JPH0422179A - Laser oscillator - Google Patents

Laser oscillator

Info

Publication number
JPH0422179A
JPH0422179A JP12713490A JP12713490A JPH0422179A JP H0422179 A JPH0422179 A JP H0422179A JP 12713490 A JP12713490 A JP 12713490A JP 12713490 A JP12713490 A JP 12713490A JP H0422179 A JPH0422179 A JP H0422179A
Authority
JP
Japan
Prior art keywords
discharge
tube
anode
tip part
cathode
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
JP12713490A
Other languages
Japanese (ja)
Inventor
Hidehiko Karasaki
秀彦 唐崎
Shuzo Yoshizumi
吉住 修三
Akio Tanaka
田中 昭男
Shigeki Yamane
茂樹 山根
Tsutomu Sugiyama
勤 杉山
Hitoshi Motomiya
均 本宮
Masashi Onishi
正史 大西
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 JP12713490A priority Critical patent/JPH0422179A/en
Publication of JPH0422179A publication Critical patent/JPH0422179A/en
Pending legal-status Critical Current

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  • Lasers (AREA)

Abstract

PURPOSE:To reduce an influence by an electric field formed in the tip part on an electric discharge operation, to enhance the stability of the electric discharge operation and to prevent a change in a laser output by a method wherein a firing auxiliary tube is installed and the cross-sectional face in its tip part is worked to be a round and protrusionless shape. CONSTITUTION:A firing auxiliary tube 10a is attached to a tube body of a discharge-tube group 1 situated between an anode 2a and a cathode 3a; and it is connected electrically to the anode 2a. Since the cross-sectional shape in the tip part of the tube 10a is formed to be a round and protrusionless shape, an electric field generated near the tip part does not generate an equipotential line which is swollen toward the inside of a discharge tube. Consequently, it is not required to form an electromagnetic lens inside the discharge tube, and also a streamer is not formed near the tip part of the auxiliary tube 10a when a pulse is oscillated (in a state that the pulse in a pulse-train shape is output on a fixed cycle). Consequently, an electric discharge at a laser oscillator is stabilized, and a stable laser output without change can be obtained.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は切断、溶接、熱処理などのためにレザ光を発生
させるレーザ発振器に関する。
DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a laser oscillator that generates laser light for cutting, welding, heat treatment, and the like.

従来の技術 従来のこの種のレーザ発振器の構成について第3図を用
いて説明する。1または複数の放電管からなる放電管群
1には、各放電管ごとに陽極2a。
2. Description of the Related Art The structure of a conventional laser oscillator of this type will be described with reference to FIG. A discharge tube group 1 consisting of one or more discharge tubes includes an anode 2a for each discharge tube.

2bと陰極3a 、sbからなる1組の放電電極が具備
されており、第3図の例では2組の放電管が形成され、
2組の放電管は対称に配置されて放電管群1が形成され
、それぞれの放電管に高圧電源4から電力が供給される
。また、放電管群1の両端には出力ミラー5.終端ミラ
ー6が配設されて光共振器を形成している。さらに、放
電管群1の両端部分の陰極型1i3a、3b近傍と中央
部の陽極電1i2a、2b間はほぼE字形の循環管体7
により接続されてガス循環路が形成され、この循環管体
7にはガスを循環させる送風機8や、ガスを冷却する複
数の熱交換器9が配設されている。まだ、放電管の外周
には放電開始補助管10a。
A set of discharge electrodes consisting of a cathode 2b, a cathode 3a, and a cathode 3a and sb are provided, and in the example shown in FIG. 3, two sets of discharge tubes are formed.
The two sets of discharge tubes are arranged symmetrically to form a discharge tube group 1, and power is supplied to each discharge tube from a high voltage power source 4. Further, output mirrors 5. are provided at both ends of the discharge tube group 1. A termination mirror 6 is arranged to form an optical resonator. Further, a circulating tube body 7 having an approximately E-shape is formed between the cathode types 1i3a, 3b at both ends of the discharge tube group 1 and the anode electrodes 1i2a, 2b at the center.
are connected to form a gas circulation path, and this circulation tube body 7 is provided with a blower 8 for circulating gas and a plurality of heat exchangers 9 for cooling the gas. There is still a discharge starting auxiliary tube 10a on the outer periphery of the discharge tube.

10bが具備されており、陽(至)2a、2bまたは陰
極3a 、3bと電気的に接続されている。
10b, and is electrically connected to the positive electrodes 2a, 2b or the negative electrodes 3a, 3b.

次に第4図Aに右側の放電管部の拡大図を示す。Next, FIG. 4A shows an enlarged view of the discharge tube section on the right side.

第4図Aより明らかなように各放電管には陽極2aと陰
1i3aからなる1組の放電電極が具備されており、放
電管管体でつながれて放電部を形成している。まだ、陽
極2aまたは陰極3aと電気的に接続された放電開始補
助管10 aが配置されており、前記放電開始補助管1
0aの先端部は材料切断時にできる鋭いエツジやパリな
どの突起形状を残したまま使用されていた。
As is clear from FIG. 4A, each discharge tube is equipped with a set of discharge electrodes consisting of an anode 2a and a cathode 1i3a, which are connected by a discharge tube body to form a discharge section. The discharge starting auxiliary tube 10a electrically connected to the anode 2a or the cathode 3a is still arranged, and the discharge starting auxiliary tube 10a is still arranged.
The tip of 0a was used with the sharp edges and protrusions created when cutting the material left intact.

このように構成されているレーザ発振器は、ガス流方向
と放電方向とレーザ光の発振軸が同軸であるため光軸方
向から見たときに、その放電およびその放電によって形
成されるゲイン分布が同心で対称性がよい。したがって
、出力されるレーザ光を用いて加工を行う場合加工性能
が良いとされている。
In a laser oscillator configured in this way, the gas flow direction, the discharge direction, and the laser beam oscillation axis are coaxial, so when viewed from the optical axis direction, the discharge and the gain distribution formed by the discharge are concentric. It has good symmetry. Therefore, it is said that the machining performance is good when machining is performed using the output laser light.

発明が解決しようとする課題 しかしながら、放電開始補助管10 a 、 10 b
の先端部から発生する電磁レンズ状の電界の影響で、特
にパルス発振時(パルス列状に定周期で断続出力する状
態)に放電開始補助管の先端部の近傍において放電管中
央部に大きなス) IJ−マが形成され、放電が不安定
になりレーザ出力変動が大きくなるという課題があった
Problems to be Solved by the Invention However, the discharge starting auxiliary tubes 10a, 10b
Due to the influence of the electromagnetic lens-shaped electric field generated from the tip of the discharge tube, a large gap may appear in the center of the discharge tube near the tip of the discharge starting auxiliary tube, especially during pulse oscillation (a state in which the pulse train is output intermittently at regular intervals). There was a problem that an IJ-ma was formed, the discharge became unstable, and the laser output fluctuation increased.

課題を解決するだめの手段 本発明は上記課題を解決するために、陽極と陰極の間に
ある放電管の外周に取り付けられ陽極または陰極と電気
的に接続された放電開始補助管の先端部の縦断面を丸く
突起のない形状に加工するものである。
Means for Solving the Problems In order to solve the above-mentioned problems, the present invention provides a discharge starting auxiliary tube which is attached to the outer periphery of the discharge tube between the anode and the cathode and is electrically connected to the anode or the cathode. The vertical section is processed into a round shape without protrusions.

作   用 本発明によれば放電開始補助管の先端部が作る電界が放
電管内部に大きく回り込んで電磁レンズ状となることを
防ぎ、電界が放電に及ぼす影響を軽減し、放電の安定性
を向上させてレーザ出力の変動をなくすことができる。
Effect: According to the present invention, the electric field generated by the tip of the discharge starting auxiliary tube is prevented from wrapping around the inside of the discharge tube to form an electromagnetic lens shape, reducing the influence of the electric field on the discharge, and improving the stability of the discharge. It is possible to improve this and eliminate fluctuations in laser output.

実施例 以下、本発明の実施例を図を用いて説明する。Example Embodiments of the present invention will be described below with reference to the drawings.

第1図に本発明の一実施例を示した。第1図は放電管群
1の右側に位置する放電管部を示しているが、左側の放
電管部はこれと対称の関係にあり、本発明の効果は同じ
である。第1図Aにおいて、10aは放電開始補助管で
あり陽極2aに電気的に接続されている。3aは陰極、
1は放電管群の管体である。第1図Bは第1図Aにおけ
る要部の縦断面拡大図であり、本発明における放電開始
補助管10aの先端部近傍を示しており先端部縦断面は
丸く突起のない形状となっている。11は放電開始補助
管を放電管群の管体から一定の距離に保つだめのヌペー
サである。
FIG. 1 shows an embodiment of the present invention. Although FIG. 1 shows the discharge tube section located on the right side of the discharge tube group 1, the discharge tube section on the left side is in a symmetrical relationship with this, and the effects of the present invention are the same. In FIG. 1A, 10a is a discharge starting auxiliary tube, which is electrically connected to the anode 2a. 3a is a cathode,
1 is a tube body of a group of discharge tubes. FIG. 1B is an enlarged vertical cross-sectional view of the main part in FIG. 1A, showing the vicinity of the tip of the discharge starting auxiliary tube 10a in the present invention, and the vertical cross-section of the tip has a round shape without protrusions. . Reference numeral 11 denotes a nupacer for keeping the discharge starting auxiliary tube at a constant distance from the tube bodies of the discharge tube group.

第4図に従来例における放電管部を示しているが、放電
開始補助管の先端断面は第4図Bに示すように管先端に
は切断加工時に生じた鋭いパリが管の内側に向って残存
している。このように内側に向う鋭いパリは放電時に第
6図に示すように、放電管の内側に向ってふくらんだ電
界を作る。図で破線は電界の等電位線を示しており放電
管の内側にふくらんだ等電位部は、放電管と同心で円を
画くため放電等の内部に電磁レンズを形成することにな
り、放電管中央部に大きなメトリーマを形成し、放電を
不安定にし、レーザ出力を変動させる原因となっていた
Figure 4 shows the discharge tube section in a conventional example, and the cross-section of the tip of the discharge starting auxiliary tube shows that, as shown in Figure 4B, the tip of the tube has sharp burrs that are produced during the cutting process toward the inside of the tube. remains. These sharp points pointing inward create an electric field that bulges inward of the discharge tube during discharge, as shown in FIG. 6. In the figure, the broken lines indicate the equipotential lines of the electric field, and the equipotential part bulging inside the discharge tube forms a circle concentrically with the discharge tube, forming an electromagnetic lens inside the discharge tube. A large metrimer was formed in the center, making the discharge unstable and causing fluctuations in laser output.

これに対し第1図Bに示す先端形状の放電開始補助管の
先端近傍に発生する電界は第2図に示す通りで、放電管
の内側に向ってふくらむ等電位線はない。従って本発明
によれば放電管内に電磁レンズを形成することがなくな
り、ストリーマも形成されず、しだがって放電は安定化
しレーザ出力の変動もなくなる。
On the other hand, the electric field generated near the tip of the discharge starting auxiliary tube having the tip shape shown in FIG. 1B is as shown in FIG. 2, and there is no equipotential line that swells toward the inside of the discharge tube. Therefore, according to the present invention, there is no need to form an electromagnetic lens within the discharge tube, no streamer is formed, and therefore the discharge is stabilized and fluctuations in laser output are eliminated.

発明の効果 以上の説明から明らかなように本発明によれば、レーザ
発振器における放電を安定化し、変動のない安定なレー
ザ出力を得ることができる。
Effects of the Invention As is clear from the above description, according to the present invention, the discharge in the laser oscillator can be stabilized, and stable laser output without fluctuation can be obtained.

【図面の簡単な説明】 第1図Aは本発明の一実施例における放電管部の構成を
示す縦断面図、第1図Bは同図Aの要部の拡大縦断面図
、第2図は本発明による放電開始補助管先端近傍に発生
する電界の状態を示す図、第3図はレーザ発振器全体の
構成を示す図、第4図Aは従来例における放電管部の構
成を示す縦断面図、第4図Bは同図への要部の拡大縦断
面図、第5図は従来例における放電開始補助管先端近傍
に発生する電界の状斡を示す図である。 1・・・・・放電管群、2a 、2b・・・・・陽匣、
3a。 3b・・・・陰極、4・・・・・高電圧電源、6・・・
・・出力ミラー 6・・・・・終端ミラー 7・・・・
・・循環管体、8・・・・送風機、9・・・・・熱交換
器、10 a 、 10 b・・放電開始補助管、11
・・・・・ヌペーサ。 代理人の氏名 弁理士 粟 野 重 孝 ほか1名〜 (Oa7 第 図 09ツ ノOa 第 図 第 図 ん−2b 3a、 3b toa、rob 放電管群 陽   物 Fl& & 電 圧 電 源 出  υ  ;  ラ  − N側御ミラ l11IIW  琶 を杢 Ll、  闇 艷 ? タ 換 ム 放電藺始桶1W
[BRIEF DESCRIPTION OF THE DRAWINGS] FIG. 1A is a vertical cross-sectional view showing the configuration of a discharge tube section in an embodiment of the present invention, FIG. 1B is an enlarged vertical cross-sectional view of the main part of FIG. 3 is a diagram showing the state of the electric field generated near the tip of the discharge starting auxiliary tube according to the present invention, FIG. 3 is a diagram showing the configuration of the entire laser oscillator, and FIG. 4A is a longitudinal section showing the configuration of the discharge tube section in the conventional example. 4B is an enlarged vertical sectional view of the main part of the same figure, and FIG. 5 is a diagram showing the state of the electric field generated near the tip of the discharge starting auxiliary tube in the conventional example. 1...discharge tube group, 2a, 2b...positive box,
3a. 3b...Cathode, 4...High voltage power supply, 6...
...Output mirror 6...Terminal mirror 7...
...Circulation pipe body, 8...Blower, 9...Heat exchanger, 10 a, 10 b...Discharge starting auxiliary pipe, 11
...Nupesa. Name of agent Patent attorney Shigetaka Awano and 1 other person (Oa7 Figure 09 Horn Oa Figure Figure 2-2b 3a, 3b toa, rob Discharge tube group positive material Fl && Voltage Power source υ; Ra - N side mirror l11IIW 琶 杢Ll, darkness 艷?Tam exchange discharge time 1W

Claims (1)

【特許請求の範囲】[Claims] 陽極と陰極とからなる少なくとも一対の放電電極を有し
1または複数の放電管からなる放電管群と、この放電群
の両端に配備されるレーザ共振用のミラーと、前記放電
電極の近傍で前記放電群に接続されこの放電群とともに
ガス循環路を構成する循環管体と、前記ガス循環路にレ
ーザ媒質としてのガスを循環させる送風機とからなり、
前記陽極と陰極の間にある放電管の外周に取り付けられ
陽極または陰極に電気的に接続された放電開始補助管の
先端部縦断面を丸く突起のない形状に加工したことを特
徴とするレーザ発振器。
A discharge tube group consisting of one or more discharge tubes and having at least one pair of discharge electrodes consisting of an anode and a cathode, a mirror for laser resonance disposed at both ends of this discharge group, and a It consists of a circulation pipe connected to the discharge group and forming a gas circulation path together with the discharge group, and a blower that circulates gas as a laser medium in the gas circulation path,
A laser oscillator characterized in that a longitudinal section of a distal end of a discharge starting auxiliary tube attached to the outer periphery of the discharge tube between the anode and the cathode and electrically connected to the anode or the cathode is processed into a round shape without protrusions. .
JP12713490A 1990-05-17 1990-05-17 Laser oscillator Pending JPH0422179A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP12713490A JPH0422179A (en) 1990-05-17 1990-05-17 Laser oscillator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP12713490A JPH0422179A (en) 1990-05-17 1990-05-17 Laser oscillator

Publications (1)

Publication Number Publication Date
JPH0422179A true JPH0422179A (en) 1992-01-27

Family

ID=14952459

Family Applications (1)

Application Number Title Priority Date Filing Date
JP12713490A Pending JPH0422179A (en) 1990-05-17 1990-05-17 Laser oscillator

Country Status (1)

Country Link
JP (1) JPH0422179A (en)

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