JPS6358885A - Silent discharge type gas laser device - Google Patents

Silent discharge type gas laser device

Info

Publication number
JPS6358885A
JPS6358885A JP20308686A JP20308686A JPS6358885A JP S6358885 A JPS6358885 A JP S6358885A JP 20308686 A JP20308686 A JP 20308686A JP 20308686 A JP20308686 A JP 20308686A JP S6358885 A JPS6358885 A JP S6358885A
Authority
JP
Japan
Prior art keywords
dielectric
electrodes
frequency
phase
high voltage
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
JP20308686A
Other languages
Japanese (ja)
Inventor
Tsukasa Fukushima
司 福島
Kenji Kumamoto
健二 熊本
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP20308686A priority Critical patent/JPS6358885A/en
Publication of JPS6358885A publication Critical patent/JPS6358885A/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

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

Abstract

PURPOSE:To prevent the abnormal discharge, the deterioration of a filling mixed gas as well as the damage to electrodes and improve the efficiency and reliability by preparing a synchronous measure for a frequency and phase of a reference oscillator and the like which causes the frequency and phase of an alternating high voltage applied to a pair of dielectric electrodes to coincide with one another among plural pairs of them. CONSTITUTION:A synchronous measure 13 of a frequency and phase having a reference oscillator 13a is prepared so as to cause the frequency and phase of alternating high voltage power sources 7a and 7b applied to dielectric electrodes 1a and 1b as well as the dielectric electrodes 4a and 4b to coincide with one another among plural of them. As a result, the upper part dielectric electrodes 1a and 4a that are adjacent each other or the lower part dielectric electrodes 1b and 4b come to the same electrical potential. Thus, the abnormal discharge among these electrodes is prevented and laser beams 12 are free from output decrease and electrode damage because of the deterioration of a mixed gas to be filled in a vacuum vessel 2 and then, more efficient and more reliable silent discharge type gas laser device is obtained.

Description

【発明の詳細な説明】 [産業上の利用分野] この発明は、無声放電式ガスレーザ装置に関する。[Detailed description of the invention] [Industrial application field] The present invention relates to a silent discharge type gas laser device.

[従来の技術] 第3図に従来の無声放電式ガスレーザ装芒の構成を示す
[Prior Art] FIG. 3 shows the configuration of a conventional silent discharge type gas laser awn.

図において、(la) 、 (lb)は真空容器(2)
内に、対向配置された第1誘電体電極であって、金属電
極(2a)、 (2b)の表面に誘電体(3a) 、 
(3b)が被覆されている。 (4a) 、 (4b)
は同じく真空容器2内に対向配置された第2誘電体電極
であって前記第1誘電体電極(la) 、 (lb)と
同様に金属電極(5a)、 (5b)の表面に誘電体(
6a)、 (6b)が被覆されている。上記の第1誘電
体電極(la) 、 (ib)と第2 、?J ’+h
休゛体極(4a) 、 (H))とを2分割構成とする
のは、レーザビームの出力の増大化を計るために誘′i
セ体電極の長さを長くすると、必然的に誘電体電極にた
わみが生じるおそれがあり、また長大の誘電体重・極で
あると、その表面に均一な膜厚の誘電体を形成し難く、
膜厚の薄い部分に電流集中が生じ絶縁破壊の原因となる
からである。
In the figure, (la) and (lb) are vacuum containers (2)
a first dielectric electrode disposed oppositely within the metal electrode (2a), (2b) having a dielectric (3a) on the surface thereof;
(3b) is coated. (4a), (4b)
is a second dielectric electrode which is also placed opposite to each other in the vacuum vessel 2, and similarly to the first dielectric electrodes (la) and (lb), the metal electrodes (5a) and (5b) have a dielectric (
6a) and (6b) are coated. The first dielectric electrode (la), (ib) and the second dielectric electrode, ? J'+h
The reason why the rest body poles (4a) and (H)) are divided into two is to increase the output of the laser beam.
If the length of the cell electrode is increased, there is a risk that the dielectric electrode will inevitably bend, and if the dielectric weight/pole is long, it will be difficult to form a dielectric with a uniform thickness on the surface.
This is because current concentration occurs in the thin portion of the film, causing dielectric breakdown.

(7a) 、 (7b)は上記第1誘電体電極(la)
 、 (lb)および第2誘゛心体電極(4a) 、 
(4b)に各々独立して接続された交流高電圧電源であ
る。(8)はト記第1?A電体電極(la) 、 (l
b)および第2誘電体電梯(4a) 、 (4b)間で
生じる無声放′屯、Ho)、  (11)はレーザ光の
光軸上に配置した全反射鏡および部分反射鏡である。 
(12)は部分反射鏡(!1)を透過して出力されるレ
ーザビームである。
(7a) and (7b) are the first dielectric electrode (la)
, (lb) and the second dielectric body electrode (4a),
(4b) are AC high voltage power supplies independently connected to each other. Is (8) No. 1 of the Book of G? A electric body electrode (la), (l
b) and the silent radiation generated between the second dielectric electric ladders (4a) and (4b), Ho) and (11) are a total reflection mirror and a partial reflection mirror arranged on the optical axis of the laser beam.
(12) is a laser beam transmitted through the partially reflecting mirror (!1) and output.

また、上記の真空容器(2)内には炭酸ガスを含んだ混
合ガス(He 、H2、CO2、Co等の混合ガス)充
填される。
Further, the vacuum container (2) is filled with a mixed gas containing carbon dioxide (a mixed gas of He, H2, CO2, Co, etc.).

上記の構成において、第1誘電体電極(la) 。In the above configuration, the first dielectric electrode (la).

(1b)および第2誘電体電極(4a) 、 (4b)
間に、それぞれ別個に接続した交流高電圧電源(7a)
 、 (7b)より交流高電圧が印加されると、前記誘
電体電極間に形成される放電空間に無声放電(8)と呼
ばれる安定な放電が生じる。この無声放電は誘電体(3
a)、 (3b)、 (6a)、 (6b)を介した交
流放電であるため、アーク放電に移行することなく、電
子温度のみが高く、分子温度の上昇しない非乎衡放電が
安定に実現できる。上記の放電空間内で無声放電が起こ
ると、全反射鏡(10)と部分反射鏡(11)とにより
構成される共振器内でレーザ発振が起り、部分反射鏡(
11)を透過してレーザビーム(12)が出力される。
(1b) and second dielectric electrode (4a), (4b)
AC high voltage power supplies (7a) connected separately between
, (7b) When an AC high voltage is applied, a stable discharge called a silent discharge (8) occurs in the discharge space formed between the dielectric electrodes. This silent discharge is caused by a dielectric (3
Since it is an AC discharge via a), (3b), (6a), and (6b), a stable non-equilibrium discharge in which only the electron temperature is high and the molecular temperature does not rise is realized without transitioning to arc discharge. can. When a silent discharge occurs in the above-mentioned discharge space, laser oscillation occurs in the resonator formed by the total reflection mirror (10) and the partial reflection mirror (11), and the partial reflection mirror (11) causes laser oscillation.
11) and a laser beam (12) is output.

[発明が解決しようとする問題点] 従来の無声放電式ガスレーザ装置では、上記のように光
軸方向に分割された第1誘電体電極(la)、 (lb
)と第2誘電体電極(4a)、 (4b)が配置され、
その各々に独立した交流高電圧電源(7a)、 (7b
)が接続されているので、その各々の容量が小さくて済
むこと、下位機種ユニットに使用可能になる等の利点を
有する反面、次のよな問題点がある。すなわち、第1誘
電体電極(la)、 (lb)間に印加される交流高電
圧■l、第2?A電体′這極(4a)、 (4b)間に
印加される交流高電圧V2の14波数と位相が揃ってい
ないと、隣り合った上部の第1誘電体電極(la) 、
第2誘電体電極(4a)間、または隣り合った下部の第
1誘電体電極(lb) 。
[Problems to be Solved by the Invention] In the conventional silent discharge gas laser device, the first dielectric electrode (la), (lb) divided in the optical axis direction as described above.
) and second dielectric electrodes (4a) and (4b) are arranged,
Independent AC high voltage power supplies (7a) and (7b)
) are connected, which has advantages such as the capacity of each unit being small and being usable for lower model units, but has the following problems. That is, the AC high voltage ■l applied between the first dielectric electrodes (la) and (lb), and the second dielectric electrode (lb). If the phases are not aligned with the 14-wave number of the AC high voltage V2 applied between the A-electrode poles (4a) and (4b), the adjacent upper first dielectric electrodes (la),
Between the second dielectric electrodes (4a) or adjacent lower first dielectric electrodes (lb).

第2誘電体電極(4b)間に高電圧がかかることがあり
、それら金属電極(2a) 、 (2b) 、 (5a
) 、 (5b)の表面に被覆した誘電体(3a)、 
(3b)、 (6a)、 (6b)が絶縁破壊し、前記
誘電体電極(la) 、 (4a)間、または前記誘電
体電極(lb) 、 (4b)間に異常放電(9a)、
 (9b)が発生する。第4図に上記の交流高電圧v1
 。
A high voltage may be applied between the second dielectric electrodes (4b), and these metal electrodes (2a), (2b), (5a
), a dielectric (3a) coated on the surface of (5b),
(3b), (6a), (6b) undergo dielectric breakdown and abnormal discharge (9a) between the dielectric electrodes (la) and (4a) or between the dielectric electrodes (lb) and (4b);
(9b) occurs. Figure 4 shows the above AC high voltage v1.
.

■2と異常放電電圧v3の電圧波形を、横軸に時間を取
ったグラフで示す。
The voltage waveforms of (2) and the abnormal discharge voltage v3 are shown in a graph with time plotted on the horizontal axis.

上記の異常放電(9a)、 (9b)により、真空容器
(2)内に充填した炭酸ガスを含んだ混合ガスが劣化し
、レーザビーム(12)の出力が低下したり、第1J’
it体電極(la)、 (xb)、第2誘電体電極(4
a)、 (4b)が損傷したりするおそれがある。さら
に、上記の異常放電(9a)、 (9b)を防止するた
めに、2分割した上記の第1誘電体電極(la)。
Due to the above abnormal discharges (9a) and (9b), the mixed gas containing carbon dioxide filled in the vacuum container (2) deteriorates, and the output of the laser beam (12) decreases.
IT body electrodes (la), (xb), second dielectric electrode (4
a) and (4b) may be damaged. Furthermore, in order to prevent the above abnormal discharges (9a) and (9b), the above first dielectric electrode (la) is divided into two.

第2誘電体電極(4a)間、および下部の第1誘電体電
極(lb) 、第2誘電体電極(4b)間の絶縁距離を
十分確保する必要があり、その場合には無声放電式カス
レーザ装置全体が長大化する等の問題点もあった。
It is necessary to ensure sufficient insulation distance between the second dielectric electrodes (4a) and between the first dielectric electrode (lb) and the second dielectric electrode (4b) at the bottom. There were also problems such as the overall length of the device.

この発明は上記のような問題点を解消するためになされ
たもので、各誘電体電極間に異常放電が生じることがな
く、真空容器内に充填した混合ガスの劣化、各誘電体電
極の損傷を防止し、高効率、高信頼性の無声放電式ガス
レーザ装置を得ることを目的とする。
This invention was made to solve the above-mentioned problems, and it prevents abnormal discharge from occurring between each dielectric electrode, causing deterioration of the mixed gas filled in the vacuum container, and damage to each dielectric electrode. The purpose of this invention is to obtain a silent discharge type gas laser device with high efficiency and high reliability.

[問題点を解決するための手段] この発明に係る無声放電式ガスレーザ装置は、一対の誘
電体電極に印加する交流高電圧の周波数と位相とを複数
の組の間で一致させる基準発蛋器等の周波数Φ位相間期
手段を備えたものである。
[Means for Solving the Problems] The silent discharge gas laser device according to the present invention has a reference incubator that matches the frequency and phase of AC high voltage applied to a pair of dielectric electrodes between a plurality of sets. It is equipped with a frequency Φ phase interval means such as .

[作用] この発明における無声放電式ガスレーザ装置は、基準発
振器等の周波数・位相同期手段により、誘電体電極間に
印加される交流高電圧の周波数と位相の同期を取り、各
個に独立して設けた交流高電圧電源から同一周波数、同
一位相の高電圧が印加されることになる。
[Function] The silent discharge type gas laser device according to the present invention synchronizes the frequency and phase of the AC high voltage applied between the dielectric electrodes using frequency/phase synchronization means such as a reference oscillator, and synchronizes the frequency and phase of the AC high voltage applied between the dielectric electrodes. High voltages of the same frequency and phase are applied from the AC high voltage power supply.

[実施例1 以下、この発明の一実施例を図について説明する。[Example 1 An embodiment of the present invention will be described below with reference to the drawings.

第1図はこの発明の無声放電式ガスレーザ装置の原理構
成図であり、従来の無声放電式ガスレーザ装置と同一部
分には同一符号を付してその詳しい説明は省略する。
FIG. 1 is a diagram illustrating the basic structure of a silent discharge gas laser device according to the present invention, and the same parts as those of a conventional silent discharge gas laser device are given the same reference numerals, and detailed explanation thereof will be omitted.

図において、(13)は、交流高電圧電源(7a) 。In the figure, (13) is an AC high voltage power supply (7a).

(7b)の周波数と位相の同期を取るだめの周波数・位
相同期手段であり、例えば一つの2!準発振器(13a
)を備えたものであるが、複数備えた各交流高電圧電源
間で上記周波数と位相とを一致させ得る7段であれば、
他の同期回路等で置換筒f七である。
It is a frequency/phase synchronization means for synchronizing the frequency and phase of (7b), for example, one 2! Quasi-oscillator (13a
), but if it has seven stages that can match the frequency and phase between each of the multiple AC high voltage power supplies,
There are other synchronous circuits, etc., and the replacement tube is f7.

上記の構成により分割された第1誘電体電極(la) 
、 (lb)間、第2誘電体電極(4a) 、 (4b
)間の電圧vl、v2は第2図に示すように、同一周波
数、同一位相となり、したがって隣り合った上部の第1
誘電体電極(la)、第2誘電体電極(4a)、および
下部の第2誘電体電極(lb) 、 (4b)の電位は
同電位となり、電圧差■3がほぼ零となるため、その間
での異常放電が生じなくなる。
The first dielectric electrode (la) divided according to the above configuration
, (lb), the second dielectric electrode (4a), (4b
) between the voltages vl and v2 have the same frequency and the same phase, as shown in Fig.
The potentials of the dielectric electrode (la), the second dielectric electrode (4a), and the lower second dielectric electrodes (lb) and (4b) are at the same potential, and the voltage difference 3 becomes almost zero, so that Abnormal discharge will no longer occur.

なお、上記の実施例では誘電体電極を2分割し、2つの
交流高電圧電源を接続した例について説明し、また図示
したが、これらは必ずしも2分割に限定されるものでは
なく、誘電体電極を複数に分割し、夫々に対応する複数
の交流高電圧電源を設けたものにも適用することができ
る。
In addition, in the above embodiment, an example was explained and illustrated in which the dielectric electrode was divided into two and two AC high voltage power supplies were connected, but these are not necessarily limited to two divisions, and the dielectric electrode It can also be applied to a system in which the system is divided into a plurality of parts and a plurality of AC high voltage power supplies corresponding to each part are provided.

[発明の効果] 以りのようにこの発明によれば、一対の誘′心体′屯極
に印加する交流高゛屯圧の周波数と位相とを複数の組の
間で同じにする基準発振器等の周波数・位相同期1段を
備えたので、隣り合った上部誘′市体電極、または下部
誘電体電極が、互いに同電位となり、したがってそれら
電極間での電位差がなくなるので、異常放電が防止され
、真空容器内に充填される混合ガスの劣化によるレーザ
ビームの出力の低下、誘電体電極の損傷がなくなり、高
効率、高信頼性の無声数′を式ガスレーザ装置が得られ
、また、誘電体電極間の絶縁距離が短くでき、そのため
無声放電式ガスレーザ装置の小型化が実現できる等の効
果を奏する。
[Effects of the Invention] As described above, according to the present invention, there is provided a reference oscillator that makes the frequency and phase of the AC high pressure applied to a pair of dielectric body poles the same among a plurality of sets. Since it is equipped with one stage of frequency and phase synchronization, adjacent upper dielectric electrodes or lower dielectric electrodes have the same potential, and therefore there is no potential difference between them, preventing abnormal discharge. As a result, a decrease in laser beam output due to deterioration of the mixed gas filled in the vacuum chamber and damage to the dielectric electrode are eliminated, and a highly efficient and reliable gas laser device with a silent number' formula can be obtained. The insulation distance between the body electrodes can be shortened, and therefore the silent discharge type gas laser device can be miniaturized.

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

第1図はこの発明の一実施例を示す無声放電式カスレー
ザ装置の原理構成図、第2図はL記無声放゛・u式ガス
レーザ装置における誘電体電極間の電圧波形図、第3図
は従来の無声放電式ガスレーザ装置の原理構成図、第4
図は一ト記従来の無声数′1[式ガスレーザ装置におけ
る誘電体電極間の電圧波形図である。 (la) 、 (lb)・・−第1誘電体電極、(4a
) 、 (4b)・・・第2誘電体電極、(5)・・・
無声放電、(7a) 。 (7h)・・・交流高電圧電源、(io)・・・全反射
鏡、(11)・・・部分反射鏡、(12)・・・レーザ
ビーム、(13)・・・周波数−位相同期手段、 (1
3a)・・・基準発振器。 なお、各図中、同一符号は同一または相当部分を示す。
Fig. 1 is a diagram showing the principle configuration of a silent discharge type gas laser device showing one embodiment of the present invention, Fig. 2 is a voltage waveform diagram between dielectric electrodes in a silent discharge type gas laser device of L type, and Fig. 3 is Principle configuration diagram of conventional silent discharge type gas laser device, No. 4
The figure is a voltage waveform diagram between dielectric electrodes in a conventional unvoiced number '1' type gas laser device. (la), (lb)...-first dielectric electrode, (4a
), (4b)...second dielectric electrode, (5)...
Silent discharge, (7a). (7h)... AC high voltage power supply, (io)... Total reflection mirror, (11)... Partial reflection mirror, (12)... Laser beam, (13)... Frequency-phase synchronization means, (1
3a)...Reference oscillator. In each figure, the same reference numerals indicate the same or corresponding parts.

Claims (1)

【特許請求の範囲】[Claims] 金属電極の表面に誘電体を被覆した一対の誘電体電極を
少なくとも二組以上備え、前記一対の誘電体電極に交流
高電圧電源が個々に独立して接続された無声放電式ガス
レーザ装置において、前記一対の誘電体電極に印加され
る交流高電圧の周波数と位相とを複数の組の間で一致さ
せる周波数・位相同期手段を備えたことを特徴とする無
声放電式ガスレーザ装置。
A silent discharge gas laser device comprising at least two or more pairs of dielectric electrodes in which the surfaces of metal electrodes are coated with a dielectric material, and an AC high voltage power source is individually and independently connected to the pair of dielectric electrodes. A silent discharge gas laser device characterized by comprising frequency/phase synchronization means for matching the frequency and phase of an AC high voltage applied to a pair of dielectric electrodes between a plurality of pairs.
JP20308686A 1986-08-29 1986-08-29 Silent discharge type gas laser device Pending JPS6358885A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP20308686A JPS6358885A (en) 1986-08-29 1986-08-29 Silent discharge type gas laser device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP20308686A JPS6358885A (en) 1986-08-29 1986-08-29 Silent discharge type gas laser device

Publications (1)

Publication Number Publication Date
JPS6358885A true JPS6358885A (en) 1988-03-14

Family

ID=16468131

Family Applications (1)

Application Number Title Priority Date Filing Date
JP20308686A Pending JPS6358885A (en) 1986-08-29 1986-08-29 Silent discharge type gas laser device

Country Status (1)

Country Link
JP (1) JPS6358885A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6364383A (en) * 1986-09-04 1988-03-22 Fanuc Ltd Gas laser device
JPS6398172A (en) * 1986-10-15 1988-04-28 Toshiba Corp High speed repetition pulse gas laser

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5513970A (en) * 1978-07-17 1980-01-31 Nec Corp Gas laser device
JPS56131986A (en) * 1980-03-19 1981-10-15 Mitsubishi Electric Corp Gas laser device
JPS56134790A (en) * 1980-03-26 1981-10-21 Mitsubishi Electric Corp Gas laser device

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5513970A (en) * 1978-07-17 1980-01-31 Nec Corp Gas laser device
JPS56131986A (en) * 1980-03-19 1981-10-15 Mitsubishi Electric Corp Gas laser device
JPS56134790A (en) * 1980-03-26 1981-10-21 Mitsubishi Electric Corp Gas laser device

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6364383A (en) * 1986-09-04 1988-03-22 Fanuc Ltd Gas laser device
JPS6398172A (en) * 1986-10-15 1988-04-28 Toshiba Corp High speed repetition pulse gas laser

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