JPS5848485A - Pulse laser oscillator - Google Patents

Pulse laser oscillator

Info

Publication number
JPS5848485A
JPS5848485A JP14568081A JP14568081A JPS5848485A JP S5848485 A JPS5848485 A JP S5848485A JP 14568081 A JP14568081 A JP 14568081A JP 14568081 A JP14568081 A JP 14568081A JP S5848485 A JPS5848485 A JP S5848485A
Authority
JP
Japan
Prior art keywords
discharge
cathode
electrode
anode
dielectric
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
Application number
JP14568081A
Other languages
Japanese (ja)
Other versions
JPS6342425B2 (en
Inventor
Yukio Sato
行雄 佐藤
Masaaki Tanaka
正明 田中
Masao Hishii
菱井 正夫
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 JP14568081A priority Critical patent/JPS5848485A/en
Publication of JPS5848485A publication Critical patent/JPS5848485A/en
Publication of JPS6342425B2 publication Critical patent/JPS6342425B2/ja
Granted 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
    • H01S3/0971Processes or apparatus for excitation, e.g. pumping by gas discharge of a gas laser transversely excited
    • H01S3/09713Processes or apparatus for excitation, e.g. pumping by gas discharge of a gas laser transversely excited with auxiliary ionisation, e.g. double discharge 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 elongate life of electrodes, to simplify a triggering structure, and to prevent the contamination of laser gas due to abraded material of the electrode, by arranging a dielectric electrode covered by a dielectric between a cathode and anode, and by steadily generating an AC discharge as an auxiliary discharge, e.g. silent discharge, between the cathode and anode or between either electrode and the auxiliary electrode. CONSTITUTION:The AC discharge is generated between the cathode 17 and the feeding line 19 and between the anode 1 and the feeding line 19 by the application of a voltage from an AC high voltage power source 21. Said AC discharge has inherent homogenity owing to the presence of the dielectric electrode 18. A low ionized state is steadily yielded in the vicinity of the cathode 17 and over the entire main discharge space. When a main discharge trigger switch 9 is made to be conducting state under the presence of the auxiliary discharge, the charge stored in a main discharge capacity 10 quickly flows between the cathode 17 and the anode 1, and the uniform pulse discharge is obtained over the entire electrode region.

Description

【発明の詳細な説明】 この発明は横方向励起型パルスレーザ発根器に関するも
のである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a laterally pumped pulsed laser generator.

第1図は従来この槌のものとして代表的な光軸放電、ガ
ス流の各方向が互1/a [l’iぼ直交するいわゆる
三軸直交型の■2レーザ発振器の要部構成を示す縦断面
図、第2図は第1図1−flよりみた横断面図で、山は
平板11!極、(2;はメックエ!極、C3)は紫外光
発光用スパークボード、14)は放電安定化抵抗、(5
1は紫外光発光用ギャップスイッチ、(6)は紫外光発
光用コンデンサー、(7)は充電抵抗、18)は充電用
直流高圧電源(9)は主放゛成用ギヤップスイップスイ
ッチ、uCは主放電用コ/デンサー、tinは遅延パル
ス発生装置、■はトリガー発生装置、a3.は放電防起
部、 aatiν−ザガス、usは全反射鏡、 ueF
i部分反射鏡、@はレーザ光軸である。+11&L山と
陰[i 121との間に、  Cot。
Figure 1 shows the main part configuration of a so-called three-axis orthogonal type ■2 laser oscillator, which is a typical example of this hammer's conventional laser oscillator, in which the optical axis discharge and gas flow directions are approximately 1/a [l'i] orthogonal to each other. The vertical cross-sectional view and FIG. 2 are cross-sectional views taken from FIG. 1 1-fl, and the peak is the flat plate 11! pole, (2; is MECUE! pole, C3) is a spark board for ultraviolet light emission, 14) is a discharge stabilizing resistor, (5
1 is a gap switch for ultraviolet light emission, (6) is a capacitor for ultraviolet light emission, (7) is a charging resistor, 18) is a DC high-voltage power supply for charging, (9) is a gap switch for main radiation generation, and uC is a gap switch for generating main radiation. Main discharge co/capacitor, tin is a delay pulse generator, ■ is a trigger generator, a3. is the discharge prevention part, aatiν-zagas, us is the total reflection mirror, ueF
i partial reflecting mirror, @ is the laser optical axis. +11&L between Mt. and Yin [i 121, Cot.

N2. H@からなるレーザガスα41矢印の方向に流
しておく、直流高圧電源(8)によって、紫外光発光用
コンデンサー(6)、および主放電用コンデンサー(I
I?充電しておく、遅延パルス発生装置Qll i O
Nにすると、tず紫外光発光用ギャップスイッチ(5)
が導通状態になり、紫外光発光用コンデンサー(6)に
蓄えられた電荷が一気にスパークボード13)に流れる
。大電流密度スパーク放電の発生により、スパークボー
ドが紫外光の発光体となり陰極(2)の近傍、ならびに
放電励起部α3の全域に渡り、混合ガスが弱電離状W1
(電子密度@@=lQ@〜108−/ll3)となる。
N2. The ultraviolet light emission condenser (6) and the main discharge condenser (I
I? Charged delayed pulse generator Qll i O
When set to N, the gap switch for ultraviolet light emission (5)
becomes conductive, and the charges stored in the ultraviolet light emission capacitor (6) flow all at once to the spark board 13). Due to the generation of a high current density spark discharge, the spark board becomes an emitter of ultraviolet light, and the mixed gas becomes weakly ionized W1 near the cathode (2) and throughout the discharge excitation part α3.
(Electron density @@=lQ@~108-/ll3).

紫外光発光用ギャップスイッチ(5)にトリガーパルス
が送られた後、数百5sec〜数s*ec して、遅延
パルス発生装置1111+が第二のパルスを発−生じて
、主放電用ギャップスイッチ(9)が導通状態となり、
主放電用コンダン−7−(IIに蓄えられた電荷が一気
に陰極(2)。
After the trigger pulse is sent to the ultraviolet light emission gap switch (5), several hundred 5 seconds to several seconds*ec, the delayed pulse generator 1111+ generates a second pulse, and the main discharge gap switch is activated. (9) becomes conductive,
The charge stored in the main discharge conductor 7-(II) is immediately transferred to the cathode (2).

陽極−ILrlaK流れ、パルス放電が形成される。Anode-ILrlaK flows and a pulsed discharge is formed.

このパルス放電は、あらかじめ放電空間が紫外光によっ
て均一な弱電離状−にされているため。
This pulse discharge occurs because the discharge space is made uniformly weakly ionized by ultraviolet light in advance.

均一な°放電となる。This results in uniform ° discharge.

この放電により形成された放電励起部a3には。In the discharge excitation part a3 formed by this discharge.

板 混合ガス141中の特定の励動準位間に反転分布が形成
される。放電励起部Q3を挾み対向配置し友全反射鏡a
Sと部分反射鏡1151と部分反射鏡(9)からレープ
ビームが出射する。
Population inversion is formed between specific excited levels in the plate mixed gas 141. Total reflection mirrors a are arranged opposite to each other with the discharge excitation part Q3 in between.
A lep beam is emitted from S, the partial reflecting mirror 1151, and the partial reflecting mirror (9).

ところで、この柿のレーザでに、単位有効放電体積当り
のレーザ出力全増加させるために。
By the way, in order to increase the total laser output per unit effective discharge volume with this persimmon laser.

lat、s (大気圧J 以上の圧力で動作させるのが
一般的であるが、圧力全増加するにつれソ、均一に放電
を行なうのが困難となり先にボしたように、紫外光等?
用い、予め放電空間全体を弱電離状態にしておくことが
必!条件となる。紫外光発光のための電極構造にはさま
ざまな形態のものが考案され、先に示し友スパークボー
ドタイプは一例にすぎな、い。しかし、iずれの形態に
お−でも、大電流密度スパーク放電全同時に多数の力所
で行なう形a會有して−る。また。
(It is common to operate at a pressure higher than atmospheric pressure J, but as the total pressure increases, it becomes difficult to discharge uniformly. As mentioned earlier, ultraviolet light, etc.)
It is necessary to make the entire discharge space into a weakly ionized state beforehand! It is a condition. Various types of electrode structures for emitting ultraviolet light have been devised, and the friend sparkboard type shown above is just one example. However, even in the case of the offset configuration, there is a configuration in which high current density spark discharges are carried out simultaneously at a large number of force points. Also.

この樵のパルスレーザを工業的に用匹る場会。This is a place where this woodcutter's pulsed laser will be used industrially.

数ffHyからi千HFでパルλ発娠させることが必要
で、いわゆる高速繰り返し機能が必要であ′   ”・
・1′す る。
It is necessary to generate a pulse λ in several ffHy to i,000HF, and a so-called high-speed repetition function is required.
・Do 1'.

しかしながら、従来のものの上記構成では。However, in the above-mentioned configuration of the conventional one.

老)  紫外光発光のために大電流密度スパーク放電が
行なわれて−るが、この放電形態では電極の摩耗が激し
く、高速繰り返し一ヲ行なうと、紫外光発光用電極の寿
命が著しく短くなる。′ (ロ)紫外光発光用電極の摩耗物質がレーザガスに混入
し、ガスを劣化させる九めレーザガスの゛封じ切り運転
が困難なものとなる。
(2) High current density spark discharge is used to emit ultraviolet light, but this type of discharge causes severe wear on the electrodes, and if the discharge is repeated at high speed, the life of the electrodes for emitting ultraviolet light will be significantly shortened. (b) Abrasion substances from the ultraviolet light emitting electrode mix into the laser gas, which deteriorates the gas.Ninth, it becomes difficult to operate the laser gas in a sealed state.

tfi  レーザの放電断面積管゛増加させるVCはメ
ッシユの1lII極; または陽極を用い、この背面か
ら放電空間全域にわたって紫外光を当てるのが有効で−
あるが、メツ゛シェの陰極、または陽極では熱容量が小
さいうえ屹水冷却が困難なため、高速繰り返し動作にお
いてはその摩” 耗が激しく適当で雇い。
To increase the discharge cross-sectional area of the tfi laser, the VC is a mesh electrode; or it is effective to use an anode and apply ultraviolet light to the entire discharge space from the back side.
However, the cathode or anode of meshwork has a small heat capacity and is difficult to cool with water, so during high-speed repetitive operations, the wear is severe and unsuitable.

に)均一な紫外光予備電離1行なうために、紫外光の発
光が行述゛われて痴ら、主放電の印加ま・でに、数百5
sec〜数s協ecの遅延時間が必要であるが、その゛
ために遅延パルス発生装置等が必要となり、そのトリガ
ー機構が複雑となる。等の欠点がある。
(2) In order to perform uniform ultraviolet light pre-ionization, ultraviolet light emission was performed, and several hundred
A delay time of several seconds to several seconds is required, which requires a delay pulse generator and the like, making the trigger mechanism complicated. There are drawbacks such as.

この発明は、上記のような、従来のものの欠点を除去し
ようとするもので、陰極と陽極の間に誘電体で被檄した
誘電体電極を配役し、これと陰、陽各極またはそれら0
匹ずれか一極との一間に補助放電としての交流放電9例
えば無声放電を定常的に□生成させるようにしたもので
ある。
This invention attempts to eliminate the above-mentioned drawbacks of the conventional ones, and uses a dielectric electrode covered with a dielectric between the cathode and the anode, and connects this to the cathode, anode, or both.
An alternating current discharge 9, for example, a silent discharge, is constantly generated as an auxiliary discharge between one pole and the other.

第3因はこG発明の一実施例の縦断面図、第4因は第3
図ff−ff線よりみた横断面図で、αηは平板陰砺、
α8σノくイレックλなどの耐熱性絶縁物のパイプ状の
誘電体電極、[ISは誘電体電極a〜に電流を供給する
給電線9頭は誘電体電極08F3を流れる冷却水:ば1
1は給電IWII■と陰極Uη、陽極(1;との間に予
備電離放電としての交流(100H)1〜100KHy
)放電を生成させる几めの交流高圧電源である。   
′ 上記実施例において框、交流高圧電源11!Dの電圧の
印加により、陰極αηと給電線α3どの間、および陽極
11:と給電+1i1ullとの間に交流放電が生じる
。この交流放電は、n電体電゛極(181の存在により
本質的に均質性を有し、陰極面の近傍運びに主放電空間
全域に渡り、定常的忙均−な低電離状態が実現する。こ
の時の電離層は、交流高圧電源の1から供給される電力
によって異なるが。
The third factor is a vertical sectional view of an embodiment of the G invention, and the fourth factor is the third factor.
In the cross-sectional view taken from the line ff-ff, αη is a flat plate shade;
Pipe-shaped dielectric electrodes made of heat-resistant insulators such as α8σ and IREC λ;
1 is an alternating current (100H) 1 to 100KHy as a preliminary ionization discharge between the power supply IWII■, the cathode Uη, and the anode (1;
) It is a sophisticated AC high-voltage power supply that generates electrical discharge.
' In the above embodiment, the stile, AC high voltage power supply 11! By applying the voltage D, alternating current discharge occurs between the cathode αη and the power supply line α3 and between the anode 11: and the power supply +1i1ull. This alternating current discharge has essentially homogeneity due to the presence of the n-electrode (181), and a steady, even, and low ionization state is realized throughout the main discharge space near the cathode surface. The ionosphere at this time differs depending on the power supplied from AC high voltage power supply 1.

紫外光源による電離と同様10”シ4−程度の電離層に
容易に得ることができる。このような補助放電の存在下
で、主放電用トリガースイッチ(9)全導通状態にする
と、主放電用コンデンサー[相]に蓄えられた電荷が一
気に陰極[171,陽極(1)間に流れ、電極全域に渡
り均一なパルス放電が得られる。
Similar to ionization by an ultraviolet light source, an ionosphere of about 10" can be easily obtained. In the presence of such an auxiliary discharge, when the main discharge trigger switch (9) is made fully conductive, the main discharge capacitor The charges stored in the [phase] flow at once between the cathode [171] and the anode (1), and a uniform pulse discharge is obtained over the entire electrode area.

ここで、従来の紫外光子備電JIII/c比べて、陰#
tjメッシ為陰極12)に換って平板陰極αりを用iて
−るため、摩耗することはなく、また背面冷却も可能と
なるので、寿命問題はなくなる。予備放電用電極につい
ても、$!誘電体電極用−てするため、その寿命は半永
久的となる。また電極の摩耗がなめために、ν−ザガス
が汚されることはなく、長時間にわたる封じ切゛り動作
が可能となる。更に交流放電は定常的に行なわれている
几め、予備電離放電と主放電の遅れ時間を考慮する必要
がなく、トリガー機構が簡略化され、特に高速繰り返し
に向く。
Here, compared to the conventional ultraviolet photon power supply JIII/c,
Since a flat plate cathode is used in place of the TJ mesh cathode 12), there is no wear and tear, and back cooling is also possible, so there is no longer a problem with life. As for the pre-discharge electrode, $! Since it is used for dielectric electrodes, its lifespan is semi-permanent. In addition, the ν-zagas is not contaminated due to wear of the electrodes, and the sealing operation can be performed for a long time. Furthermore, AC discharge does not require consideration of delay times between pre-ionization discharge and main discharge, which are regularly performed, and the trigger mechanism is simplified, making it particularly suitable for high-speed repetition.

放電領域を拡大したい場合は、放電断面に沿って、誘電
体電極の道にる数を増やせばよ暦わけで、その意味で自
由度が大きい。
If you want to expand the discharge area, you just need to increase the number of dielectric electrodes along the discharge cross section, and in that sense you have a lot of freedom.

上記実施例におhてけ、陰極側の近傍[6電体電極Q8
1配設した場合を示したが、*極印の近傍に配設しても
同様の効果が得られる。
In the above embodiment, near the cathode side [6 electric body electrode Q8
Although the case where one is arranged is shown, the same effect can be obtained even if it is arranged near the * pole mark.

第5自はこの発明の他の実施例の平面面で誘電体電極(
1g+ i光軸のと直交する方向に運べた場合の、陰極
部分のみを示した平面図、第6図はその側面図で、レー
ザの放電長が長く、光軸方向に沿って長い誘電体電極を
設置できなiとき。
The fifth element is a dielectric electrode (
1g+i A plan view showing only the cathode part when it is carried in a direction perpendicular to the optical axis, and Fig. 6 is a side view of the cathode.The laser discharge length is long and the dielectric electrode is long along the optical axis direction. When I can't install the.

この構成が有効である。This configuration is valid.

また、第7図は更に他の実施例の平面図で誘電体電極と
して、多くの穴を有する金属板に。
Moreover, FIG. 7 is a plan view of still another embodiment, in which a metal plate with many holes is used as a dielectric electrode.

ガラスライニングを施したものを用いた陰極部分のみ含
水した平面図、第8図はその側面図で。
A plan view of a glass-lined cathode in which only the cathode part is hydrated, and Figure 8 is a side view.

(至)は数多くの透孔129ヲ有し、交流高電圧が印加
される金属平板、@は金属平板を包むO電体で。
(To) is a flat metal plate with many through holes 129 and to which high AC voltage is applied, and @ is an O electric body that wraps around the flat metal plate.

先に示した誘電体電極a8と同様の!l!能を待つ。Similar to the dielectric electrode a8 shown above! l! Waiting for Noh.

この発明はレーザガスの気流を挾んで相対向するように
配設されパルス状の直流高電圧が印加されてグロー放電
を生成するlI[!と陰極、および上記レーザガス気流
中に配設され常に交流高電圧が印加されて上記1118
および陰極との間で無声放電を生成する酔電電#を備、
tたもの÷。
This invention is arranged to face each other across the airflow of laser gas, and a pulsed DC high voltage is applied to generate a glow discharge. and a cathode, and the above 1118 is disposed in the laser gas flow and is constantly applied with an AC high voltage.
Equipped with a saidenden # that generates silent discharge between it and the cathode,
t things ÷.

電極寿命を延ばし、トリガー機構を簡略化し。Extends electrode life and simplifies trigger mechanism.

さらには電極の摩耗物によるレーザガスの汚れを防ぎ、
レーザ・ガスの封じ切りが可能となる。
Furthermore, it prevents contamination of the laser gas due to abrasions on the electrodes.
It becomes possible to seal off the laser gas.

これKより、工業的応用において重要である数百〜数I
Q(y高速繰り返し状態における連続運転が可能となり
、装置の高性能化を図ることができる。
From this K, several hundred to several I, which is important in industrial applications,
Q(y) Continuous operation in a high-speed repetition state is possible, and the performance of the device can be improved.

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

第1図は従来のパルスレーザ発振器の縦断面図、第2■
tit第1■l−11よりみた横断面図。 wEa図はこの発明の一実施例の縦#r面図、第4図は
第3■IV−IV線よりみた横断面一、第5崗はこの発
明の他の実施例の要部拡大平INF図、II6因はその
酋面図、第7図げこの発明の他の実施例の要部拡大平面
図、第8図はその側面図である。 図において、+1)は平面陽極、12)はメ、シ、。 (4)は放電安定化抵抗、(8)は充電用直流高圧電源
。 (9)は主放電用ギャップスイッチ、叫は主放電用コン
デンサー、 (121にトリガー発生装置、a3は放電
励起部、a#はレーザガス、 Q51は全反射z、 (
1G+は部分反射鏡、a71Fi平板陰極、 QB+は
誘電体′c&極。 a9は給電線、■は冷却水、aは交流高圧電源。 @は光軸、のは金属平板、(至)は誘電体、伺は透孔で
ある。 なお、因中同−符号はそれぞれ同一または相当部分を示
す。 代理人 葛野信−(外1名) 李 3 ぬ rvl ! ■−
Figure 1 is a longitudinal cross-sectional view of a conventional pulsed laser oscillator, and Figure 2
FIG. 1 is a cross-sectional view seen from 1-11. Figure wEa is a vertical #r view of one embodiment of this invention, Figure 4 is a cross-sectional view taken from line 3 IV-IV, and Figure 5 is an enlarged plane INF of main parts of another embodiment of this invention. FIG. 7 is an enlarged plan view of a main part of another embodiment of the present invention, and FIG. 8 is a side view thereof. In the figure, +1) is a flat anode, 12) is a flat anode, and 12) is a flat anode. (4) is a discharge stabilizing resistor, and (8) is a DC high-voltage power supply for charging. (9) is the main discharge gap switch, (121 is the trigger generator, a3 is the discharge excitation part, a# is the laser gas, Q51 is the total reflection z, (
1G+ is a partial reflecting mirror, a71Fi flat plate cathode, and QB+ is a dielectric 'c& pole. a9 is the power supply line, ■ is the cooling water, and a is the AC high voltage power supply. @ is the optical axis, is the metal flat plate, (to) is the dielectric, and the opening is the through hole. It should be noted that the same reference numerals in the figures indicate the same or corresponding parts. Agent Shin Kuzuno (1 other person) Lee 3 Nurvl! ■−

Claims (1)

【特許請求の範囲】 II+  レーザガスの気流を挾んで相対向するように
配設されパルス状の直流高電圧が印加されてグロー放電
を生成する陽極と陰極、および上記レーザガス気流中に
配設され常に交流高電圧が印加されて上記陽極および陰
極との間で無声放電を生成する銹電体電4ilt−備え
たパルスレーザ発振器。 (2)棒状に形成されたI電体電極が陽II#または陰
極の放電面を援うよ5うにレーザ光軸方向また社交軸と
交鎖する方向に複数本配列されてiる構成とした特許請
求の範囲第1項記戦のパルスレーず発振器。 131 −電体電極が複数の透孔が形成されて−る平板
状に形成されたものである特許請求の範囲第1項記戦の
パルスレーザ発振器。
[Scope of Claims] II+ An anode and a cathode that are arranged to face each other across the laser gas airflow and to which a pulsed DC high voltage is applied to generate a glow discharge; A pulsed laser oscillator equipped with a 4ilt-electronic body to which an AC high voltage is applied to generate a silent discharge between the anode and the cathode. (2) A plurality of rod-shaped I electric body electrodes are arranged in the direction of the laser optical axis or in the direction intersecting with the social axis so as to support the discharge surface of the positive II# or cathode. A pulse laser oscillator according to claim 1. 131 - The pulsed laser oscillator according to claim 1, wherein the electric electrode is formed into a flat plate shape with a plurality of through holes formed therein.
JP14568081A 1981-09-16 1981-09-16 Pulse laser oscillator Granted JPS5848485A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP14568081A JPS5848485A (en) 1981-09-16 1981-09-16 Pulse laser oscillator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP14568081A JPS5848485A (en) 1981-09-16 1981-09-16 Pulse laser oscillator

Publications (2)

Publication Number Publication Date
JPS5848485A true JPS5848485A (en) 1983-03-22
JPS6342425B2 JPS6342425B2 (en) 1988-08-23

Family

ID=15390599

Family Applications (1)

Application Number Title Priority Date Filing Date
JP14568081A Granted JPS5848485A (en) 1981-09-16 1981-09-16 Pulse laser oscillator

Country Status (1)

Country Link
JP (1) JPS5848485A (en)

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6190486A (en) * 1984-10-09 1986-05-08 Mitsubishi Electric Corp Short pulse laser device of discharge excitation type
JPS61104683A (en) * 1984-10-29 1986-05-22 Toshiba Corp Gas laser oscillation device
JPS61116888A (en) * 1984-11-12 1986-06-04 Mitsubishi Electric Corp Discharge excitation short pulse laser device
JPS61137380A (en) * 1984-12-10 1986-06-25 Toshiba Corp Lateral-excited gas laser oscillator
JPS61188982A (en) * 1985-02-18 1986-08-22 Mitsubishi Electric Corp Discharge excitation type short pulse laser device
JPH0220362U (en) * 1988-07-27 1990-02-09
US5205888A (en) * 1990-07-03 1993-04-27 Mitsubishi Gas Chemical Company, Inc. Process for producing carbon fiber reinforced carbon materials

Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5010090A (en) * 1973-05-23 1975-02-01
JPS5241039A (en) * 1975-09-24 1977-03-30 Tmc Corp Heel piece
JPS5340878A (en) * 1976-09-27 1978-04-13 Yazaki Corp Wiring head
JPS5424591A (en) * 1977-07-26 1979-02-23 Mitsubishi Electric Corp Gas laser unit
JPS54118792A (en) * 1978-03-08 1979-09-14 Komatsu Mfg Co Ltd Method of modulating output of laser
JPS5570085A (en) * 1978-11-03 1980-05-27 Voest Ag Pneumatic gas laser laterally electrically excited by pulse *tea laser*
JPS5680190A (en) * 1979-12-05 1981-07-01 Mitsubishi Electric Corp Gas laser device

Patent Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5010090A (en) * 1973-05-23 1975-02-01
JPS5241039A (en) * 1975-09-24 1977-03-30 Tmc Corp Heel piece
JPS5340878A (en) * 1976-09-27 1978-04-13 Yazaki Corp Wiring head
JPS5424591A (en) * 1977-07-26 1979-02-23 Mitsubishi Electric Corp Gas laser unit
JPS54118792A (en) * 1978-03-08 1979-09-14 Komatsu Mfg Co Ltd Method of modulating output of laser
JPS5570085A (en) * 1978-11-03 1980-05-27 Voest Ag Pneumatic gas laser laterally electrically excited by pulse *tea laser*
JPS5680190A (en) * 1979-12-05 1981-07-01 Mitsubishi Electric Corp Gas laser device

Cited By (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6190486A (en) * 1984-10-09 1986-05-08 Mitsubishi Electric Corp Short pulse laser device of discharge excitation type
JPH0344429B2 (en) * 1984-10-09 1991-07-05 Mitsubishi Electric Corp
JPS61104683A (en) * 1984-10-29 1986-05-22 Toshiba Corp Gas laser oscillation device
JPH0329316B2 (en) * 1984-10-29 1991-04-23 Tokyo Shibaura Electric Co
JPS61116888A (en) * 1984-11-12 1986-06-04 Mitsubishi Electric Corp Discharge excitation short pulse laser device
JPH0464477B2 (en) * 1984-11-12 1992-10-15 Mitsubishi Electric Corp
JPS61137380A (en) * 1984-12-10 1986-06-25 Toshiba Corp Lateral-excited gas laser oscillator
JPH0337318B2 (en) * 1984-12-10 1991-06-05 Tokyo Shibaura Electric Co
JPS61188982A (en) * 1985-02-18 1986-08-22 Mitsubishi Electric Corp Discharge excitation type short pulse laser device
JPH0220362U (en) * 1988-07-27 1990-02-09
US5205888A (en) * 1990-07-03 1993-04-27 Mitsubishi Gas Chemical Company, Inc. Process for producing carbon fiber reinforced carbon materials

Also Published As

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