JPH0240979A - Gas laser oscillator - Google Patents
Gas laser oscillatorInfo
- Publication number
- JPH0240979A JPH0240979A JP19173888A JP19173888A JPH0240979A JP H0240979 A JPH0240979 A JP H0240979A JP 19173888 A JP19173888 A JP 19173888A JP 19173888 A JP19173888 A JP 19173888A JP H0240979 A JPH0240979 A JP H0240979A
- Authority
- JP
- Japan
- Prior art keywords
- discharge tube
- discharge
- coil
- insulators
- tube
- 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
Links
- 239000012212 insulator Substances 0.000 claims abstract description 19
- 238000004804 winding Methods 0.000 claims abstract 2
- 239000002184 metal Substances 0.000 claims description 34
- 230000010355 oscillation Effects 0.000 claims description 11
- 230000002093 peripheral effect Effects 0.000 claims description 6
- 230000003287 optical effect Effects 0.000 claims description 5
- 239000003989 dielectric material Substances 0.000 claims description 3
- 230000005284 excitation Effects 0.000 claims description 2
- 230000020169 heat generation Effects 0.000 abstract description 5
- 238000003754 machining Methods 0.000 abstract 1
- 239000000853 adhesive Substances 0.000 description 2
- 230000001070 adhesive effect Effects 0.000 description 2
- 238000007664 blowing Methods 0.000 description 1
- 238000004891 communication Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES 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
- H01S3/00—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
- H01S3/09—Processes or apparatus for excitation, e.g. pumping
- H01S3/097—Processes or apparatus for excitation, e.g. pumping by gas discharge of a gas laser
- H01S3/0975—Processes 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
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は、放電管の軸力向と光軸方向が−・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] [Field of Industrial Application] The present invention relates to a gas laser oscillation device in which the axial force direction of a discharge tube and the optical axis direction match, and in particular, the present invention relates to a gas laser oscillation device that achieves high efficiency of laser oscillation. This invention relates to a gas laser oscillation device.
従来、この種のガスレーザ発振装置としては例えば第2
図および第3図に示すように、ガラス等の誘電体よりな
る円筒杖の放電管(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)を互い
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13.56Ml1z、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m内の放電空間(5ンの両端に
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(1)
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)の他端間に一対の分岐管(9)(to)を両管(1
)(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(ll)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
より昇温したレーザガスを冷却する熱交換器(12)(
13)を配設してなる、いわゆる軸流型のガスレーザ発
振装置が知られている。Conventionally, as this type of gas laser oscillation device, for example, a second
As shown in Fig. 3 and Fig. 3, a pair of metal electrodes (2) (3) are placed at a predetermined interval on two positions on both sides of the tube axis on the outer peripheral surface of a cylindrical discharge tube (1) made of a dielectric material such as glass. ) are arranged in close contact with each other in a state facing each other, and the pair of metal electrodes (2) and (3) are connected to a high frequency AC power source (4),
For example, 13.56Ml1z, 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 m sandwiched between them, and these total reflection mirrors (6) and a partially reflecting mirror (7) constitute an optical resonator, and the discharge tube (1)
An air pipe (8) is provided in communication with the center between both electrodes (2) and (3) of the discharge tube (1), and both ends of the discharge tube (1) and the air pipe (
Connect a pair of branch pipes (9) (to) between the other ends of both pipes (1
) (8) to form a pair of circulation passages branching in two directions from the center of the discharge tube (1). ), and a heat exchanger is provided in the air pipe (8) on both sides of the blower (ll) to cool down the laser gas that has been heated due to discharge in the discharge space (5) and driving of the blower (11). (12)(
A so-called axial flow type gas laser oscillation device is known, in which a so-called axial flow type gas laser oscillation device is provided.
なお、前記送風機(H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7認があ
る。In addition, as the blower (H), it is recommended to use a blower having a blowing ability capable of obtaining a gas flow having a flow velocity of about 100 m/see in the discharge space (5).
」−記構成の従来装置では、まず、一対の金属電極(2
)(3)に島内被電1(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電エネ
ルギーを得て励起されると共に、全反射鏡(6)および
部分反射鏡(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
)をレーザ加工等の用途に供することになる。In the conventional device having the configuration described above, first, a pair of metal electrodes (2
)(3) is applied with a high frequency and high voltage from the island's electrified device 1 (4) to generate a glow-like discharge in the discharge space (5), the laser gas passing through this discharge space (5) absorbs the discharge energy. At the same time, the optical resonator formed by the total reflection mirror (6) and the partial reflection mirror (7) becomes resonant, and the laser beam (B) is output from the partial reflection mirror (7). This laser beam (B
) will be used for purposes such as laser processing.
ところで1.1−記のように金属電極(2)(3)間に
高周波高電圧を印加してレーザビーム(B)を得る場合
、両金属電極(2)(3)間のインピーダンスによって
放電管内の放電状態が支配されることになり、このイン
ピーダンスを一定化するため、従来では例えば金属電極
(2)(3)を放電管(+)の外周面上に接着剤(14
)等を用いて固着し、また、高周波電源(4)と金属電
極(2)(3)間のインピーダンス整合をとるために両
者間に共振回路(I5)を介装するようにしていた。By the way, when obtaining a laser beam (B) by applying a high frequency and high voltage between the metal electrodes (2) and (3) as described in 1.1-, the impedance between the metal electrodes (2 and 3) causes damage inside the discharge tube. In order to keep this impedance constant, for example, metal electrodes (2) and (3) were placed on the outer peripheral surface of the discharge tube (+) with an adhesive (14).
) etc., and in order to achieve impedance matching between the high frequency power source (4) and the metal electrodes (2) and (3), a resonant circuit (I5) was interposed between them.
しかしながら、上記従来構造のガスレーザ発振装置によ
ると放電管(1)の発熱等によって接着剤(14)が劣
化するため、金属電極(2)(3)間のインピーダンス
が変化する上、共振回路(15)と金属電極(2)(3
)間の接続配線から浮遊容量が発生して整合条件にばら
つきが生じることになるため、放電が不安定となり、レ
ーザビームを効率よ(取出すことができないという問題
点があった。However, in the gas laser oscillator having the conventional structure described above, the adhesive (14) deteriorates due to heat generation of the discharge tube (1), so the impedance between the metal electrodes (2) and (3) changes, and the resonant circuit (15 ) and metal electrodes (2) (3
Stray capacitance is generated from the connecting wires between the two, causing variations in matching conditions, making the discharge unstable and causing the problem that the laser beam cannot be extracted efficiently.
本発明は、1−記のような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の
安定性を確保して、装置の信頼性の向−ヒを図ることを
目的とするものである。The present invention has been made in order to solve the conventional problems as described in 1., and aims to improve the reliability of the device by ensuring the stability of the discharge in the discharge space within the discharge tube. The purpose is to
」1記に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
方向にレーザビートを発生するガスレーザ発振装置にお
いて、前記金属電極を前記放電管との間に挟み込む2枚
一組の半円筒状絶縁物を配設し、この半円筒状絶縁物の
外周にコイルを巻付けてこのコイルにより前記)1′円
筒状絶縁物を放電管の外周面Eに固定すると共に、前記
コイルをインピーダンス整合をとるための共振回路素子
として前記金属電極間に接続してなることを特徴とする
ものである。In order to achieve the above object in item 1, the present invention allows a laser gas to flow in the optical axis direction inside a discharge tube made of a dielectric material, and metal electrodes are provided on the outer circumferential surface of the discharge tube to face each other in the tube diameter direction. In a gas laser oscillator device that generates a discharge in the discharge tube by applying a high frequency voltage between the two, and uses this discharge as a laser excitation source to generate a laser beat in the tube axis direction of the discharge tube, the metal electrode is connected to the discharge tube. A set of two semi-cylindrical insulators is placed between them, and a coil is wound around the outer periphery of the semi-cylindrical insulators. E, and the coil is connected between the metal electrodes as a resonant circuit element for impedance matching.
本発明は!−記構成により、金属電極間のインピーダン
ス整合をとるための共振回路素子をコイルにより構成し
、このコイルで半円筒状絶縁物の固定丁9段を兼用させ
ているので、構造が簡略化され、しかも、共振回路素子
を別に設けなくてもよく、これにより共振回路と金属電
極間の接続配線は僅かの長さで済むことになる。したが
って、接続配線による浮遊容量の発生を極力抑制できる
ので、金属電極間のインピーダンスを安定化でき、また
、金属電極と高周波電源間のインピーダンス整合のばら
つきが抑制されるので、放電の安定性を確保することが
できる。This invention! - According to the configuration described above, the resonant circuit element for impedance matching between metal electrodes is constituted by a coil, and this coil also serves as the nine stages of fixed plates of semi-cylindrical insulators, so the structure is simplified. Moreover, there is no need to separately provide a resonant circuit element, and as a result, the length of the connection wiring between the resonant circuit and the metal electrode can be reduced. Therefore, the generation of stray capacitance due to connection wiring can be suppressed as much as possible, making it possible to stabilize the impedance between the metal electrodes.Also, variations in impedance matching between the metal electrode and the high-frequency power source are suppressed, ensuring stability of discharge. can do.
更に、金属電極はコイルによって絶縁物を介して放電管
の外周に常時圧着状態に保持されているので、放電管の
発熱による剥離を防止することができる。Furthermore, since the metal electrode is always held in a compressed state on the outer periphery of the discharge tube by the coil via the insulator, it is possible to prevent the metal electrode from peeling off due to heat generation of the discharge tube.
以ド、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、構成並びに作用が共通する部分は共
通の符号を付すこととし、小腹を避けるためにその説明
を省略するものとする。This embodiment device has the same basic configuration as the conventional example described above, so parts with common configurations and functions will be given the same reference numerals, and their explanation will be omitted to avoid misunderstandings. do.
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、放電管(1)の外周に、この放電管(1)
との間で金属電極(2)(3)を挟み込む2枚−・紐の
半円筒状絶縁物(]B)を配設してあり、更に、この絶
縁物(16)の外周にコイル(17)を巻付けて、この
コイル(I7)により同絶縁物(1B)を放電管(1)
の外周面上に固定した構造としている。In FIG. 1, in the gas laser oscillation device according to this embodiment, the discharge tube (1) is attached to the outer periphery of the discharge tube (1).
A semi-cylindrical insulator (]B) made of two pieces of string is arranged between which the metal electrodes (2) and (3) are sandwiched, and a coil (17 ), and this coil (I7) connects the same insulator (1B) to the discharge tube (1).
The structure is such that it is fixed on the outer peripheral surface of the
また、前記コイル(17)は金属電極(2)(3)と高
岡7t[源(4)間のインピーダンス整合をとるための
共振回路素子として作用するものであり、前記高周波電
源(4)の両端に短い配線を介して接続されている。こ
のようにコイル(17)で」(振回路素子を兼用させる
ことで、共振回路と高周波電源(4)間等の配線を大幅
に削減でき、また、金属電極(2)(3)はコイル(1
7)によって絶縁物(1B)を介して放電管(1)の外
j11に常時圧着状態に保持されているので、放電管(
+)の発熱による剥離を防11することができる。Further, the coil (17) acts as a resonant circuit element for impedance matching between the metal electrodes (2) (3) and the Takaoka 7t [source (4), and is connected to both ends of the high frequency power source (4). connected via a short wire. By making the coil (17) double as the resonant circuit element in this way, the wiring between the resonant circuit and the high-frequency power source (4) can be significantly reduced, and the metal electrodes (2) and (3) 1
7), the discharge tube (
+) peeling due to heat generation can be prevented.
以上説明したように本発明によれば、金属電極を前記放
電管との間に挟み込む2枚一組の半円t5状絶縁物を配
設し、この半円筒状絶縁物を外周に巻付けたコイルによ
り放電管の外周面上に固定すると共に、前記コイルをイ
ンピーダンス整合をとるための共振回路素子として前記
金属電極間に接続してなるものとしたので、金属電極間
のインピーダンス整合をとるための共振回路素子をコイ
ルにより構成し、このコイルで半円筒状絶縁物の固定手
段を兼用させて金属電極と共振回路とを一体化している
ので、共振回路素子を別に設けなくてもよ(、構造を簡
略化することができる。As explained above, according to the present invention, a set of two semicircular T5-shaped insulators are provided to sandwich the metal electrode between the discharge tube, and this semi-cylindrical insulator is wrapped around the outer periphery. The coil is fixed on the outer peripheral surface of the discharge tube by a coil, and the coil is connected between the metal electrodes as a resonant circuit element for impedance matching. The resonant circuit element is constituted by a coil, and this coil also serves as a fixing means for the semi-cylindrical insulator to integrate the metal electrode and the resonant circuit, so there is no need to provide a separate resonant circuit element. can be simplified.
また、これにより共振回路と金属電極間の接続配線は僅
かの長さで済むことになるため、接続配線による浮遊容
はの発生を極力抑制できる。したがって、金属電極間の
インピーダンスを安定化でき、また、金属電極と高周波
電源間のインピーダンス整合のばらつきが抑制されるの
で、放電の安定性を確保することができる。Further, since this allows the connection wiring between the resonant circuit and the metal electrode to be of a short length, the generation of stray capacitance due to the connection wiring can be suppressed as much as possible. Therefore, the impedance between the metal electrodes can be stabilized, and variations in impedance matching between the metal electrodes and the high-frequency power source can be suppressed, so that stability of discharge can be ensured.
史に、金属電極はフィルによって絶縁物を介して放電管
の外周に常時圧着状態に保持されているので、放電管の
発熱による剥離を防止することができる。Historically, the metal electrode has always been held in a compressed state on the outer periphery of the discharge tube via an insulator by a fill, so that it is possible to prevent the metal electrode from peeling off due to heat generation of the discharge tube.
このように本発明によれば、比較的簡単に構成し得るも
のでありながら、信頼性か高く、優れたレーザ加に性能
を発揮するガスレーザ発振装置を提供できるに至った。As described above, according to the present invention, it has been possible to provide a gas laser oscillation device that can be constructed relatively easily, has high reliability, and exhibits excellent laser performance.
第1図は本発明の一実施例を示す放電管の斜視図、第2
図は従来例の縦断正面図、第3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、(
l[i)・・・半円筒状絶縁物、(17)・・・コイル
。
確
第1図
1f:コイルFIG. 1 is a perspective view of a discharge tube showing one embodiment of the present invention, and FIG.
The figure is a longitudinal sectional front view of a conventional example, and FIG. 3 is a longitudinal sectional side view of a conventional discharge tube. (1)...discharge tube, (2)(3)...metal electrode, (
l[i)...Semi-cylindrical insulator, (17)...Coil. Figure 1 1f: Coil
Claims (1)
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、前記金属電極を前記放電管との間
に挟み込む2枚一組の半円筒状絶縁物を配設し、この半
円筒状絶縁物の外周にコイルを巻付けてこのコイルによ
り前記半円筒状絶縁物を放電管の外周面上に固定すると
共に、前記コイルをインピーダンス整合をとるための共
振回路素子として前記金属電極間に接続してなるガスレ
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 set of two semi-cylindrical insulators sandwiching the metal electrode and the discharge tube is provided. a resonant circuit for winding a coil around the outer periphery of the semi-cylindrical insulator to fix the semi-cylindrical insulator on the outer peripheral surface of the discharge tube and for impedance matching the coil; A gas laser oscillation device which is connected between the metal electrodes as an element.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP19173888A JPH0240979A (en) | 1988-07-30 | 1988-07-30 | Gas laser oscillator |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP19173888A JPH0240979A (en) | 1988-07-30 | 1988-07-30 | Gas laser oscillator |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH0240979A true JPH0240979A (en) | 1990-02-09 |
Family
ID=16279678
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP19173888A Pending JPH0240979A (en) | 1988-07-30 | 1988-07-30 | Gas laser oscillator |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0240979A (en) |
-
1988
- 1988-07-30 JP JP19173888A patent/JPH0240979A/en active Pending
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