JPH0318073A - Metal vapor laser device - Google Patents

Metal vapor laser device

Info

Publication number
JPH0318073A
JPH0318073A JP15193089A JP15193089A JPH0318073A JP H0318073 A JPH0318073 A JP H0318073A JP 15193089 A JP15193089 A JP 15193089A JP 15193089 A JP15193089 A JP 15193089A JP H0318073 A JPH0318073 A JP H0318073A
Authority
JP
Japan
Prior art keywords
pulse
generating circuit
discharge
switch means
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
JP15193089A
Other languages
Japanese (ja)
Inventor
Akihiko Iwata
明彦 岩田
Shigeo Eguri
成夫 殖栗
Kazuhiko Hara
一彦 原
Yoichiro Tabata
要一郎 田畑
Yoshihiro Ueda
植田 至宏
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 JP15193089A priority Critical patent/JPH0318073A/en
Publication of JPH0318073A publication Critical patent/JPH0318073A/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
    • H01S3/031Metal vapour lasers, e.g. metal vapour generation

Landscapes

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

Abstract

PURPOSE:To get high efficiency even in the case where the number of pulse repeat is high by providing a second pulse generating circuit separately from a first pulse generating circuit, and applying first pulse voltage from the first pulse generating circuit to a discharge tube, and then applying second pulse voltage from the second pulse generating circuit, being delayed by specified time. CONSTITUTION:This is equipped with a first pulse generating circuit 13a, which supplies first pulse voltage for generating gas discharge in a discharge tube 11, and a second pulse generating circuit 13b, which supplies second pulse voltage to the discharge tube 11 being delayed by a specified time from the first pulse voltage, and those are composed of charge/discharge capacitors 14a and 14b and switching means 15a and 15b being constituted by connecting many solid switching elements in series and parallel. And this is equipped with high voltage power sources 17a and 17b which supply power, through interference preventing reactors 20a and 20b, to the charge/ discharge capacitors 14a and 14b of the first and second pulse generating circuits 13a and 13b. Accordingly, the relaxation from a lower state to a ground state is accelerated between each pulse, and the inverted population with the next pulse becomes complete. Hereby, even if the number of pulse repeat is high, high efficiency can be obtained.

Description

【発明の詳細な説明】[Detailed description of the invention]

[産業上の利用分野] この発明はガス放電によって金属を加熱、気化させてレ
ーザ出力を得る放電管を備えた金属蒸気レーザ装置に関
するものである。 [従来の技術] 第4図は、例えばコツパー バボウア レーザス カム
 オフ゛エージイ(COPPER  VAPORLAS
ERS  COME  OF  AGE)レーザ フォ
ーカス ジュライ 1 9 8 2 (LASERFO
CUS, JULY, 1982)に記載された、従来
の銅蒸気レーザ装置の駆動C原としてのパルス発生回路
を示す図であり、第4図において1は高圧電諒、2は充
電用リアクトル、3は充電用ダイオード、4は充放電を
行うコンデンサ、5は充電用抵抗、6はサイラトロンス
イッチ、7は放電管(レーザTUBE)である。 次に動作について説明する。高圧電源1から発生される
高圧電圧(数KV〜数十KV)は、リアクトル2、ダイ
オード3、充電用抵抗5を介してコンデンサ4に充電さ
れる。 この充電状態において、サイラトロンスイッチ6が導通
すると、主コンデンサ4に蓄えられていた電圧は、サイ
ライトロンスイッチ6を通り放電管7に印加され、放電
管7の中にガス放電を形成する.その際、放電管7のイ
ンピーダンスは充電用抵抗5の抵抗値より大幅に小さく
なるために、サイラトロンスイッチ6に流れる電流は主
として放電管7に流れる。 この放電の熱エネルギによって、放電管7内の温度は1
 500℃程度の高温に上昇し、予じめ収納してある金
属例えば銅粒子を蒸気にすると共に放電管内に銅蒸気を
充満させる。 放電管7内に形成されたガス放電によって放電プラズマ
の電子を加速し、この電子は放電管7内に充満された銅
原子に衝突すると共に銅原子の原子レベルを第一共鳴準
位である上準位に励起し、準安定準位である下準位へ励
起される数は少ないため、反転分布が形成される。上準
位にある銅原子はレーザ発振を伴って下準位に落ち、さ
らに下準位から基底準位にゆっくりと緩和する。以上の
動作を数KHzで繰り返す。 下準位から基底準位への緩和は放電管7の口径が小さい
場合は、放電管7の壁と励起原子との衝突で行われ、放
電管7の口径が大きい場合は、下準位原子と低速電子と
の超弾性衝突にて行われ、その寿命は数百μsecと長
い。 〔発明が解決しようとする課題〕 従来の銅蒸気レーザ装置は以上のように構成されている
ので、下準位から基底準位に緩和する時間が数百μSe
Cと非常に長く、緩和が終了するのを待って次のパルス
を印加するとパルス繰り返し数が小さくなり、またパル
ス繰り返し数を高くするとパルス印加時の下準位の数が
多くなるため反転分布が不完全となり銅蒸気レーザの効
率が低下するという問題点があった。 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、各パルスの間で下準位から基底準位への緩和
を促進させ、次のパルスでの反転分布をより安全なもの
とすることで、パルス繰り返し数が高い場合でも、効率
が高い金属蒸気レーザ装置を得ることを目的とする。 〔課題を解決するための手段】 この発明に係る金属蒸気レーザ装置は、充放電コンデン
サと多数の固体スイッチング素子を直並列接続して構成
したスイッチ手段からなり、前記放電管にガス放電を発
生させる第1のパルス電圧を供給する第1のパルス発生
回路および該第1のパルス電圧より所定時間遅れて該放
電管に第2のパルス電圧を供給する第2のパルス発生回
路と、前記第1.第2のパ゛ルス発生回路の充放電コン
デンサにそれぞれ干渉防止リアクトルを介して給電する
別個独立に設けられた複数の高圧電源とを具備したもの
である。
[Industrial Application Field] The present invention relates to a metal vapor laser device equipped with a discharge tube that heats and vaporizes metal by gas discharge to obtain laser output. [Prior art] Fig. 4 shows, for example, a COPPER VAPORLAS cam off-age.
ERS COME OF AGE) Laser Focus July 1 9 8 2 (LASERFO
CUS, JULY, 1982) is a diagram showing a pulse generation circuit as a driving C source for a conventional copper vapor laser device, and in FIG. A charging diode, 4 a capacitor for charging and discharging, 5 a charging resistor, 6 a thyratron switch, and 7 a discharge tube (laser tube). Next, the operation will be explained. A high voltage (several KV to several tens of KV) generated from a high voltage power supply 1 is charged to a capacitor 4 via a reactor 2, a diode 3, and a charging resistor 5. In this charged state, when the thyratron switch 6 is turned on, the voltage stored in the main capacitor 4 passes through the thyratron switch 6 and is applied to the discharge tube 7, forming a gas discharge in the discharge tube 7. At this time, since the impedance of the discharge tube 7 becomes significantly smaller than the resistance value of the charging resistor 5, the current flowing through the thyratron switch 6 mainly flows through the discharge tube 7. Due to the thermal energy of this discharge, the temperature inside the discharge tube 7 increases to 1
The temperature is raised to about 500° C., and the metal, such as copper particles, stored in advance is turned into vapor, and the discharge tube is filled with copper vapor. The gas discharge formed in the discharge tube 7 accelerates electrons in the discharge plasma, and these electrons collide with the copper atoms filling the discharge tube 7 and raise the atomic level of the copper atoms to the first resonance level. Since the number excited to the lower level, which is a metastable level, is small, population inversion is formed. The copper atoms in the upper level fall to the lower level accompanied by laser oscillation, and then slowly relax from the lower level to the ground level. The above operation is repeated at several KHz. When the diameter of the discharge tube 7 is small, relaxation from the lower level to the ground level occurs through collision of the excited atoms with the wall of the discharge tube 7, and when the diameter of the discharge tube 7 is large, the relaxation occurs by the lower level atoms. This is done through superelastic collisions between low-speed electrons and low-velocity electrons, and its lifetime is as long as several hundred microseconds. [Problem to be solved by the invention] Since the conventional copper vapor laser device is configured as described above, the relaxation time from the lower level to the ground level is only a few hundred μSe.
If the next pulse is applied after waiting for the relaxation to complete, the number of pulse repetitions will become smaller, and if the number of pulse repetitions is increased, the number of lower levels during pulse application will increase, resulting in population inversion. There was a problem in that the copper vapor laser became incomplete and the efficiency of the copper vapor laser decreased. This invention was made to solve the above problems, and promotes relaxation from the lower level to the ground level between each pulse, making population inversion in the next pulse safer. By doing so, the object is to obtain a metal vapor laser device with high efficiency even when the number of pulse repetitions is high. [Means for Solving the Problems] A metal vapor laser device according to the present invention includes a switching means configured by connecting a charging/discharging capacitor and a large number of solid state switching elements in series and parallel, and generates a gas discharge in the discharge tube. a first pulse generating circuit that supplies a first pulse voltage; a second pulse generating circuit that supplies a second pulse voltage to the discharge tube after a predetermined time delay from the first pulse voltage; It is equipped with a plurality of independently provided high-voltage power supplies that respectively supply power to the charging and discharging capacitors of the second pulse generating circuit via interference prevention reactors.

【イ乍用] この発明においては、第1のパルス発生回路から供給さ
れる第1のパルス電圧間に第2のパルス発生回路から発
生される第2のパルス電圧を印加し、下準位原子と低速
電子との超弾性衝突を強性的に生じさせ、その結果、下
準位原子の緩和が促進され、第1のパルス発生回路から
第1のパルス電圧が印加される場合に反転分布がより完
全なものとなり、高い繰り返しにおいてもレーザ効率の
低下を防止する。 また、第1のパルス発生回路および第2のパルス発生回
路を多数の固体スイッチング素子を直並列接続して構成
したスイッチ手段を用いているので、応答速度が速く、
従来のサイライトロンスイッチに存在したアノードデレ
イタイムのような使用条件でスイッチング時間が変わる
ことがなく、信頼性が高く、長寿命化が図られる。 〔実施例J 以下、この発明の一実施例を図について説明する.第1
図において、1lは放電管、12は放電管l1と並列接
続した充電用抵抗、13aは充放電コンデンサ14aと
多数の固体スイッチング素子を直並列接続して構成した
スイッチ手段15aを直列接続して構成した第1のパル
ス発生回路、13bは充放電コンデンサL4bと多数の
固体スイッチング素子を直並列接続して構成したスイッ
チ手段15bを直列接続して構成した第2のパルス発生
回路である。この第1,第2のパルス発生回路13a,
13bはそれぞれリアクトル16a16bを介して放電
管11と並列接続されている。 17aはリアクトル18a、ダイオード19a、干渉防
止リアクトル20aを介して充放電コンデンサ14aに
給電する高圧電源、17bはリアクトル18b、ダイオ
ード19b、干渉防止リアクトル20bを介して充放電
コンデンサ14bに給電する高圧電源、2lはスイッチ
手段15aに導通信号を出力する発振器、22は導通信
号を所定時間遅延させてスイッチ手段15bに供給する
遅延回路である。 第2図はスイッチ手段15a,15bの具体例を示す構
成図であり、例えば多数のFET23を直並列接続した
ものである。なお、FET23の代わりに、SIT,I
GBT,SIサイリスタ、トランジスタ、サイリスク等
の固体スイッチング素子であってもよい。 次に動作を第3図のタイムチャート図を参照して説明す
る。高圧電源17a,(17b)から、リアクトル18
a (18b) 、ダイオード19a(19b).干渉
防止リアクトル20a (20b)を介して充放電コン
デンサ14a(14b)に高圧電圧が充電される。 次に、発振器2lからの導通信号によってスイッチ手段
15aが導通すると、充放電コンデンサ14aに充電さ
れた高圧電圧は放電管1lに印加され,放電管11の中
にガス放電を形成する。 一方、遅延回路22は発振器2lからの導通信号を所定
時間だけ遅延した後、スイッチ手段15bを導通させ、
充放電コンデンサ14bに充電されている高圧電圧を放
電管11に印加する。 この結果、放電管1lには、時刻七〇において、充放電
コンデンサ14aの充電電圧が印加されてガス放電を発
生し、時刻t0から所定時間でだけ遅延されて充放電コ
ンデンサ14bの充電電圧が印加される。 上記スイッチ手段15a,15bL:v導通によって該
各スイッチ手段に流れる電流Ia,Ibは、充放電コン
デンサ14a,14bとリアクトル16a,16bおよ
び放電管11のインピーダンスによって決定され第3図
に示すような波形となる。 銅蒸気レーザ装置において、下準位原子の基底準位への
緩和は、内管2の口径が大きい場合は下準位と低速電子
との超弾性衝突によって行われる。 つまり、 C u * + e ilawl− C u + e 
(rastここで、Cu*は下準位原子 Cuは基底準位原子 e jml。1は低速電子 ear畠富tlは高速電子 となる。 第2のパルス発生回路13bから印加される電圧は、銅
原子を上準位に励起しない低い電圧であるが、電子の加
速は行われるため電子と銅原子との衝突は激しくなる。 その結果、下準位原子と電子との超弾性衝突が活発にな
り、よって下準位の緩和が促進される。 なお、干渉防止リアクトル20a,20bはスイッチ手
段15a,15bを導通したときに流れる電流の周波数
成分に対しては大きなインピーダンスとなるようにイン
ダクタンス値を選ぶ。例えば一般に銅蒸気レーザ装置の
場合、放電管l1に流れる電流は、パルス幅が最大でも
500μ88Cであるから、基本周波数或分としては約
IMHzとなる。干渉防止リアクトル20a,20bが
IMHzに対し充分大きなインピーダンスを持つために
は、干渉防止リアクトル20a,20bのインダクタン
スをLzとすると、 2ifLz》Zr Zrは放電管1lのインピーダンスが必要となる。通常
、インピーダンスZTは数Ω〜数十Ωであるから、例え
ば50Ωとすると、 となる.よって、インダクタンスLzはHiooμH以
上に選べばよい。インダクタンスLzを上記のように選
択することで、例えばスイッチ手段15a,15bの導
通と共に充放電コンデンサ14a,14bから放電電流
が流れだすことはない。 【発明の効果】 以上のように、この発明によれば、第1のパルス発生回
路と別に第2のパルス発生回路を設け、放電管に第1の
パルス発生回路から第lのパルス電圧が印加された後、
所定時間遅延して第2のパルス発生回路から再び上記放
電管に第2のパルス電圧を印加するように構成したので
、下準位の原子が基底準位に緩和する時間が短縮され、
その結果第lのパルス発生回路からの次のパルス印加時
に反転分布がより完全なものとなり、高繰り返しにおい
ても効率の高い金属蒸気レーザ装置を得ることができる
効果がある. また、第1のパルス発生回路および第−2のパルス発生
回路のスイッチ手段を、多数の固体スイッチング素子を
直並列接続して構成しているので、応答速度が早く、従
来のサイラトロンスイッチに存在したアノードデレイタ
イムのような使用条件でスイッチング時間が変わること
がなく、信頼性が高く、長寿命化が図られる。
[For use] In this invention, a second pulse voltage generated from a second pulse generation circuit is applied between the first pulse voltage supplied from the first pulse generation circuit, and lower level atoms are This causes strong superelastic collisions with low-velocity electrons, and as a result, relaxation of lower-level atoms is promoted, and population inversion occurs when the first pulse voltage is applied from the first pulse generation circuit. It becomes more complete and prevents the laser efficiency from decreasing even at high repetition rates. In addition, since the first pulse generating circuit and the second pulse generating circuit are constructed using a switching means constructed by connecting a large number of solid-state switching elements in series and parallel, the response speed is fast.
The switching time does not change depending on usage conditions, such as the anode delay time that existed in conventional Cylytron switches, resulting in high reliability and long life. [Example J Hereinafter, an example of the present invention will be explained with reference to the drawings. 1st
In the figure, 1l is a discharge tube, 12 is a charging resistor connected in parallel with the discharge tube 11, and 13a is a charging/discharging capacitor 14a and a switch means 15a, which is constructed by connecting a number of solid-state switching elements in series and parallel, connected in series. The first pulse generating circuit 13b is a second pulse generating circuit constructed by connecting in series a charging/discharging capacitor L4b and a switching means 15b constructed by connecting a large number of solid state switching elements in series and parallel. These first and second pulse generation circuits 13a,
13b are connected in parallel to the discharge tube 11 via reactors 16a and 16b, respectively. 17a is a high-voltage power supply that supplies power to the charge/discharge capacitor 14a via the reactor 18a, diode 19a, and interference prevention reactor 20a; 17b is a high-voltage power supply that supplies power to the charge/discharge capacitor 14b via the reactor 18b, diode 19b, and interference prevention reactor 20b; 2l is an oscillator that outputs a conductive signal to the switch means 15a, and 22 is a delay circuit that delays the conductive signal by a predetermined time and supplies it to the switch means 15b. FIG. 2 is a block diagram showing a specific example of the switch means 15a, 15b, in which, for example, a large number of FETs 23 are connected in series and parallel. In addition, instead of FET23, SIT, I
It may also be a solid state switching element such as a GBT, SI thyristor, transistor, or thyrisk. Next, the operation will be explained with reference to the time chart shown in FIG. From the high voltage power supply 17a, (17b), the reactor 18
a (18b), diode 19a (19b). A high voltage is charged to the charge/discharge capacitor 14a (14b) via the interference prevention reactor 20a (20b). Next, when the switching means 15a is turned on by the conduction signal from the oscillator 2l, the high voltage charged in the charging/discharging capacitor 14a is applied to the discharge tube 1l, and a gas discharge is formed in the discharge tube 11. On the other hand, the delay circuit 22 delays the conduction signal from the oscillator 2l by a predetermined time, and then makes the switch means 15b conductive.
The high voltage charged in the charging/discharging capacitor 14b is applied to the discharge tube 11. As a result, the charging voltage of the charging/discharging capacitor 14a is applied to the discharge tube 1l at time 70 to generate gas discharge, and the charging voltage of the charging/discharging capacitor 14b is applied after a delay of a predetermined time from time t0. be done. The currents Ia and Ib flowing through the switch means 15a and 15bL:v due to the conduction are determined by the impedances of the charging and discharging capacitors 14a and 14b, the reactors 16a and 16b, and the discharge tube 11, and have a waveform as shown in FIG. becomes. In the copper vapor laser device, lower level atoms are relaxed to the ground level by superelastic collisions between the lower level and slow electrons when the diameter of the inner tube 2 is large. That is, C u * + e ilawl- C u + e
(ras) Here, Cu* is a lower level atom Cu is a ground level atom e jml. 1 is a slow electron ear and Hatatomi tl is a fast electron. The voltage applied from the second pulse generation circuit 13b is Although the voltage is low and does not excite the atoms to the upper level, the electrons are accelerated and collisions between the electrons and the copper atoms become more intense.As a result, superelastic collisions between the lower level atoms and electrons become active. Therefore, the relaxation of the lower level is promoted. Note that the inductance value of the interference prevention reactors 20a and 20b is selected so as to have a large impedance with respect to the frequency component of the current flowing when the switching means 15a and 15b are turned on. For example, in general, in the case of a copper vapor laser device, the current flowing through the discharge tube l1 has a maximum pulse width of 500μ88C, so the fundamental frequency is approximately IMHz.The interference prevention reactors 20a and 20b are sufficiently In order to have a large impedance, if the inductance of the interference prevention reactors 20a and 20b is Lz, then 2ifLz》Zr Zr needs the impedance of the discharge tube 1l. Usually, the impedance ZT is from several ohms to several tens of ohms. , for example, 50Ω, then the inductance Lz should be selected to be greater than HiooμH.By selecting the inductance Lz as described above, for example, when the switch means 15a and 15b are turned on, the charging and discharging capacitors 14a and 14b are discharged. No current starts to flow. [Effects of the Invention] As described above, according to the present invention, the second pulse generation circuit is provided separately from the first pulse generation circuit, and the first pulse generation circuit is connected to the discharge tube. After the lth pulse voltage is applied from
Since the second pulse voltage is applied to the discharge tube again from the second pulse generation circuit after a predetermined time delay, the time for the lower level atoms to relax to the ground level is shortened.
As a result, the population inversion becomes more complete when the next pulse is applied from the l-th pulse generation circuit, which has the effect of making it possible to obtain a highly efficient metal vapor laser device even at high repetition rates. In addition, since the switching means of the first pulse generation circuit and the -second pulse generation circuit are constructed by connecting a large number of solid state switching elements in series and parallel, the response speed is fast, and the switching means of the first pulse generation circuit and the -second pulse generation circuit are constructed by connecting a large number of solid state switching elements in series and parallel. Switching time does not change depending on usage conditions such as anode delay time, resulting in high reliability and long life.

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

第1図はこの発明の一実施例による金属蒸気レーザ装置
の回路図、第2図はスイッチ手段の構成図、第3図は上
記実施例の動作を説明するタイムチャート図、第4図は
従来の金R蒸気レーザ装置の回路図である。 1lは放電管、13aはの第1のパルス発生回路、13
bは第2のパルス発生回路、15a,15bはスイッチ
手段、1.7a,17bは高圧電源、21は発振器、2
2は遅延回路。 なお、図中、同一符号は同一または相当部分を示す。
Fig. 1 is a circuit diagram of a metal vapor laser device according to an embodiment of the present invention, Fig. 2 is a configuration diagram of a switch means, Fig. 3 is a time chart diagram explaining the operation of the above embodiment, and Fig. 4 is a conventional one. FIG. 2 is a circuit diagram of the gold R vapor laser device of FIG. 1l is a discharge tube, 13a is a first pulse generating circuit, 13
b is a second pulse generation circuit; 15a and 15b are switch means; 1.7a and 17b are high-voltage power supplies; 21 is an oscillator;
2 is a delay circuit. In addition, in the figures, the same reference numerals indicate the same or corresponding parts.

Claims (1)

【特許請求の範囲】[Claims]  ガス放電によって金属を加熱、気化させてレーザ出力
を得る放電管と、多数の固体スイッチング素子を直並列
接続して構成したスイッチ手段を充放電コンデンサに接
続し、このスイッチ手段の開閉によって、前記放電管に
ガス放電を発生させる第1のパルス電圧を供給する第1
のパルス発生回路と、前記スイッチ手段と同一構成のス
イッチ手段を充放電コンデンサに接続し、このスイッチ
手段の開閉によって前記放電管に第2のパルス電圧を供
給する第2のパルス発生回路と、前記第1のパルス発生
回路のスイッチ手段に導通信号を供給する発振器と、前
記導通信号を所定時間遅延して前記第2のパルス発生回
路のスイッチ手段に導通信号を供給する遅延回路と、前
記第1のパルス発生回路および前記第2のパルス発生回
路のそれぞれの充放電コンデンサに干渉防止リアクトル
を介して給電する別個独立に設けられた第1の電源およ
び第2の電源とを備えた金属蒸気レーザ装置。
A discharge tube that heats and vaporizes metal by gas discharge to obtain a laser output, and a switch means configured by connecting a large number of solid state switching elements in series and parallel are connected to a charge/discharge capacitor, and by opening and closing the switch means, the discharge a first supplying a first pulsed voltage that produces a gas discharge in the tube;
a second pulse generating circuit which connects a switch means having the same configuration as the switch means to a charging/discharging capacitor and supplies a second pulse voltage to the discharge tube by opening and closing the switch means; an oscillator that supplies a conduction signal to the switch means of the first pulse generation circuit; a delay circuit that delays the conduction signal by a predetermined time and supplies the conduction signal to the switch means of the second pulse generation circuit; A metal vapor laser device comprising a first power source and a second power source that are independently provided to supply power to each of the charging and discharging capacitors of the pulse generating circuit and the second pulse generating circuit via an interference prevention reactor. .
JP15193089A 1989-06-14 1989-06-14 Metal vapor laser device Pending JPH0318073A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP15193089A JPH0318073A (en) 1989-06-14 1989-06-14 Metal vapor laser device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP15193089A JPH0318073A (en) 1989-06-14 1989-06-14 Metal vapor laser device

Publications (1)

Publication Number Publication Date
JPH0318073A true JPH0318073A (en) 1991-01-25

Family

ID=15529309

Family Applications (1)

Application Number Title Priority Date Filing Date
JP15193089A Pending JPH0318073A (en) 1989-06-14 1989-06-14 Metal vapor laser device

Country Status (1)

Country Link
JP (1) JPH0318073A (en)

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