JPS5821892A - Noiseless discharge carbon dioxide gas laser - Google Patents
Noiseless discharge carbon dioxide gas laserInfo
- Publication number
- JPS5821892A JPS5821892A JP12071981A JP12071981A JPS5821892A JP S5821892 A JPS5821892 A JP S5821892A JP 12071981 A JP12071981 A JP 12071981A JP 12071981 A JP12071981 A JP 12071981A JP S5821892 A JPS5821892 A JP S5821892A
- Authority
- JP
- Japan
- Prior art keywords
- pair
- dielectric
- electrodes
- carbon dioxide
- dielectric electrodes
- 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.)
- Granted
Links
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
-
- 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
- H01S3/02—Constructional details
- H01S3/03—Constructional details of gas laser discharge tubes
- H01S3/038—Electrodes, e.g. special shape, configuration or composition
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】
この発明は大出力の無声放電式炭酸ガスレーザ装置、と
くに不安定共振器形の炭酸ガスレーザ装置に関するもの
である。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a high-output silent discharge type carbon dioxide laser device, particularly to an unstable resonator type carbon dioxide laser device.
従来、この種の装置として第1図に示すものがあった。Conventionally, there has been a device of this type as shown in FIG.
図において、(1)は一対の誘電体電極であり。In the figure, (1) is a pair of dielectric electrodes.
夫々金属電極(11a) (11b)がガラス等の誘電
体m−、(51は凹面ミラー(4)に対向する凸面ミラ
ーからなる部分反射鏡であり、凹面ミラー(4)ととも
に不安定共振器を構成している。(6)は出力ビームで
ある。また、一対の誘電体膜′!1iL(11及び不安
定共振器は密閉容器内に収納されている。(7)は一対
の誘電体電極(1)間の放電空間で、aO2−00−N
2− Ho 等からなる混合気体のレーザガスが高速
で流されている。The metal electrodes (11a) and (11b) are made of dielectric material such as glass, respectively, and (51 is a partially reflecting mirror consisting of a convex mirror facing the concave mirror (4), which together with the concave mirror (4) forms an unstable resonator. (6) is the output beam. Also, a pair of dielectric films'!1iL (11 and the unstable resonator are housed in a sealed container. (7) is a pair of dielectric electrodes. (1) In the discharge space between aO2-00-N
A laser gas mixture consisting of 2-Ho and the like is flowing at high speed.
次に、このように構成された従来装置の動作について説
明する。先ず、一対の誘電体電極(+1に高周波電源(
3)から約10 kV 、 100 kHz程度の
圧を加える。これにともない放電空間(7)に無声放電
が生じ、レーザガスが励起されミラー+4) +51に
より構成される不安定共振器で発振が起リ、内部発振ビ
ーム(2)が形成され、一部が出力ビーム(6)として
外部にとり出されることになる。Next, the operation of the conventional device configured as described above will be explained. First, a pair of dielectric electrodes (+1 is connected to a high frequency power source (
3) to about 10 kV, 100 kHz
Apply pressure. As a result, a silent discharge occurs in the discharge space (7), the laser gas is excited, and oscillation occurs in the unstable resonator formed by the mirror +4) +51, forming an internal oscillation beam (2), with a part of it being output. It will be taken out as a beam (6).
このようにして取り出された出力ビーム(6)をレーザ
ビームとして溶断、溶接等の種々の用途に用いることに
なる。The output beam (6) extracted in this way is used as a laser beam for various purposes such as fusing and welding.
ところで、従来の装置は以上のように構成されているの
で、ミラー(51、(4)の対向配設位置関係が少しず
れると、内部発振ビーム(2)が誘電体電極(1)を構
成するガラス(12a)または(12b)に当ることに
なり、そのためガラス(12a)または(t2b)が損
傷を受けてしまうという欠点があった。またこの欠点を
なくすために、ミラー(4)。By the way, since the conventional device is configured as described above, if the opposing arrangement positions of the mirrors (51, (4) are slightly shifted), the internal oscillation beam (2) will form the dielectric electrode (1). There was a drawback that the glass (12a) or (t2b) would be hit by the glass (12a) or (12b), and therefore the glass (12a) or (t2b) would be damaged.Also, in order to eliminate this drawback, the mirror (4).
(5)の位置関係を調整することは非常に難しく。It is very difficult to adjust the positional relationship in (5).
にガラス面保護用の防壁を設けたものであり。A barrier is installed to protect the glass surface.
電極の信頼性の高い無声放電式炭酸ガスレーザ装置を提
供することを目的とする。The purpose of the present invention is to provide a silent discharge type carbon dioxide laser device with highly reliable electrodes.
以下、この拠明の一実施例を図について説明する。An embodiment of this principle will be described below with reference to the drawings.
第2図はこの発明の一実施例装置を示すものであり1図
中QDはセラミクス板で、一対の誘電体電極(1)のガ
ラス面(12a) (121))から放電空間(7)側
に約3m突出させたものであり、この実施例では凹面ミ
ラー(4)側及び中央部のガラス面(12a) (12
b)に配設している。なお9図中第1図と同一または相
当部分には同一符号を付しその説明を省略している。Figure 2 shows an apparatus according to an embodiment of the present invention. In Figure 1, QD is a ceramic plate, which is connected to the discharge space (7) from the glass surface (12a) (121)) of the pair of dielectric electrodes (1). In this example, the concave mirror (4) side and the central glass surface (12a) (12
b). In FIG. 9, the same or corresponding parts as in FIG. 1 are given the same reference numerals, and their explanations are omitted.
このようにセラミクス板Qυを要所lこ適宜配設してい
るので、ミラー(4) (5)の角度位置設定不良時に
とのレーザ装置を作動させても、内部発振ビーム(2)
がセラミクス板6111により偏向されることになるた
め、ガラス面(12a) (12b)がビーム(2)に
よって直撃され損傷を受けることが回避できることにな
る。さらにセラミクス板e2Dはビームにより加熱され
てもレーザ発振に影響を与え好なレーザ出力ビーム(6
)を得られることになる。Since the ceramic plates Qυ are appropriately arranged at important points in this way, even if the laser device is activated when the angular position of the mirrors (4) and (5) is incorrect, the internal oscillation beam (2)
Since the beam is deflected by the ceramic plate 6111, the glass surfaces (12a) (12b) can be avoided from being directly hit and damaged by the beam (2). Furthermore, even if the ceramic plate e2D is heated by the beam, it will affect the laser oscillation and will not be able to maintain a favorable laser output beam (6
) will be obtained.
なお、上記実施例ではセラミクス板を防壁として用いた
が、この発明ではこれに限られず。In addition, although the ceramic board was used as a barrier in the said Example, this invention is not limited to this.
(12b)から放電空間(7)に突出するように配設す
ればよい。What is necessary is just to arrange|position so that it may protrude from (12b) into discharge space (7).
以上のように、この発明装置は一対の誘電体電極の誘電
体膜から放電空間側lこ突出するように無機絶縁物を適
宜配設したものであり、内部共振ビームが誘電体膜を直
撃しないように無機絶縁物の突出部により偏向している
ので、誘電体膜の損傷を防止することができ、信頼性の
高い大出力の無声放電式炭酸ガスレーザ装置とすること
ができるとい、う効果がある。As described above, in the device of this invention, an inorganic insulator is appropriately arranged so as to protrude from the dielectric film of the pair of dielectric electrodes toward the discharge space, so that the internal resonant beam does not directly hit the dielectric film. Since the beam is deflected by the protruding part of the inorganic insulator, damage to the dielectric film can be prevented, and a highly reliable high-output silent discharge type carbon dioxide laser device can be achieved. be.
第1図は従来の無声放電式炭酸ガスレーザ装置の原理構
成図、第2図はこの発明の一実施例の構成を示す図であ
る。
(1)・・・誘電体電極、 (12a) (12b)・
・・誘電体膜。
(2)・・・内部発振ビーム、(3)・−・高周波電源
、(4)・・・凹面ミラー、(5)・・・凸面ミラー、
Qト・・セラミクス板。
な詔2図中、同−符号は同−又は相当部分を示す。
?)許出願人 丁乳技術院長
石板誠−FIG. 1 is a diagram showing the basic configuration of a conventional silent discharge type carbon dioxide laser device, and FIG. 2 is a diagram showing the configuration of an embodiment of the present invention. (1)...Dielectric electrode, (12a) (12b)
...Dielectric film. (2)...Internal oscillation beam, (3)...High frequency power supply, (4)...Concave mirror, (5)...Convex mirror,
Q...Ceramics board. The same reference numerals in the figures indicate the same or equivalent parts. ? ) Applicant: Makoto Ishiban, Director of Dingyu Technology Institute
Claims (1)
電体電極、上記一対の誘電体電極に接続された高周波電
源、上記一対の誘電体JK極間の放電空間に流されるレ
ーザガス、上記一対予誘電体電極間の放電空間を介して
対向する全゛反射鏡と部分反射鏡とからなる不安定共振
器。 注記一対の誘電体電極及び不安定共振器を密閉、I °′収納する密閉容器、上記一対の誘電体電極の誘電体
膜から放電空間側に突出するように適宜配設された無機
絶縁物を備えてなる無声放電式炭酸ガスレーザ装置。[Scope of Claims] A pair of dielectric electrodes covered with a dielectric film and facing each other with a predetermined gap therebetween, a high frequency power source connected to the pair of dielectric electrodes, and a discharge space between the pair of dielectric JK electrodes. An unstable resonator consisting of a total reflection mirror and a partial reflection mirror that face each other through a discharge space between the flowing laser gas and the pair of pre-dielectric electrodes. Note: An airtight container in which the pair of dielectric electrodes and the unstable resonator are hermetically housed, and an inorganic insulator appropriately arranged so as to protrude from the dielectric film of the pair of dielectric electrodes to the discharge space side. A silent discharge type carbon dioxide laser device.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP12071981A JPS5840354B2 (en) | 1981-08-03 | 1981-08-03 | Silent discharge type carbon dioxide laser device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP12071981A JPS5840354B2 (en) | 1981-08-03 | 1981-08-03 | Silent discharge type carbon dioxide laser device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5821892A true JPS5821892A (en) | 1983-02-08 |
| JPS5840354B2 JPS5840354B2 (en) | 1983-09-05 |
Family
ID=14793300
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP12071981A Expired JPS5840354B2 (en) | 1981-08-03 | 1981-08-03 | Silent discharge type carbon dioxide laser device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5840354B2 (en) |
-
1981
- 1981-08-03 JP JP12071981A patent/JPS5840354B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5840354B2 (en) | 1983-09-05 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| JPS5821892A (en) | Noiseless discharge carbon dioxide gas laser | |
| US3568088A (en) | Laser with improved power and frequency stability | |
| JPS603170A (en) | Silent discharge type gas laser device | |
| JPH03185885A (en) | Pulsed gas laser | |
| JP2700345B2 (en) | Gas laser device | |
| JPH0371683A (en) | Gas laser device | |
| JPH0234196B2 (en) | GASUREEZASOCHI | |
| JP2640345B2 (en) | Gas laser oscillation device | |
| JPH08506934A (en) | Ring laser discharge start concept | |
| JPS622678A (en) | Gas laser oscillator | |
| JPS63202982A (en) | Laser oscillating equipment | |
| JPS63227082A (en) | Gas laser oscillator | |
| US6567456B1 (en) | Method and apparatus for achieving polarization in a laser using a dual-mirror mirror mount | |
| JPH0635485Y2 (en) | High gas pressure laser oscillator | |
| JPH03178179A (en) | Gas laser oscillation equipment | |
| JPH0225267B2 (en) | ||
| JP3265644B2 (en) | Semiconductor laser pumped solid-state laser device | |
| JPH06101600B2 (en) | Transversely excited gas laser oscillator | |
| JPS62202579A (en) | Gas laser oscillator | |
| JPS5855656Y2 (en) | gas laser tube | |
| JPH03292781A (en) | Gas laser oscillation device | |
| JPH0384976A (en) | Excimer laser device | |
| JPS5878479A (en) | Optical adjusting mechanism for gas laser tube | |
| JPH01194481A (en) | Gas laser oscillating apparatus | |
| JPS5861688A (en) | Mirror sealing method of gas laser tube |