とから成る放電ユニットを放電空間
の軸方向に複数基配列し、各放電ユニットにおいてレー
ザガスを放電励起することにより、レーザ出力を得る放
電励起型レーザ装置において、上記各放電ユニットの電
源電圧の波形および位相を一致させたことを特徴とする
[Means for Solving the Problems] In order to achieve the above object, the present invention provides a pair of discharge electrodes arranged opposite to each other so as to sandwich a discharge space filled with laser gas, and a power source for applying voltage to the discharge electrodes. In a discharge excitation type laser device that obtains a laser output by arranging a plurality of discharge units in the axial direction of the discharge space and exciting the laser gas by discharge in each discharge unit, the waveform of the power supply voltage of each discharge unit and It is characterized by matching the phases.

【0011】[0011]

【作用】上記構成に係る放電励起型レーザ装置によれば
、装置に組み込まれる複数基の放電ユニットの電源電圧
の波形および位相が一致するように構成されているため
、軸方向に隣接する電極間に電位差が発生することがな
く、異常放電の発生が少ないため、高い効率でレーザ発
振を行なうことができる。
[Operation] According to the discharge-excited laser device having the above configuration, the waveforms and phases of the power supply voltages of the plurality of discharge units incorporated in the device are configured to match, so that the distance between adjacent electrodes in the axial direction is Since no potential difference is generated between the laser beams and abnormal discharges are less likely to occur, laser oscillation can be performed with high efficiency.

【0012】また絶縁距離を短縮することができるため
、装置をコンパクト化できる上に、レーザガスの非励起
領域を低減させることができ、小型で高い発振効率を有
する放電励起型レーザ装置を提供することができる。
[0012] Furthermore, since the insulation distance can be shortened, the device can be made compact, and the non-excited region of the laser gas can be reduced, thereby providing a discharge-excited laser device that is compact and has high oscillation efficiency. I can do it.

【0013】[0013]

【実施例】次に本発明の一実施例について添付図面を参
照して説明する。図1は本発明の一実施例を示す断面図
であり、図2は本実施例装置の電源電圧を示す図である
。なお、図5,6に示す従来例と同一要素には同一符号
を付して、その重複する説明を省略する。
DESCRIPTION OF THE PREFERRED EMBODIMENTS Next, an embodiment of the present invention will be described with reference to the accompanying drawings. FIG. 1 is a sectional view showing one embodiment of the present invention, and FIG. 2 is a diagram showing the power supply voltage of the device of this embodiment. Note that the same elements as those in the conventional example shown in FIGS. 5 and 6 are denoted by the same reference numerals, and redundant explanation thereof will be omitted.

【0014】すなわち、本実施例に係る放電励起型レー
ザ装置は、レーザガス8を封入した放電空間4を挟むよ
うに対抗して配置された一対の放電電極5a,5bと、
この放電電極5a,5bに電圧を印加する電源6とから
成る放電ユニット7を放電空間4の軸方向に2基並列に
配列し、各放電ユニット7,7においてレーザガス8を
放電励起することにより、レーザ出力を得る放電励起型
レーザ装置において、上記各放電ユニット7,7の電源
電圧の波形および位相を一致させる位相基準器8を配設
して構成される。
That is, the discharge excitation type laser device according to this embodiment includes a pair of discharge electrodes 5a and 5b arranged opposite to each other so as to sandwich a discharge space 4 filled with laser gas 8;
By arranging two discharge units 7 in parallel in the axial direction of the discharge space 4, each consisting of a power source 6 that applies a voltage to the discharge electrodes 5a and 5b, and exciting the laser gas 8 by discharge in each discharge unit 7, A discharge-excited laser device that obtains a laser output includes a phase reference device 8 that matches the waveform and phase of the power supply voltage of each of the discharge units 7, 7.

【0015】A系列およびB系列の放電ユニット7,7
の電源6,6は位相基準器8に接続されており、電源6
,6はそれぞれ位相基準器8から信号を受け、その位相
および波形が一致するように調整される。電源6,6か
ら個別にA系列およびB系列の電極5a,5bおよび5
a,5b間に電圧が印加される。
A-series and B-series discharge units 7, 7
The power supplies 6, 6 are connected to the phase reference device 8, and the power supplies 6, 6 are connected to the phase standard 8.
, 6 each receive a signal from the phase reference device 8 and are adjusted so that their phases and waveforms match. The A series and B series electrodes 5a, 5b and 5 are individually connected to the power supplies 6, 6.
A voltage is applied between a and 5b.

【0016】ここで両系列の電源6,6の位相および波
形がともに一致することとなるため、図1.2に示すよ
うにA系列の電源6の出力電圧V10とB系列の電源6
の出力電圧V20とがほぼ同一となるため、A系列の電
極5a,5bとB系列の電極5a,5b間に印加される
電圧も相互に等しくなり電位差を生じることもなく、異
常放電が起こるおそれも少ない。したがって軸方向に隣
接する電極間に大きな絶縁距離を確保する必要がなくな
り、装置を小型化することができる。
Since the phases and waveforms of the power supplies 6 and 6 of both series match, the output voltage V10 of the power supply 6 of the A series and the power supply 6 of the B series match as shown in FIG. 1.2.
Since the output voltage V20 of the electrodes is almost the same, the voltages applied between the A-series electrodes 5a, 5b and the B-series electrodes 5a, 5b are also equal to each other, and no potential difference occurs, which may cause abnormal discharge. There are also few. Therefore, there is no need to ensure a large insulation distance between electrodes adjacent in the axial direction, and the device can be downsized.

【0017】また絶縁距離も短縮できることから、レー
ザガスの非励起領域を低減することが可能となり、さら
にレーザ光の吸収による損失が低減され、装置全体とし
てレーザ光の発振効率を大幅に高めることができる。ま
たレーザ光の発振容量を一定にした場合には、相対的に
電源容量を小型化することができ、また電源の配設数も
削減することができる。
[0017] Furthermore, since the insulation distance can be shortened, it is possible to reduce the non-excited region of the laser gas, and furthermore, the loss due to laser light absorption is reduced, and the laser light oscillation efficiency of the entire device can be greatly increased. . Further, when the oscillation capacity of the laser beam is kept constant, the power supply capacity can be relatively reduced, and the number of power supplies can also be reduced.

【0018】次に本発明の他の実施例について図3,4
を参照して説明する。図3に示す実施例においては、図
1に示す構成要素に加えて、A,B各系列の放電ユニッ
ト7,7の電源6,6と位相基準器8との間に、各電源
回路の回路長の違いによって生じる位相差を解消する位
相補正器9,9をそれぞれ配設して構成される。
Next, regarding other embodiments of the present invention, FIGS.
Explain with reference to. In the embodiment shown in FIG. 3, in addition to the components shown in FIG. It is constructed by disposing phase correctors 9, 9, respectively, to eliminate the phase difference caused by the difference in length.

【0019】本実施例によれば、電源6,6が高周波回
路で構成され、電源電圧V10と放電用電極の印加電圧
V20との間に、送電路長の微妙な違いによって大きな
位相差を生じる場合においても両者の位相をより正しく
一致させることができる。
According to this embodiment, the power supplies 6, 6 are constructed of high-frequency circuits, and a large phase difference occurs between the power supply voltage V10 and the applied voltage V20 of the discharge electrode due to a subtle difference in the length of the power transmission path. Even in this case, the phases of the two can be matched more accurately.

【0020】すなわち、電源6と電極5a,5bとの間
の配線のインピーダンスが、A,B各系列の電源回路毎
になり、電源6,6側の電圧を一致させると、電極5a
,5b,5a,5b間の印加電圧の位相が図4に示すよ
うに異なってしまう場合においても、位相補正器9,9
に内蔵した遅延回路を調整して一方の電源電圧V10,
V20の位相をずらし、最終的にA,B両系列の放電電
極5a,5b,5a,5bの印加電圧V11およびV2
1を相互に一致するように調整することができる。
That is, the impedance of the wiring between the power supply 6 and the electrodes 5a and 5b is different for each power supply circuit of the A and B series, and when the voltages on the power supply 6 and 6 sides are matched, the impedance of the wiring between the power supply 6 and the electrodes 5a and 5b is
, 5b, 5a, 5b, even if the phases of the applied voltages differ as shown in FIG.
By adjusting the built-in delay circuit, one power supply voltage V10,
By shifting the phase of V20, the voltages V11 and V2 applied to the discharge electrodes 5a, 5b, 5a, 5b of both series A and B are finally applied.
1 can be adjusted to match each other.

【0021】[0021]

【発明の効果】以上説明の通り本発明に係る放電励起型
レーザ装置によれば、装置に組み込まれる複数基の放電
ユニットの電源電圧の波形および位相が一致するように
構成されているため、軸方向に隣接する電極間に電位差
が発生することがなく、異常放電の発生が少ないため、
高い効率でレーザ発振を行なうことができる。
Effects of the Invention As explained above, according to the discharge-excited laser device according to the present invention, the waveforms and phases of the power supply voltages of the plurality of discharge units incorporated in the device match, so that the axial There is no potential difference between adjacent electrodes in the direction, and abnormal discharges are less likely to occur.
Laser oscillation can be performed with high efficiency.

【0022】また絶縁距離を短縮することができるため
、装置をコンパクト化できる上に、レーザガスの非励起
領域を低減させることができ、小型で高い発振効率を有
する放電励起型レーザ装置を提供することができる。
[0022] Furthermore, since the insulation distance can be shortened, the device can be made compact, and the non-excited region of the laser gas can be reduced, thereby providing a discharge-excited laser device that is compact and has high oscillation efficiency. I can do it.

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

【図1】本発明に係る放電励起型レーザ装置の一実施例
を示す断面図。
FIG. 1 is a cross-sectional view showing an embodiment of a discharge-pumped laser device according to the present invention.

【図2】図1に示す装置の電源電圧を示す図。FIG. 2 is a diagram showing the power supply voltage of the device shown in FIG. 1;

【図3】本発明の他の実施例を示す断面図。FIG. 3 is a sectional view showing another embodiment of the present invention.

【図4】図3に示す装置の電源電圧および電極間電圧を
示す図。
FIG. 4 is a diagram showing the power supply voltage and inter-electrode voltage of the device shown in FIG. 3;

【図5】従来の放電励起型レーザ装置の構成例を示す断
面図。
FIG. 5 is a cross-sectional view showing a configuration example of a conventional discharge-excited laser device.

【図6】図5に示すレーザ装置の電源電圧を示す図。6 is a diagram showing the power supply voltage of the laser device shown in FIG. 5. FIG.

【符号の説明】[Explanation of symbols]

1  放電容器 2  誘電体 3  誘電体 4  放電空間 5a,5b  電極 6  電源 7  放電ユニット 8  位相基準器 9  位相補正器 1 Discharge vessel 2 Dielectric material 3 Dielectric material 4 Discharge space 5a, 5b electrode 6 Power supply 7 Discharge unit 8 Phase reference device 9 Phase corrector

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】  レーザガスを封入した放電空間を挟む
ように対抗して配置された一対の放電電極と、この放電
電極に電圧を印加する電源とから成る放電ユニットを放
電空間の軸方向に複数基配列し、各放電ユニットにおい
てレーザガスを放電励起することにより、レーザ出力を
得る放電励起型レーザ装置において、上記各放電ユニッ
トの電源電圧の波形および位相を一致させたことを特徴
とする放電励起型レーザ装置。
Claim 1: A plurality of discharge units are arranged in the axial direction of the discharge space, each consisting of a pair of discharge electrodes arranged opposite to each other so as to sandwich a discharge space filled with laser gas, and a power supply that applies voltage to the discharge electrodes. A discharge pumped laser device which obtains a laser output by discharging and exciting a laser gas in each discharge unit, characterized in that the waveform and phase of the power supply voltage of each discharge unit are matched. Device.
JP500991A 1991-01-21 1991-01-21 Discharge-exciting type laser Pending JPH04236474A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP500991A JPH04236474A (en) 1991-01-21 1991-01-21 Discharge-exciting type laser

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP500991A JPH04236474A (en) 1991-01-21 1991-01-21 Discharge-exciting type laser

Publications (1)

Publication Number Publication Date
JPH04236474A true JPH04236474A (en) 1992-08-25

Family

ID=11599552

Family Applications (1)

Application Number Title Priority Date Filing Date
JP500991A Pending JPH04236474A (en) 1991-01-21 1991-01-21 Discharge-exciting type laser

Country Status (1)

Country Link
JP (1) JPH04236474A (en)

Similar Documents

Publication Publication Date Title
US5247531A (en) Apparatus for preionizing apulsed gas laser
US6456643B1 (en) Surface preionization for gas lasers
JPH04236474A (en) Discharge-exciting type laser
US4788691A (en) Method for the operation of a gas laser and a gas laser operated in accord therewith
JP2996706B2 (en) Pulse laser oscillation device
JPH0484474A (en) Laser apparatus
JPH0337318B2 (en)
JP2002151762A (en) Gas laser device
JP2614231B2 (en) Gas laser device
JPS622678A (en) Gas laser oscillator
JPS6321885A (en) Discharge type gas laser
JP3627193B2 (en) Laser corona preionizer
JPH04105378A (en) Discharge-excited excimer laser device
JPS63228681A (en) Gas laser oscillator
JPH01194481A (en) Gas laser oscillating apparatus
JPH05283777A (en) Gas laser oscillation device
JPH0389572A (en) Pulse laser device
JPS61251087A (en) Discharge excitation type short pulse laser device
JPS63228776A (en) Gas laser device
JPH053153B2 (en)
JPH0276281A (en) Pulse laser oscillator
JPS62139372A (en) Discharge excitation type short pulse laser device
JPS61188982A (en) Discharge excitation type short pulse laser device
JPS6062184A (en) Nitrogen laser device
JPH10150237A (en) Excimer laser device