JPH0240975A - Gas laser oscillator - Google Patents
Gas laser oscillatorInfo
- Publication number
- JPH0240975A JPH0240975A JP19173788A JP19173788A JPH0240975A JP H0240975 A JPH0240975 A JP H0240975A JP 19173788 A JP19173788 A JP 19173788A JP 19173788 A JP19173788 A JP 19173788A JP H0240975 A JPH0240975 A JP H0240975A
- Authority
- JP
- Japan
- Prior art keywords
- discharge tube
- carbon
- discharge
- laser beam
- 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
Links
- 229910052799 carbon Inorganic materials 0.000 claims abstract description 10
- OKTJSMMVPCPJKN-UHFFFAOYSA-N Carbon Chemical compound [C] OKTJSMMVPCPJKN-UHFFFAOYSA-N 0.000 claims abstract description 9
- 230000010355 oscillation Effects 0.000 claims abstract description 8
- 239000002184 metal Substances 0.000 claims description 7
- 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
- 230000000694 effects Effects 0.000 abstract description 3
- 238000000151 deposition Methods 0.000 abstract 2
- OKTJSMMVPCPJKN-NJFSPNSNSA-N Carbon-14 Chemical compound [14C] OKTJSMMVPCPJKN-NJFSPNSNSA-N 0.000 abstract 1
- 230000003247 decreasing effect Effects 0.000 abstract 1
- 230000008021 deposition Effects 0.000 abstract 1
- 238000002310 reflectometry Methods 0.000 abstract 1
- 239000011521 glass Substances 0.000 description 2
- 230000002093 peripheral effect Effects 0.000 description 2
- 241000406668 Loxodonta cyclotis Species 0.000 description 1
- 230000002411 adverse Effects 0.000 description 1
- 238000007664 blowing Methods 0.000 description 1
- 150000001721 carbon Chemical class 0.000 description 1
- 230000001055 chewing effect Effects 0.000 description 1
- 238000004891 communication Methods 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 238000003754 machining Methods 0.000 description 1
- 238000004519 manufacturing process Methods 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)
- Pigments, Carbon Blacks, Or Wood Stains (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、良質なレーザビームを発振
できるようにし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 coincide with each other, and particularly relates to a gas laser oscillation device that can oscillate a high-quality laser beam. It is related to the device.
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
る円筒吠の放電管(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
に対向杖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13.511iMHz、2
kv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
(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)(10)を両
管(1)(8)と連通伏態で配設して、放電管(’I)
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, the third
As shown in Fig. 4 and Fig. 4, a pair of metal electrodes (2) (3) are arranged at a predetermined interval on two places on both sides of the outer peripheral surface of a cylindrical discharge tube (1) made of a dielectric material such as glass. ) are disposed in close contact with the opposing canes, and the pair of metal electrodes (2) and (3) are connected to a high frequency AC power source (4),
For example, 13.511iMHz, 2
While applying a high frequency high voltage of kv, 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 these mirrors. (6) and partially reflective mirror (
7) constitutes an optical resonator, and an air pipe (8) is connected from the center between the electrodes (2) and (3) of the discharge tube (1).
A pair of branch pipes (9) and (10) are provided in communication with both pipes (1) and (8) between both ends of the discharge tube (1) and the other end of the air supply pipe (8). Arrange the discharge tube ('I)
A pair of circulation passages branching in two directions from the center of the
In history, a blower (11) is provided in the middle of the air pipe (8), and air pipes (8) are provided on both sides of the blower (11).
a discharge in the discharge space (5) and a blower (11);
A heat exchanger (
12) A so-called axial flow type gas laser oscillation device is known, which is provided with (13).
なお、前記送風機(11)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。Note that the blower (11) needs to have a blowing capacity capable of producing a gas flow at a flow rate of about 100 m/see in the discharge space (5).
上記構成の従来装置では、まず、一対の金属電極(2)
(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
)をレーザ加玉等の用途に供することになる。In the conventional device with the above configuration, first, a pair of metal electrodes (2)
When a high-frequency high voltage is applied to (3) from the high-frequency power source (4) to generate a glow-like discharge in the discharge space (5), the laser gas passing through the discharge space (5) obtains the discharge energy and is excited. At the same time, the optical resonator formed by the total reflection mirror (6) and the partial reflection mirror (7) enters a resonant state, whereby a laser beam (B) is output from the partial reflection mirror (7). This laser beam (B
) will be used for purposes such as laser beading.
ところで、上記従来構造のものでは、放電管(1)の内
壁面は例えばガラスの反射而となっている。By the way, in the conventional structure described above, the inner wall surface of the discharge tube (1) is made of, for example, a reflective glass.
しかしながら、このように放電管(+)の内壁面が反射
而となっているものでは、全反射鏡(6)と部分反射鏡
(7)の間に位置ずれが生じている場合、前記放電管(
+)の内壁面で全反射された定在波が増幅されて、その
一部が部分反射鏡(7)を通じて雑光として放出される
ため、この雑光がレーザビーム(B)に混入してレーザ
加工に悪影響を及ぼすという問題点があった。However, in such a case where the inner wall surface of the discharge tube (+) is reflective, if there is a positional shift between the total reflection mirror (6) and the partial reflection mirror (7), the discharge tube (
The standing wave that is totally reflected by the inner wall surface of the laser beam (+) is amplified and a part of it is emitted as noise light through the partially reflecting mirror (7), so this noise mixes into the laser beam (B). There was a problem that it adversely affected laser processing.
本発明は、こ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、放電管の内壁面の反射をなくすことによ
り、雑光が混入していない良質なレーザビームを発振で
きるがスレーザ発振装置の提供を[1的とするものであ
る。The present invention was made to solve these conventional problems, and by eliminating reflections on the inner wall surface of the discharge tube, it is possible to oscillate a high-quality laser beam without mixed light. The first purpose is to provide equipment.
一ヒ記目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
外周面に設けられた金属電極間に島内波電圧を印加して
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、前記放電管の内壁面にカ
ーボンを蒸着したことを特徴とするものである。In order to achieve the above object, the present invention causes a laser gas to flow in the optical axis direction in a discharge tube made of a dielectric material, and applies an island wave voltage between metal electrodes provided on the outer peripheral surface of the discharge tube. A gas laser oscillation device that generates a discharge in a discharge tube and uses the discharge as a laser excitation source to generate a laser beam in the axial direction of the discharge tube, characterized in that carbon is deposited on the inner wall surface of the discharge tube. be.
本発明は上記構成により、全反射鏡と部分反射鏡とが位
置ずれしているような場合であっても、前記放電管の内
壁面は蒸着されたカーボンにより反射率が極めて低(な
っているので、雑光の発生が大幅に抑制され、レーザビ
ームには雑光が殆ど混入せず、したがって、良質なレー
ザビームを得ることができるものである。With the above configuration, the present invention has an extremely low reflectance on the inner wall surface of the discharge tube due to vapor-deposited carbon even when the total reflection mirror and the partial reflection mirror are misaligned. Therefore, the generation of noise light is greatly suppressed, and the laser beam is hardly mixed with noise light, so that a high quality laser beam can be obtained.
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、重複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 the same configuration and function will be given the same reference numerals, and their explanation will be omitted to avoid duplication. 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、円筒状の放電管(1)の内壁面に数μ(ミ
クロン)程度のカーボン(I4)が蒸着されている。こ
のカーボン蒸着膜(I4)により放電管(+)内壁面の
反射率が極端に低下し、定在波は殆ど反射しないので、
雑光の発生が著しく少なくなる。したがって、部分反射
鏡(7)から放出されるレーザビーム(B)は雑光が殆
ど混入していない良質なものとなり、例えば切断加工に
おいて、加工面の仕上げ精度を向上させることができる
ものである。In FIG. 1, in the gas laser oscillation device according to this embodiment, carbon (I4) of several μ (microns) is deposited on the inner wall surface of a cylindrical discharge tube (1). This carbon deposited film (I4) extremely reduces the reflectance of the inner wall surface of the discharge tube (+), and standing waves are hardly reflected.
The generation of stray light is significantly reduced. Therefore, the laser beam (B) emitted from the partially reflecting mirror (7) is of high quality with almost no stray light mixed in, and can improve the finishing accuracy of the machined surface during cutting, for example. .
第2図に従来例と本発明との切断加工面の而粗さの相違
を示しており、この結果から明らかなように、本発明装
置では放電管(・I)の内壁面にカーボン蒸着膜(I4
)を設けたものでは切断加工面の仕上げ精度が格段に向
上するものである。Fig. 2 shows the difference in the roughness of the cut surface between the conventional example and the present invention, and as is clear from this result, in the device of the present invention, there is a carbon vapor deposited film on the inner wall surface of the discharge tube (I). (I4
), the finishing accuracy of the cut surface is significantly improved.
以」二説明したように本発明によれば、放電管の内壁面
にカーボンを蒸着して、前記内壁面の反射率を大幅に低
ドさせているので、雑光のない良質なレーザビームを得
ることができ、切断加工等のレーザ加工の仕」こげ精度
を向上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, carbon is deposited on the inner wall surface of the discharge tube to significantly lower the reflectance of the inner wall surface, so that a high-quality laser beam without any stray light can be produced. This has resulted in excellent effects such as improving the accuracy of laser machining such as cutting.
第1図は本発明の一実施例を示す放電管の縦断面図、第
2図は従来例と本発明との切断加工面の而粗さの相違を
示す棒線図、第3図は従来例の縦断正面図、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、
(+4)・・・カーボン。
逆へ
仁′デ噛
象31
ミ(々
−のり
ご
J
第3
2(3〕Fig. 1 is a longitudinal cross-sectional view of a discharge tube showing an embodiment of the present invention, Fig. 2 is a bar diagram showing the difference in roughness of cut surfaces between the conventional example and the present invention, and Fig. 3 is a conventional example. FIG. 4 is a longitudinal sectional front view of the example, and FIG. 4 is a longitudinal sectional side view of a conventional discharge tube. (1)...discharge tube, (2)(3)...metal electrode,
(+4)...Carbon. Gyakuhen'de chewing elephant 31 Mi (Norigo J No. 3 2 (3)
Claims (1)
し、前記放電管の外周面に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、前記放
電管の内壁面にカーボンを蒸着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 circumferential surface of the discharge tube to generate a discharge within the discharge tube, and this discharge is used as a laser excitation source. A gas laser oscillation device that generates a laser beam in the axial direction of the discharge tube, characterized in that carbon is deposited on an inner wall surface of the discharge tube.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP19173788A JPH0240975A (en) | 1988-07-30 | 1988-07-30 | Gas laser oscillator |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP19173788A JPH0240975A (en) | 1988-07-30 | 1988-07-30 | Gas laser oscillator |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH0240975A true JPH0240975A (en) | 1990-02-09 |
Family
ID=16279661
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP19173788A Pending JPH0240975A (en) | 1988-07-30 | 1988-07-30 | Gas laser oscillator |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0240975A (en) |
-
1988
- 1988-07-30 JP JP19173788A patent/JPH0240975A/en active Pending
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