JPH05226742A - Laser oscillator - Google Patents

Laser oscillator

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Publication number
JPH05226742A
JPH05226742A JP2877692A JP2877692A JPH05226742A JP H05226742 A JPH05226742 A JP H05226742A JP 2877692 A JP2877692 A JP 2877692A JP 2877692 A JP2877692 A JP 2877692A JP H05226742 A JPH05226742 A JP H05226742A
Authority
JP
Japan
Prior art keywords
frequency power
discharge tube
high frequency
laser oscillator
laser
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
JP2877692A
Other languages
Japanese (ja)
Inventor
Hidehiko Karasaki
秀彦 唐▲崎▼
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP2877692A priority Critical patent/JPH05226742A/en
Publication of JPH05226742A publication Critical patent/JPH05226742A/en
Pending legal-status Critical Current

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  • Lasers (AREA)

Abstract

PURPOSE:To prevent a reduction in a laser oscillation efficiency caused by high frequency power differences which are produced by impedance differences in a discharge tube and which are injected in the discharge tube in the case where a high frequency power source through a matching circuit is combined with a laser oscillator to discharge. CONSTITUTION:A variable capacitor 15 is provided in the vicinity of at least an electrode 6, whereby fine impedance differences in a plurality of discharge tubes are corrected so that a high frequency power derived from a high frequency power source part 14 can uniformly be injected to each of the discharge tubes through a matching circuit 13.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は発生したレーザ光を利用
して、金属などを切断、溶接、熱処理などを行なう工業
用レーザ発振器に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an industrial laser oscillator that cuts, welds, heat-treats metal or the like by utilizing generated laser light.

【0002】[0002]

【従来の技術】近年、金属加工機として工業用ガスレー
ザ装置の需要が増加するとともに、その改善が望まれて
きた。
2. Description of the Related Art In recent years, as the demand for industrial gas laser devices as metal working machines has increased, improvements have been desired.

【0003】以下に従来のレーザ発振器について図面を
参照しながら説明する。図2に示すように高速軸流型と
言われているガスレーザ発振器は、出力鏡1、出力鏡ホ
ルダー2、メインフランジ3、集合ブロック4、放電管
5、電極6、折り返しブロック7、終端鏡ホルダー8、
終端鏡9、熱交換器10、ガス配管11、送風器12で
構成されている。
A conventional laser oscillator will be described below with reference to the drawings. As shown in FIG. 2, the gas laser oscillator, which is called a high-speed axial flow type, includes an output mirror 1, an output mirror holder 2, a main flange 3, an assembly block 4, a discharge tube 5, an electrode 6, a folding block 7, and a terminal mirror holder. 8,
It is composed of a terminal mirror 9, a heat exchanger 10, a gas pipe 11, and a blower 12.

【0004】以上の構成要素よりなるレーザ発振器につ
いて、以下その各構成要素の関係と動作を説明する。ま
ず、メインフランジ3、集合ブロック4、放電管5、熱
交換器10、ガス配管11、送風器12から構成される
真空容器にレーザ媒質ガスを充満し、一定の圧力で保持
すると同時に送風器12でレーザ媒質ガスを循環させ
る。循環させたレーザ媒質ガスに外部に設けられた高周
波電源部から電極6を介して高周波電力を放電管5に注
入し、レーザ媒質ガスを放電させ、レーザ光を発生させ
る。発生したレーザ光は出力鏡1、折り返しブロック
7、終端鏡9から構成される光共振器で増幅され、その
一部が出力鏡1から外部に取りだされ、加工に利用され
る。この際放電管5で発生した熱を除去しレーザ媒質ガ
スを冷却する目的でガス配管11の途中に熱交換器10
が設けられている。さらに、光共振器を構成するために
は出力鏡1と終端鏡9が折り返しブロック7を介して平
行に維持される必要があり、そのため出力鏡ホルダー2
と終端鏡ホルダー8を用いて微調整を行なう。また、メ
インフランジ3と、集合ブロック4は構造的に強固にで
きていて、熱膨張や外力に対して出力鏡1と終端鏡9の
角度が変化しないように十分な強度を有している。
With respect to the laser oscillator having the above components, the relationship and operation of each component will be described below. First, the laser medium gas is filled in a vacuum container composed of the main flange 3, the assembly block 4, the discharge tube 5, the heat exchanger 10, the gas pipe 11, and the blower 12, and the blower 12 is held at a constant pressure. To circulate the laser medium gas. High-frequency power is injected into the circulated laser medium gas from the external high-frequency power source through the electrode 6 into the discharge tube 5 to discharge the laser medium gas and generate laser light. The generated laser light is amplified by an optical resonator composed of the output mirror 1, the folding block 7, and the terminal mirror 9, and a part of the laser light is taken out from the output mirror 1 and used for processing. At this time, in order to remove the heat generated in the discharge tube 5 and cool the laser medium gas, the heat exchanger 10 is provided in the middle of the gas pipe 11.
Is provided. Further, in order to form the optical resonator, the output mirror 1 and the terminal mirror 9 need to be maintained in parallel via the folding block 7, and therefore the output mirror holder 2
And the end mirror holder 8 are used for fine adjustment. Further, the main flange 3 and the assembly block 4 are structurally strong, and have sufficient strength so that the angle between the output mirror 1 and the terminal mirror 9 does not change due to thermal expansion or external force.

【0005】つぎに、図4に示すように従来の高周波電
源部14とレーザ発振器の一般的な接続方法では、整合
回路13が高周波電源部14と電極6の間に設けられ高
周波電源部14からは一般に出力インピーダンス50オ
ームの同軸ケーブル17で出力され整合回路13に接続
される。整合回路13からは銅板18などで放電管5ご
とに設けた電極6に並列接続され、高周波電力が伝送さ
れる。
Next, as shown in FIG. 4, in a general connection method of the conventional high frequency power supply unit 14 and the laser oscillator, the matching circuit 13 is provided between the high frequency power supply unit 14 and the electrode 6 and Is generally output by a coaxial cable 17 having an output impedance of 50 ohms and is connected to the matching circuit 13. The matching circuit 13 is connected in parallel to the electrode 6 provided for each discharge tube 5 with a copper plate 18 or the like, and high frequency power is transmitted.

【0006】[0006]

【発明が解決しようとする課題】しかしながら上記従来
の構成では、実際に高周波電源部を整合回路を介してレ
ーザ発振器を構成する放電管の電極に接続すると、放電
管電極の微妙なインピーダンスの差から高周波電力が各
放電管電極に均等に注入されず発振効率が低下するとい
う問題点を有していた。
However, in the above-mentioned conventional structure, when the high frequency power supply is actually connected to the electrodes of the discharge tube constituting the laser oscillator through the matching circuit, a slight difference in impedance between the electrodes of the discharge tube is caused. There is a problem that high frequency power is not evenly injected into each discharge tube electrode and the oscillation efficiency is reduced.

【0007】本発明は上記従来の問題点を解決するもの
で、複数の放電管電極のインピーダンス差を補正し、発
振効率の低下を防止したレーザ発振器を提供することを
目的とする。
The present invention solves the above-mentioned conventional problems, and an object of the present invention is to provide a laser oscillator in which the impedance difference between a plurality of discharge tube electrodes is corrected and a decrease in oscillation efficiency is prevented.

【0008】[0008]

【課題を解決するための手段】上記目的を達成するため
に本発明のレーザ発振器は、少なくとも1つの電極近傍
に設けた可変コンデンサを微調整して放電管電極の微妙
なインピーダンス差を補正し、高周波電力が各放電管電
極ごとに均等に注入するような構成を有している。
To achieve the above object, the laser oscillator of the present invention corrects a delicate impedance difference between discharge tube electrodes by finely adjusting a variable capacitor provided in the vicinity of at least one electrode. The high frequency power is evenly injected into each discharge tube electrode.

【0009】[0009]

【作用】本発明は上記した構成において、高周波電源部
を整合回路を介してレーザ発振器に接続するとき、複数
の放電管電極の間で微妙なインピーダンス差があると高
周波電力が各放電管電極に均等に注入されないので、電
源の出力インピーダンスと全放電管電極のインピーダン
ス整合するために整合回路を設けている。レーザ媒質ガ
スの圧力差があると、複数の放電管でのインピーダンス
差は無視され、各放電管に注入される高周波電力に差が
発生する。各放電管電極に注入された高周波電力の差は
その放電管を通過するレーザ媒質ガスに温度差を発生さ
せる。レーザの発振効率はある温度をこえると顕著に低
下するため、1本でもその限界温度を越える放電管が存
在すると全体のレーザ発振効率に影響を与える。そこ
で、各放電管の近傍に少なくとも1つの可変コンデンサ
を設け放電管の微妙なインピーダンス差を補正し、高周
波電力を各放電管ごとに均等に注入できることとなる。
According to the present invention, in the above structure, when the high frequency power source is connected to the laser oscillator through the matching circuit, if there is a slight impedance difference between the plurality of discharge tube electrodes, the high frequency power is applied to each discharge tube electrode. Since it is not injected evenly, a matching circuit is provided to match the output impedance of the power supply with the impedance of all discharge tube electrodes. If there is a pressure difference in the laser medium gas, the impedance difference between the plurality of discharge tubes is ignored, and a difference occurs in the high frequency power injected into each discharge tube. The difference in the high frequency power injected into each discharge tube electrode causes a temperature difference in the laser medium gas passing through the discharge tube. Since the oscillation efficiency of the laser decreases remarkably when the temperature exceeds a certain temperature, the presence of even one discharge tube exceeding the limit temperature affects the overall laser oscillation efficiency. Therefore, at least one variable capacitor is provided in the vicinity of each discharge tube to correct a slight impedance difference between the discharge tubes, and high-frequency power can be evenly injected into each discharge tube.

【0010】[0010]

【実施例】以下、本発明の一実施例について、図面を参
照しながら説明する。レーザ発振器そのものの構成は従
来例で説明した図2に示すものと同一であり、説明は省
略し、特に放電管と高周波電源の接続周辺について説明
する。図1に示すように本実施例のレーザ発振器の放電
管電極6は、高周波電源部14、可変コンデンサ15、
固定コンデンサ16、整合回路13で構成される回路で
接続されている。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the present invention will be described below with reference to the drawings. The configuration of the laser oscillator itself is the same as that shown in FIG. 2 described in the conventional example, and the description thereof is omitted. In particular, the connection peripheral of the discharge tube and the high frequency power source will be described. As shown in FIG. 1, the discharge tube electrode 6 of the laser oscillator of the present embodiment includes a high frequency power supply unit 14, a variable capacitor 15,
They are connected by a circuit composed of a fixed capacitor 16 and a matching circuit 13.

【0011】以上の構成要素よりなるレーザ発振器の電
極回路について、図1および図2を用いてその構成要素
の関係と動作を説明する。まず、整合回路13は放電管
5の電極6からみた高周波電源部14の出力インピーダ
ンスと全電極6のインピーダンスを整合させており、本
実施例ではその整合点よりややコンデンサ成分が低い値
に設定され、実際は固体コンデンサ16と合わせてその
電極6のインピーダンスに整合している。固体コンデン
サ16の値は可変コンデンサ15の可変範囲の中心値と
同値に設定している。したがって、レーザ媒質ガスの圧
力差などで複数の放電管の間で電極6のインピーダンス
差がある場合は、残りの電極に設けられた可変コンデン
サ15の値を調整し、各電極6に注入される高周波電力
の差が発生しないようにする。各放電管に注入された高
周波電力の差を軽減するとその放電管を通過するレーザ
媒質ガスの温度に差が減少し、全体のレーザ発振効率を
高い水準で維持できる。
With respect to the electrode circuit of the laser oscillator including the above components, the relationship and operation of the components will be described with reference to FIGS. 1 and 2. First, the matching circuit 13 matches the output impedance of the high frequency power supply unit 14 as viewed from the electrode 6 of the discharge tube 5 and the impedance of all the electrodes 6, and in this embodiment, the capacitor component is set to a value slightly lower than the matching point. Actually, the impedance of the electrode 6 is matched with the solid capacitor 16. The value of the solid capacitor 16 is set to the same value as the center value of the variable range of the variable capacitor 15. Therefore, when there is a difference in the impedance of the electrodes 6 among the plurality of discharge tubes due to the pressure difference of the laser medium gas, etc., the value of the variable capacitor 15 provided on the remaining electrodes is adjusted and injected into each electrode 6. Make sure there is no difference in high frequency power. When the difference in the high frequency power injected into each discharge tube is reduced, the difference in the temperature of the laser medium gas passing through the discharge tube is reduced, and the overall laser oscillation efficiency can be maintained at a high level.

【0012】[0012]

【発明の効果】以上の実施例から明らかなように本発明
によれば、複数の放電管電極間のインピーダンスのばら
つきが大きくても各電極に加えられる高周波電力の差を
少なくすることができる。図3に従来の技術で説明した
図4の回路の場合と、本実施例で説明した図1の回路の
場合について、測定値の比較に示すように、放電管電極
の複素インピーダンスのばらつき幅に対して放電管電極
への注入高周波電力のばらつきが、本実施例によれば数
%改善されることがわかる。以上の結果として発振効率
の高い優れたレーザ発振器を実現できるものである。
As is apparent from the above embodiments, according to the present invention, it is possible to reduce the difference in the high frequency power applied to each electrode even if there are large variations in the impedance between the plurality of discharge tube electrodes. As shown in the comparison of the measured values between the case of the circuit of FIG. 4 described in FIG. 3 of the related art and the case of the circuit of FIG. 1 described in the present embodiment, the variation width of the complex impedance of the discharge tube electrode On the other hand, it can be seen that the variation of the high frequency power injected into the discharge tube electrode is improved by several% according to the present embodiment. As a result of the above, an excellent laser oscillator with high oscillation efficiency can be realized.

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

【図1】本発明の一実施例のレーザ発振器の電源回路図FIG. 1 is a power supply circuit diagram of a laser oscillator according to an embodiment of the present invention.

【図2】ガスレーザ発振器の構成断面図FIG. 2 is a sectional view showing the configuration of a gas laser oscillator.

【図3】放電管電極注入電力のインピーダンス特性図FIG. 3 is an impedance characteristic diagram of electric power injected into a discharge tube electrode.

【図4】従来のレーザ発振器の電源回路図FIG. 4 is a power supply circuit diagram of a conventional laser oscillator.

【符号の説明】[Explanation of symbols]

1 出力鏡 5 放電管 6 電極 9 終端鏡 11 ガス配管 12 送風器 13 整合回路 14 高周波電源部 15 可変コンデンサ 1 Output Mirror 5 Discharge Tube 6 Electrode 9 Terminal Mirror 11 Gas Pipe 12 Blower 13 Matching Circuit 14 High Frequency Power Supply 15 Variable Capacitor

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】複数の放電管と、その両端に出力鏡と終端
鏡を具備したレーザ共振器と前記各放電管に接続したガ
ス配管に送風器を設け前記ガス配管内にガスを循環し、
前記各放電管の外部にほぼ平行に配した電極を介して外
部の高周波電源部より高周波電力を伝送し放電させるこ
とでレーザ光を発生せしめ、前記高周波電源部と前記電
極の間に整合回路を設け、さらに少なくとも1つの前記
電極の近傍に可変コンデンサを配してなるレーザ発振
器。
1. A plurality of discharge tubes, a laser resonator having output mirrors and terminal mirrors at both ends thereof, and a gas pipe connected to each of the discharge tubes is provided with an air blower to circulate gas in the gas pipes.
Laser light is generated by transmitting and discharging high-frequency power from an external high-frequency power source through electrodes arranged substantially parallel to the outside of each discharge tube, and a matching circuit is provided between the high-frequency power source and the electrodes. A laser oscillator provided with a variable capacitor disposed in the vicinity of at least one of the electrodes.
JP2877692A 1992-02-17 1992-02-17 Laser oscillator Pending JPH05226742A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2877692A JPH05226742A (en) 1992-02-17 1992-02-17 Laser oscillator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2877692A JPH05226742A (en) 1992-02-17 1992-02-17 Laser oscillator

Publications (1)

Publication Number Publication Date
JPH05226742A true JPH05226742A (en) 1993-09-03

Family

ID=12257812

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2877692A Pending JPH05226742A (en) 1992-02-17 1992-02-17 Laser oscillator

Country Status (1)

Country Link
JP (1) JPH05226742A (en)

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