JPH0240974A - Gas laser oscillator - Google Patents

Gas laser oscillator

Info

Publication number
JPH0240974A
JPH0240974A JP19173288A JP19173288A JPH0240974A JP H0240974 A JPH0240974 A JP H0240974A JP 19173288 A JP19173288 A JP 19173288A JP 19173288 A JP19173288 A JP 19173288A JP H0240974 A JPH0240974 A JP H0240974A
Authority
JP
Japan
Prior art keywords
tube
discharge tube
discharge
laser
wall
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
JP19173288A
Other languages
Japanese (ja)
Inventor
Hitoshi Motomiya
均 本宮
Naoya Horiuchi
直也 堀内
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 JP19173288A priority Critical patent/JPH0240974A/en
Publication of JPH0240974A publication Critical patent/JPH0240974A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S3/00Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
    • H01S3/09Processes or apparatus for excitation, e.g. pumping
    • H01S3/097Processes or apparatus for excitation, e.g. pumping by gas discharge of a gas laser
    • H01S3/0975Processes or apparatus for excitation, e.g. pumping by gas discharge of a gas laser using inductive or capacitive excitation

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Engineering & Computer Science (AREA)
  • Plasma & Fusion (AREA)
  • Optics & Photonics (AREA)
  • Lasers (AREA)

Abstract

PURPOSE:To realize high efficiency of laser oscillation by installing a protruding stripes along the tube axis on the inner wall, of a discharge tube, corresponding with the end-egdes of metal electodes. CONSTITUTION:The inner diameter of a cylindrical discharge tube 1 is 200mm, and the radial thickness is about 3mm. Along the tube axis, four semi-columnar protruding stripes are formed on the inner wall part, of discharge tube, corresponding with the end-edges 2a, 3a of a pair of metal electrodes 2, 3 in the axial direction of external peripheral surface of the tube 1. The radial thickness of these parts only become thick, and the concentration of electric field can be avoided. Further, the tube wall of other parts do not obstruct power injection, so that laser beam can be led out with high efficiency.

Description

【発明の詳細な説明】 〔産業上の利用分野〕゛ 本発明は、放電管の軸方向と光軸方向が一致したガスレ
ーザ発振装置に係り、特に、レーザ発振の高効率化を図
ったガスレーザ発振装置に関するものである。
[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a gas laser oscillation device in which the axial direction of a discharge tube and the optical axis direction are aligned, and particularly relates to a gas laser oscillation device that achieves high laser oscillation efficiency. It is related to the device.

〔従来の技術〕[Conventional technology]

従来、この種のガスレーザ発振装置としては例えば第3
図および第4図に示すように、ガラス等の誘電体よりな
る円筒状の放電管(1)の外周面管軸方向の両側2箇所
に所定間隔を設けて一対の金属電極(2)(3)を仔い
に対向状に密着して配設すると共に、これら一対の金属
電極(2)(3)を高周波交流電源(4)に接続して、
両電極(2)(3)に例えば13.56MHz 、2k
Vの高周波高電圧を印加する一方、両金属電極(2)(
3)間に挟まれた放電管(1)内の放電空間(5)の両
端に全反射鏡(6)と部分反射鏡(7)とを固定位置に
配設して、これら全反射鏡(6)および部分反射鏡(7
)により光共振器を構成してあり、また、前記放電管(
+)の両電極(2)(3)間の中央から送気管(8)を
連通状態で設けると共に、放電管(1)の両端側と送気
管(8)の他端間に−・対の分岐管(9)(10)を両
管(+)(8)と連通状態で配設して、放電管(1)の
中央から2方向に分岐する一対の循環通路を構成し、史
に、前記送気管(8)の途中部に送風機(11)を設け
て、この送風機(11)の両側方となる送気管(8)中
に、放電空間(5)中での放電および送風機(11)の
駆動によりh’ 7Mしたレーザガスを冷却する熱交換
器(12)(+3)を配設してなる、いわゆる軸流型の
がスレーザ発振装置が知られている。
Conventionally, as this type of gas laser oscillation device, for example, the third
As shown in FIG. 4 and FIG. 4, a pair of metal electrodes (2) (3 ) are arranged in close contact with each other facing each other, and the pair of metal electrodes (2) and (3) are connected to a high frequency AC power source (4),
For example, 13.56MHz, 2k for both electrodes (2) and (3).
While applying a high frequency high voltage of V, both metal electrodes (2) (
3) A total reflection mirror (6) and a partial reflection mirror (7) are arranged at fixed positions at both ends of the discharge space (5) in the discharge tube (1) sandwiched between them, and these total reflection mirrors ( 6) and partially reflective mirror (7
) constitutes an optical resonator, and the discharge tube (
An air pipe (8) is provided in communication from the center between the electrodes (2) and (3) of the discharge tube (1), and a pair of - and air pipes are provided between both ends of the discharge tube (1) and the other end of the air pipe (8). The branch pipes (9) and (10) are arranged in communication with both pipes (+) and (8) to form a pair of circulation passages branching in two directions from the center of the discharge tube (1). A blower (11) is provided in the middle of the air pipe (8), and the air discharge in the discharge space (5) and the blower (11) are provided in the air pipe (8) on both sides of the air pipe (11). A so-called axial flow type laser oscillation device is known, which is provided with a heat exchanger (12) (+3) for cooling the laser gas heated to h' 7M by driving.

なお、1Fi記送風機(II)としては、放電空間(5
)において流速が約100m/see程度のガス流を得
ることができる程度の送風能力を備えたものを使用する
必要がある。
In addition, as a 1 Fi blower (II), a discharge space (5
), it is necessary to use one that has an air blowing capacity that can obtain a gas flow with a flow velocity of about 100 m/see.

L記構成の従来装置では、まず、一対の金属電極(2H
3)に高周波電源(4)から高周波高電圧を印加して放
電空間(5)にグロー状の放電を発生させると、この放
電空間(5)を通過するレーザガスは前記放−hエネル
ギーを得て励起されると共に、全反射鏡(6)および)
1り分厚射鏡(7)により形成された光共振器の作用に
より共振状態となり、これによって部分反射鏡(7)か
らレーザビーム(B)が出力され、このレーザビーム(
B)をレーザ加1.1の用途に供することになる。
In the conventional device having the configuration L, first, a pair of metal electrodes (2H
When a high-frequency high voltage is applied from the high-frequency power source (4) to 3) to generate a glow-like discharge in the discharge space (5), the laser gas passing through the discharge space (5) obtains the emitted-h energy. Excited, total reflection mirror (6) and)
Due to the action of the optical resonator formed by the mirror (7) with a thickness of 1.5 mm, a resonant state is created, and as a result, a laser beam (B) is output from the partially reflecting mirror (7), and this laser beam (
B) will be used for laser processing 1.1.

ところで、[−記のように金属電極(2)(31間に高
周波高電圧を印加してレーザビーム(B)をjする場合
、画電極(2)(3)のエツジ(2a)(3a)に電界
が集中して放電状態が悪化する。特に、誘電体である放
電管(1)の誘電体損失の変化によって放電空間(5)
内に注入+1J能な電力が決定されることになる。
By the way, when applying a high frequency high voltage between the metal electrodes (2) (31 to emit the laser beam (B) as shown in [-], the edges (2a) (3a) of the picture electrodes (2) (3) The electric field concentrates in the discharge space (5), deteriorating the discharge condition.In particular, changes in the dielectric loss of the discharge tube (1), which is a dielectric material, cause the discharge space (5) to deteriorate.
The power that can be injected within +1J will be determined.

このため、放電管(1)の肉厚が薄いと放電空間(5)
の電界分布に不均一が生じて放電集中が起こり、逆に、
放電管(1)の肉厚が厚いと放電管(1)の誘電体損失
により、放電空間(5)内に注入できる電力が減少する
のであるが、従来では、放電集中の防止に力点をおき、
肉厚の大きい放電管(+)を使用していた。
For this reason, if the wall thickness of the discharge tube (1) is thin, the discharge space (5)
Non-uniformity occurs in the electric field distribution, causing discharge concentration, and conversely,
If the wall thickness of the discharge tube (1) is thick, the power that can be injected into the discharge space (5) will decrease due to the dielectric loss of the discharge tube (1), but conventionally, emphasis has been placed on preventing discharge concentration. ,
A thick discharge tube (+) was used.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

しかしながら、肉厚の大きい放電管(1)を用いた従来
のガスレーザ発振装置の場合、必然的に放電管(+)の
誘電体損失による71人電力の損失が大きくなるという
結果を招(ため、効率よくレーザビームを取り出せない
という問題点があった。
However, in the case of a conventional gas laser oscillator using a discharge tube (1) with a large wall thickness, the loss of power due to the dielectric loss of the discharge tube (+) inevitably increases. There was a problem in that the laser beam could not be extracted efficiently.

本発明は、かかる従来の問題点を解決するためになされ
たもので、放電管内の放電空間における放電集中をなく
し、しかも、放電管での注入電力の損失を最少限に抑制
し得るガスレーザ発振装置を提供することを[1的とす
るものである。
The present invention has been made in order to solve these conventional problems, and is a gas laser oscillation device that can eliminate discharge concentration in the discharge space within the discharge tube and can also minimize the loss of power injected into the discharge tube. The first objective is to provide the following.

〔課題を解決するための手段〕[Means to solve the problem]

に記[。1的を達成するために本発明は、誘電体よりな
る放電管内を光軸方向にレーザガスを流し、前記放電管
の外周面に管径方向でr7いに対向して設けられた金属
電極間に高周波電圧を印加してこの放電管内に放電を発
生させ、この放電をレーザ励起源として前記放電管の管
軸方向にレーザビームを発生するガスレーザ発振装置に
おいて、前記金属電極のエツジに対応する前記放電管の
内壁部分に管軸方向に沿う凸条を形成したことを特徴と
するものである。
Written in[. In order to achieve the first objective, the present invention allows a laser gas to flow in the optical axis direction inside a discharge tube made of a dielectric material, and creates a gap between metal electrodes provided on the outer circumferential surface of the discharge tube and facing each other in the tube diameter direction. In a gas laser oscillation device that applies a high frequency voltage to generate a discharge in the discharge tube and uses the discharge as a laser excitation source to generate a laser beam in the tube axis direction of the discharge tube, the discharge corresponding to the edge of the metal electrode It is characterized in that a protrusion is formed on the inner wall portion of the tube along the tube axis direction.

〔作   用〕[For production]

本発明は1−記構成により、金属電極のエツジに対応す
る放電管の内壁部分の肉厚のみが凸条によって1“ノ(
なっているので電界集中が回避され、しかも、放電管の
その他の部分の管壁は電力の注入を妨げない程度の厚さ
にすることができるので、レーザビームを高効率で取り
出すことがIIJ能になる。
In the present invention, according to the configuration described in 1-, only the wall thickness of the inner wall portion of the discharge tube corresponding to the edge of the metal electrode is reduced by 1"(1") by the convex strip.
This avoids electric field concentration, and the thickness of the tube wall in other parts of the discharge tube can be made to the extent that it does not interfere with power injection, making it possible to take out the laser beam with high efficiency. become.

〔実 施 例〕〔Example〕

以下、本発明の実施例を図面に基づき詳細に説明する。 Hereinafter, embodiments of the present invention will be described in detail based on the drawings.

なお、この実施例装置は、前述した従来例と基本構成が
共通しているので、構成71F2びに作用がノ(通ずる
部分は共通の符壮を付すこととし、重複を避けるために
その説明を省略するものとする。
Note that this embodiment device has the same basic configuration as the conventional example described above, so the configuration 71F2 and the function (common parts will be given common symbols, and their explanation will be omitted to avoid duplication. It shall be.

第1図において、この実施例に係るガスレーザ発振装置
においては、円筒状の放電管(1)の内径を2011I
I+に対して肉厚を31としており、この放電管(1)
の外周面の管軸方向に形成された一対の金属電極(2)
(3)のエツジ(2a)(3a)に対応する放電管(+
)の内壁部分には、それぞれ管軸方向に沿う4木の゛目
11柱状の凸条(14)を形成しである。
In FIG. 1, in the gas laser oscillation device according to this embodiment, the inner diameter of the cylindrical discharge tube (1) is 2011I.
The wall thickness is 31 for I+, and this discharge tube (1)
A pair of metal electrodes (2) formed in the tube axis direction on the outer peripheral surface of the
Discharge tubes (+) corresponding to edges (2a) and (3a) in (3)
) are formed with convex stripes (14) in the shape of 11 columns with 4 squares extending along the tube axis direction.

第2図にレーザ出力効ネ(と放電管(1)の内壁に設け
る凸条(14)の有無との関係を測定した結果を示して
おり、この結果から明らかなように、放電管(1)の内
壁に凸条(14)を設けたものは、内壁全周にtイって
均一な肉厚としたものと比較してレー炉出力効率が格段
に向にするものである。
Figure 2 shows the results of measuring the relationship between the laser output efficiency and the presence or absence of the protruding stripes (14) provided on the inner wall of the discharge tube (1). ) has a convex strip (14) on the inner wall, and the output efficiency of the furnace is much higher than that of the inner wall having a uniform thickness around the entire circumference.

〔発明の効果〕〔Effect of the invention〕

以」二説明したように本発明によれば、放電管の外周面
に設けられた金属電極のエツジに対応する放電管の内壁
部分に管軸方向に沿う凸条を形成して、前記放電管内の
電界分布を均一・化しているので、金属電極のエツジ形
成部位における電界集中が回避され、しかも、放電管の
その他の部分の管壁は電力の注入を妨げない程度の厚さ
にすることができるので、レーザビーt、を高効率で取
り出すことができる。したがって、電力消費を節減でき
て経済性に富み、晶いレーザ加工性能を実現できるなど
の優れた効果を奏するに至った。
As explained below, according to the present invention, a convex strip along the tube axis direction is formed on the inner wall portion of the discharge tube corresponding to the edge of the metal electrode provided on the outer peripheral surface of the discharge tube, so that the inside of the discharge tube is Since the electric field distribution is made uniform, electric field concentration at the edge forming part of the metal electrode is avoided, and the wall thickness of other parts of the discharge tube can be made thick enough not to interfere with power injection. Therefore, the laser beam t can be extracted with high efficiency. Therefore, it has achieved excellent effects such as being able to reduce power consumption, being highly economical, and realizing crystalline laser processing performance.

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

第1図は本発明の一実施例を、1(す放電管の型部斜視
図、第2図はレーザ山内効率と放電管の内壁に設ける凸
条の有無との関係を示す棒線図、第3図は従来例の縦断
市面図、第4図は従来例の放電管の縦断側面図である。 (1)・・・放電管、(2)(3)・・・金属電極、(
2a)(3a)・・・金属電極のエツジ、 (14)・・・凸条。 第1 図 第3 第4 放電管内壁凸条の自無
Fig. 1 shows an embodiment of the present invention; Fig. 1 is a perspective view of a mold part of a discharge tube; Fig. 2 is a bar diagram showing the relationship between the laser mountain internal efficiency and the presence or absence of protrusions provided on the inner wall of the discharge tube; Fig. 3 is a longitudinal sectional view of a conventional example, and Fig. 4 is a longitudinal sectional side view of a conventional discharge tube. (1)...discharge tube, (2)(3)...metal electrode, (
2a) (3a)...Edge of metal electrode, (14)...Convex strip. Figure 1 Figure 3 Figure 4 The nature of the convex stripes on the inner wall of the discharge tube

Claims (1)

【特許請求の範囲】[Claims]  誘電体よりなる放電管内を光軸方向にレーザガスを流
し、前記放電管の外周面に管径方向で互いに対向して設
けられた金属電極間に高周波電圧を印加してこの放電管
内に放電を発生させ、この放電をレーザ励起源として前
記放電管の管軸方向にレーザビームを発生するガスレー
ザ発振装置において、前記金属電極のエッジに対応する
前記放電管の内壁部分に管軸方向に沿う凸条を形成した
ことを特徴とするガスレーザ発振装置。
A laser gas is caused to flow in the optical axis direction within a discharge tube made of a dielectric material, and a high-frequency voltage is applied between metal electrodes provided on the outer peripheral surface of the discharge tube facing each other in the tube diameter direction to generate a discharge within the discharge tube. In a gas laser oscillation device that generates a laser beam in the tube axis direction of the discharge tube using this discharge as a laser excitation source, a convex strip along the tube axis direction is provided on the inner wall portion of the discharge tube corresponding to the edge of the metal electrode. A gas laser oscillation device characterized in that:
JP19173288A 1988-07-30 1988-07-30 Gas laser oscillator Pending JPH0240974A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP19173288A JPH0240974A (en) 1988-07-30 1988-07-30 Gas laser oscillator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP19173288A JPH0240974A (en) 1988-07-30 1988-07-30 Gas laser oscillator

Publications (1)

Publication Number Publication Date
JPH0240974A true JPH0240974A (en) 1990-02-09

Family

ID=16279571

Family Applications (1)

Application Number Title Priority Date Filing Date
JP19173288A Pending JPH0240974A (en) 1988-07-30 1988-07-30 Gas laser oscillator

Country Status (1)

Country Link
JP (1) JPH0240974A (en)

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