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JPH01103889A - Gas laser generating device - Google Patents

Gas laser generating device

Info

Publication number
JPH01103889A
JPH01103889A JP13978787A JP13978787A JPH01103889A JP H01103889 A JPH01103889 A JP H01103889A JP 13978787 A JP13978787 A JP 13978787A JP 13978787 A JP13978787 A JP 13978787A JP H01103889 A JPH01103889 A JP H01103889A
Authority
JP
Japan
Prior art keywords
discharge
electrode
auxiliary
current
discharge 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
Application number
JP13978787A
Other languages
Japanese (ja)
Inventor
Minoru Suzuki
実 鈴木
Tsutomu Sugiyama
勤 杉山
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.)
Hitachi Ltd
Original Assignee
Hitachi 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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP13978787A priority Critical patent/JPH01103889A/en
Publication of JPH01103889A publication Critical patent/JPH01103889A/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
    • H01S3/02Constructional details
    • H01S3/03Constructional details of gas laser discharge tubes
    • H01S3/038Electrodes, 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

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、補助電極を改良したガスレーザ発生装置に関
する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a gas laser generator with an improved auxiliary electrode.

〔従来の技術〕[Conventional technology]

ガスレーザ発生装置の出力を増加させる目的で、放電管
内のガス圧を高くすることが行なわれる。
In order to increase the output of the gas laser generator, the gas pressure within the discharge tube is increased.

一方、ガス圧を上昇させると放電開始電圧が上昇する為
、放電開始を円滑に行なわせるために、放電管内に補助
電極を設置し外部より電圧を印加する方式が提案されて
いる(例えば特開昭60−161687号)。
On the other hand, since the discharge starting voltage increases when the gas pressure increases, in order to start the discharge smoothly, a method has been proposed in which an auxiliary electrode is installed inside the discharge tube and a voltage is applied from the outside (for example, (Sho 60-161687).

従来のガスレーザ発生装置を第4図、第5図(A)、(
B)、(C)により説明する。スイッチ22をオンして
、放電管1内の主電極2と3との間および主電極2と補
助電極30との間に直流電源21を接続し、直流電源の
放電電源電圧Vを印加すると、グロー放電電流11およ
び補助電流12が流れる。放電電源電圧V、グロー放電
電流11、補助電流12と時間tとの関係の変化は、第
5図(A)ないしくC)に示す特性図となる。
Conventional gas laser generators are shown in Figures 4, 5 (A), and (
This will be explained using B) and (C). When the switch 22 is turned on, the DC power supply 21 is connected between the main electrodes 2 and 3 in the discharge tube 1 and between the main electrode 2 and the auxiliary electrode 30, and the discharge power supply voltage V of the DC power supply is applied. A glow discharge current 11 and an auxiliary current 12 flow. Changes in the relationship between the discharge power supply voltage V, the glow discharge current 11, the auxiliary current 12, and the time t are shown in the characteristic diagrams shown in FIGS. 5(A) to 5(C).

放電電源電圧■は第5図(A)に示す如く、放電開始時
に高く、放電開始後は時間tの経過と共に一定となるの
で、グロー放電電流11も同図(B)になる。グロー放
電電流11は放電開始時を除き一定である。放電開始時
は、同図(C)に示す如く、補助電流12が急激に増加
し、放電開始後は時間tの経過と共に一定になる。
As shown in FIG. 5(A), the discharge power supply voltage {circle around (2)} is high at the start of discharge and becomes constant as time t elapses after the start of discharge, so that the glow discharge current 11 also becomes as shown in FIG. 5(B). The glow discharge current 11 is constant except at the start of discharge. At the start of discharge, the auxiliary current 12 increases rapidly, as shown in FIG. 3(C), and after the start of discharge, it becomes constant as time t passes.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

このように、従来例においては、放電管内に補助電極3
0を設置している為に放電が開始された後も、補助電極
30でグロー放電が維持される為に、補助電流12が流
れ続け、この電流値を規制する抵抗器31が必要であり
、抵抵器31の発熱で熱的な損失が発生する。又、補助
電極30の損耗による放電管内の汚損及び放電管内に補
助電極30を設置する為に構造が複雑になる等の欠点を
有していた。
In this way, in the conventional example, the auxiliary electrode 3 is placed inside the discharge tube.
Since glow discharge is maintained at the auxiliary electrode 30 even after the discharge has started, the auxiliary current 12 continues to flow, and a resistor 31 is required to regulate this current value. The heat generated by the resistor 31 causes thermal loss. Further, there are drawbacks such as contamination of the inside of the discharge tube due to wear and tear of the auxiliary electrode 30 and a complicated structure due to the installation of the auxiliary electrode 30 inside the discharge tube.

ちなみに上記の抵抗における発生熱を概算すると、放電
管を4本使用した500W級の発振器においては、補助
電極の電流規制抵抗は2MΩ程度となり、放電維持電圧
が12kVであることより発生熱量は、288Wとなり
、発振出力の半分以上の熱が損失として放出されている
ことが解る。
By the way, roughly estimating the heat generated in the above resistance, in a 500W class oscillator using four discharge tubes, the current regulating resistance of the auxiliary electrode is about 2MΩ, and the discharge sustaining voltage is 12kV, so the amount of heat generated is 288W. It can be seen that more than half of the heat of the oscillation output is released as loss.

本発明の目的は、放電開始時のみ主電極と補助電極との
間に補助電流を流すようにして、消費電力を低減したガ
スレーザ発生装置を提供することにある。
An object of the present invention is to provide a gas laser generator that reduces power consumption by flowing an auxiliary current between a main electrode and an auxiliary electrode only at the start of discharge.

〔問題点を解決するための手段〕[Means for solving problems]

放電管内側と外側との一方の主電極と補助電極とを対向
して配置し、補助電極を他方の主電極と同電位になるよ
うに接続する。
A main electrode and an auxiliary electrode on one of the inside and outside of the discharge tube are arranged to face each other, and the auxiliary electrode is connected to the other main electrode so as to have the same potential.

〔作用〕[Effect]

グロー放電開始前の放電電源電圧Vは、充電電圧の最高
値まで急激に電圧を上昇させるので、電圧の時間変化(
dv/dt)が大きいが、−旦放電を開始するとグロー
放電の一定電圧値となる為、d v / d tは小さ
な値となる。補助電極と主電極の間は放電管の壁で仕切
られており、この間のインピーダンスは静電容量である
ことにより、dv/dtが大きい時だけ補助電流が供給
されるようにした。
The discharge power supply voltage V before the start of glow discharge rapidly increases to the maximum value of the charging voltage, so the voltage change over time (
dv/dt) is large, but once the discharge starts, it becomes a constant voltage value of glow discharge, so dv/dt becomes a small value. The auxiliary electrode and the main electrode are separated by the wall of the discharge tube, and the impedance between them is capacitance, so that the auxiliary current is supplied only when dv/dt is large.

〔実施例〕〔Example〕

以下、本発明の実施例を第1図に示し説明する。 An embodiment of the present invention is shown in FIG. 1 and will be described below.

第1図は、放電管1を2本面列に接続した例である。FIG. 1 shows an example in which discharge tubes 1 are connected in a two-sided row.

供給管12より供給されたレーザガス12Aは、放電管
1を通過後排気管13より排出され、図示を省略したガ
ス循環装置、冷却装置により再び供給管12へ供給され
ている。放電管1はガラス。
The laser gas 12A supplied from the supply pipe 12 passes through the discharge tube 1 and is discharged from the exhaust pipe 13, and is supplied to the supply pipe 12 again by a gas circulation device and a cooling device (not shown). Discharge tube 1 is glass.

セラミックス等の絶縁物で形成され、その内部に陽極側
および陰極側の主電極2および3が設けられている。主
電極2,3の間には、直流電源21が接続されており、
放電により励起されたレーザガス12Aは、出力鏡5と
全反射鏡6の間でレーザ発振を生じ、外部ヘレーザ光7
が放出される。
It is formed of an insulator such as ceramics, and main electrodes 2 and 3 on the anode side and the cathode side are provided inside. A DC power supply 21 is connected between the main electrodes 2 and 3,
The laser gas 12A excited by the discharge causes laser oscillation between the output mirror 5 and the total reflection mirror 6, and external laser light 7 is generated.
is released.

一方の主電極側の放電管外側には導体形で形成されたリ
ングから成る補助電極4が設置されている。
An auxiliary electrode 4 consisting of a ring formed in the shape of a conductor is installed on the outside of the discharge tube on the side of one of the main electrodes.

補助電極4は他方の主電極3と同電位に電気的に接続さ
れている。
The auxiliary electrode 4 is electrically connected to the other main electrode 3 at the same potential.

次に、スイッチ22をオンして、主電極2と3との間お
よび主電極2と補助電極4との間に直流電源21の放電
電源電圧Vを印加すると、第3図(A)、同図(B)に
は、第5図(A)、(B)と同様な放電電源電圧■およ
びグロー放電電流11が流れるが、グロー放電開始時は
、同図(C)に示す補助電流12が流れる。補助電流1
2は放型開始時に急激に流れるが、放電開始後は流れな
い。この理由は、主電極2と補助電極4との間には放電
管1の壁で仕切られており、この間のインピーダンスは
静電容量であることにより、放電開始時の放電電源電圧
Vの時間的変化(dv/dt)が大きい時だけ、補助電
流12が流れる。つまり補助電流12の大きい時だけ流
れ、補助電流12が小さい時は流れない。補助電流12
が小さい時は放電管1の絶縁物(誘電率1)により、補
助電流12の流れが阻止される。
Next, when the switch 22 is turned on and the discharge power supply voltage V of the DC power supply 21 is applied between the main electrodes 2 and 3 and between the main electrode 2 and the auxiliary electrode 4, as shown in FIG. In Figure (B), the same discharge power supply voltage ■ and glow discharge current 11 as in Figures 5 (A) and (B) flow, but at the start of glow discharge, the auxiliary current 12 shown in Figure 5 (C) flows. flows. Auxiliary current 1
No. 2 flows rapidly at the start of mold release, but does not flow after the start of discharge. The reason for this is that the main electrode 2 and the auxiliary electrode 4 are partitioned by the wall of the discharge tube 1, and the impedance between them is capacitance. The auxiliary current 12 flows only when the change (dv/dt) is large. In other words, it flows only when the auxiliary current 12 is large, and does not flow when the auxiliary current 12 is small. Auxiliary current 12
When the auxiliary current 12 is small, the insulator (dielectric constant 1) of the discharge tube 1 blocks the flow of the auxiliary current 12.

〔発明の効果〕〔Effect of the invention〕

この結果、本発明の実施例によれば、従来必要であった
、補助電流制御用抵抗が不要となり、抵抗で発生してい
た熱損失の発生が無く、レーザ発振に必要な電力量の低
減を画ることができる。又、放電管外に補助電極を設置
する為、電極の消耗等による発振器内の汚損及び、電極
の交換が不要となり信頼性の向上する等の効果を得るこ
とができる。
As a result, according to the embodiment of the present invention, there is no need for an auxiliary current control resistor, which was necessary in the past, and there is no heat loss caused by the resistor, reducing the amount of power required for laser oscillation. I can draw. In addition, since the auxiliary electrode is installed outside the discharge tube, there is no need for contamination in the oscillator due to electrode consumption, and there is no need to replace the electrode, resulting in improved reliability.

又、パルス放電により短時間で高パルスピークの発振を
行なう場合は、短時間内に電流をレーザガスに供給する
必要がある為、一般に放電電源の電源立上がり特性を速
くするが、本発明は、この様な場合に更に急峻な電流供
給が行なえる為、放電の立上がりが早くなり一層の効果
を得ることができる。
In addition, when oscillating with a high pulse peak in a short period of time by pulse discharge, it is necessary to supply current to the laser gas within a short period of time. In such cases, a steeper current supply can be performed, so that the discharge rises more quickly and even more effects can be obtained.

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

第1図は本発明の実施例であるガスレーザ発生装置の概
略斜視図、第2図は第1図の概略説明図、第3図(A)
ないしくB)は第1図、第2図の特性図、第4図は従来
のガスレーザ発生装置の概略説明図、第5図(A)ない
しくC)は第4図の特性図である。 1・・・放電管、2および3・・・陽極および陰極側の
主電極、4・・・補助電極。
FIG. 1 is a schematic perspective view of a gas laser generator according to an embodiment of the present invention, FIG. 2 is a schematic explanatory diagram of FIG. 1, and FIG. 3 (A)
or B) are characteristic diagrams of FIGS. 1 and 2, FIG. 4 is a schematic explanatory diagram of a conventional gas laser generator, and FIGS. 5(A) to C) are characteristic diagrams of FIG. 4. DESCRIPTION OF SYMBOLS 1...Discharge tube, 2 and 3...Main electrodes on anode and cathode sides, 4...Auxiliary electrode.

Claims (1)

【特許請求の範囲】[Claims] 1. 放電管内にレーザガスを供給し、放電管内に少な
くとも一対の主電極を配置し、主電極間を直流回路に接
続し、主電極間に直流回路の電圧を印加し、主電極間に
グロー放電を発生させ、グロー放電によりレーザガスを
励起し、レーザ光を発生する装置において、上記一方の
主電極側の放電管外側に補助電極を設け、補助電極を他
方側主電極と同電位に接続することを特徴とするガスレ
ーザ発生装置。
1. Supply laser gas into the discharge tube, place at least one pair of main electrodes inside the discharge tube, connect the main electrodes to a DC circuit, apply the voltage of the DC circuit between the main electrodes, and generate a glow discharge between the main electrodes. The device excites laser gas by glow discharge to generate laser light, characterized in that an auxiliary electrode is provided outside the discharge tube on the side of one of the main electrodes, and the auxiliary electrode is connected to the same potential as the main electrode on the other side. Gas laser generator.
JP13978787A 1987-06-05 1987-06-05 Gas laser generating device Pending JPH01103889A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP13978787A JPH01103889A (en) 1987-06-05 1987-06-05 Gas laser generating device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP13978787A JPH01103889A (en) 1987-06-05 1987-06-05 Gas laser generating device

Publications (1)

Publication Number Publication Date
JPH01103889A true JPH01103889A (en) 1989-04-20

Family

ID=15253417

Family Applications (1)

Application Number Title Priority Date Filing Date
JP13978787A Pending JPH01103889A (en) 1987-06-05 1987-06-05 Gas laser generating device

Country Status (1)

Country Link
JP (1) JPH01103889A (en)

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0788201A1 (en) 1996-02-02 1997-08-06 Shibuya Kogyo Co., Ltd Laser oscillator
JPH1012948A (en) * 1996-06-18 1998-01-16 Kawasaki Heavy Ind Ltd Axial-flow type gas laser device and operating method thereof
WO1999060676A1 (en) * 1998-05-20 1999-11-25 Kabushiki Kaisha Toshiba Pulsed gas laser device
WO2001093380A1 (en) * 2000-05-30 2001-12-06 Matsushita Electric Industrial Co., Ltd. Laser oscillating device
EP1326311A1 (en) * 2000-05-30 2003-07-09 Matsushita Electric Industrial Co., Ltd. Auxiliary electrode for gas laser oscillator
CN104333353B (en) * 2014-09-30 2017-01-18 西北核技术研究所 Integrated sharpening unit used for electromagnetic pulse simulation device

Cited By (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0788201A1 (en) 1996-02-02 1997-08-06 Shibuya Kogyo Co., Ltd Laser oscillator
US5790582A (en) * 1996-02-02 1998-08-04 Shibuya Kogyo Co., Ltd. Laser oscillator
JPH1012948A (en) * 1996-06-18 1998-01-16 Kawasaki Heavy Ind Ltd Axial-flow type gas laser device and operating method thereof
WO1999060676A1 (en) * 1998-05-20 1999-11-25 Kabushiki Kaisha Toshiba Pulsed gas laser device
WO2001093380A1 (en) * 2000-05-30 2001-12-06 Matsushita Electric Industrial Co., Ltd. Laser oscillating device
EP1248332A4 (en) * 2000-05-30 2003-01-29 Matsushita Electric Ind Co Ltd Laser oscillating device
EP1326311A1 (en) * 2000-05-30 2003-07-09 Matsushita Electric Industrial Co., Ltd. Auxiliary electrode for gas laser oscillator
US6895030B1 (en) 2000-05-30 2005-05-17 Matsushita Electric Industrial Co., Ltd. Laser oscillating device
US6944200B2 (en) 2000-05-30 2005-09-13 Matsushita Electric Industrial Co., Ltd. Laser oscillator
CN104333353B (en) * 2014-09-30 2017-01-18 西北核技术研究所 Integrated sharpening unit used for electromagnetic pulse simulation device

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