JPS62101093A - Metal vapor laser apparatus - Google Patents

Metal vapor laser apparatus

Info

Publication number
JPS62101093A
JPS62101093A JP23948485A JP23948485A JPS62101093A JP S62101093 A JPS62101093 A JP S62101093A JP 23948485 A JP23948485 A JP 23948485A JP 23948485 A JP23948485 A JP 23948485A JP S62101093 A JPS62101093 A JP S62101093A
Authority
JP
Japan
Prior art keywords
tube
discharge
inner tube
metal vapor
ceramic
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
JP23948485A
Other languages
Japanese (ja)
Inventor
Hironobu Kimura
博信 木村
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.)
Toshiba Corp
Original Assignee
Toshiba 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 Toshiba Corp filed Critical Toshiba Corp
Priority to JP23948485A priority Critical patent/JPS62101093A/en
Publication of JPS62101093A publication Critical patent/JPS62101093A/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 obtain a long-life metal vapor laser apparatus which provides high output steadily by composing a discharge tube of a multilayer tube. CONSTITUTION:The discharge tube 20 of a metal vapor laser apparatus is composed of a ceramic inner tube 20A, a ceramic intermediate tube 20B and a high melting pint metal outer tube 20C. When discharge is induced in the discharge part 2 in the inner tube 20A, discharge plasma is induced inside auxiliary electrodes 21a and 21b. As the inner tube 20A is supported by ceramic spacers 22 only, the temperature distribution in the tube is nearly uniform. Gas gaps 5A and 6A are provided between the outside circumferences of the tip parts of anodes 5 and 6 and the inside circumference of the intermediate tube 20B so that even if the tubes are heated to the high temperature, the two open ends of the intermediate tube 20B are not influenced by the heat. As the outer tube 20C is closely contacted with the outside of the intermediate tube 20B, the temperature in the intermediate tube 20B can be kept uniform in the portion corresponding to the length of the outer tube 20C. With this constitution, the output can be elevated significantly.

Description

【発明の詳細な説明】 〔発明の技術分野〕 本発明は金属蒸気をレーtア媒質とする金属蒸気レーデ
装置に係り、特に、金属粒子を内蔵りる族Ti管を改良
した金属蒸気レーザ装置に関する。
[Detailed Description of the Invention] [Technical Field of the Invention] The present invention relates to a metal vapor laser device using metal vapor as a laser medium, and particularly to a metal vapor laser device that is an improved group Ti tube containing metal particles. Regarding.

〔発明の技術的背景〕[Technical background of the invention]

従来、この種の金属蒸気レーザ装置は、第3図に示すよ
うに構成され、耐熱性に涜れたセラミック管1を放電管
に構成している。
Conventionally, this type of metal vapor laser device is constructed as shown in FIG. 3, and the discharge tube is a ceramic tube 1 with poor heat resistance.

セラミック管1はその内部の放電部2にガス供給系3か
らHC!、Ne等の71り市川バッファガスが供給され
ると共に、ロータリポンプ4により排気され、陽極5と
陰極6とを両端部に対向配置している。
The ceramic tube 1 receives HC! from the gas supply system 3 to the discharge section 2 inside it. , Ne, and the like are supplied and exhausted by a rotary pump 4, and an anode 5 and a cathode 6 are disposed facing each other at both ends.

陽極5と陰極6との間にはパルス高電圧電源7からのパ
ルス高電圧が印加され、パルス2極放′1゛uを行なっ
て放電プラズマを発生する。このパルス高電圧は電圧が
数kV〜10数kV、繰返し周波数が数k t−I z
 〜10数k l−I zである。
A pulsed high voltage from a pulsed high voltage power source 7 is applied between the anode 5 and the cathode 6, and a pulsed bipolar discharge '1'u is performed to generate discharge plasma. This pulsed high voltage has a voltage of several kV to several tens of kV, and a repetition frequency of several kilovolts.
~10 k l - I z.

セラミック管1内には複数の金属粒子8が配置dされ、
この金属粒子8が放電プラズマと接触してけラミック管
1が非富な高温状態に1111熱されて金属粒子8が蒸
発することにより、レーザ媒質となる金属蒸気が生成さ
れる。
A plurality of metal particles 8 are arranged in the ceramic tube 1,
When the metal particles 8 come into contact with the discharge plasma, the lamic tube 1 is heated to an extremely high temperature 1111 and the metal particles 8 evaporate, thereby generating metal vapor which becomes the laser medium.

金属蒸気はセラミック管1内に1014〜1016n 
/ cdの密度で一様に分布し、放電プラズマ中の自由
電子により励起されることによって、イの金属特有の波
長の光を発光し、この光が外囲8為であるケーシング9
の窓9aを通して、セラミック管1の両側に置かれた出
力ミラー10と全反射ミラー11とで構成される光共振
器を往復する間に増幅され、出力ミラー10側よりレー
ザ光となって出力される。
The metal vapor is 1014 to 1016n in the ceramic tube 1.
The casing 9 is uniformly distributed with a density of / cd, and when excited by the free electrons in the discharge plasma, emits light with a wavelength specific to the metal of A, and this light is emitted by the outer shell 9.
Through the window 9a, the laser beam is amplified while reciprocating through an optical resonator consisting of an output mirror 10 and a total reflection mirror 11 placed on both sides of the ceramic tube 1, and is output as a laser beam from the output mirror 10 side. Ru.

なお、しラミック管1の外周には、タングステン、タン
タルJ3よびモリブデン等高融点金属の複数の遮蔽板1
2を同軸状に積層さけて収容する真空断熱室13が配設
され、セラミック管1の保温を図っている。真空断熱室
13はベローズ14を介して伸縮自在に接続されたセラ
ミック管1により気密にシールされ、この室内排気はロ
ータリポンプ15により行なわれる。
In addition, on the outer periphery of the lamic tube 1, a plurality of shielding plates 1 made of high melting point metals such as tungsten, tantalum J3, and molybdenum are provided.
A vacuum insulation chamber 13 is provided to house the ceramic tubes 1 while coaxially stacking them to keep the ceramic tubes 1 warm. The vacuum insulation chamber 13 is hermetically sealed by a ceramic tube 1 which is telescopically connected via a bellows 14, and the room is evacuated by a rotary pump 15.

また、第3図中、符号16はケーシング9の外周に巻回
されてこれを冷却するための水冷7JI配管である。
Further, in FIG. 3, reference numeral 16 is a water-cooled 7JI pipe that is wound around the outer periphery of the casing 9 to cool it.

〔背景技術の問題点〕[Problems with background technology]

しかしながら、このような従来の金属蒸気レーザ装置に
あっては次のような問題があった。
However, such conventional metal vapor laser devices have the following problems.

すなわち、レーザ光出力を上シフさせるために、放電用
バッファガスの圧力を昇圧して投入電力を上シtさUる
と、両電極5.6の先端部の極く一部から1/i雷が開
始し、両電極5.6の先端が局部的に過熱される。しか
も、これら両電極5.6の先端部外周面はセラミック管
1の内周面に接触しているので、この接触部でセラミッ
ク管1が局部的に過熱される。
That is, in order to shift the laser light output upward, when the pressure of the discharge buffer gas is increased and the input power is increased, 1/i Lightning starts and the tips of both electrodes 5.6 become locally heated. Furthermore, since the outer circumferential surfaces of the tips of both electrodes 5.6 are in contact with the inner circumferential surface of the ceramic tube 1, the ceramic tube 1 is locally overheated at this contact portion.

この過熱が原因で、セラミック管1の寿命が極端に短縮
し、最悪の場合は割れを生ずるという問題h(あった。
Due to this overheating, the life of the ceramic tube 1 is extremely shortened, and in the worst case, cracks may occur.

さらに、真空断熱室13を真空シールするセラミック管
1にはOリング17およσベローズ14を設けているた
めに、これらがおるセラミック管1の両端部を冷却して
いた。このために、セラミック管1内の軸方向中間部が
高温で、その両端部が低温の温度勾配を生じていた。
Furthermore, since the ceramic tube 1 that vacuum-seals the vacuum insulation chamber 13 is provided with an O-ring 17 and a σ bellows 14, both ends of the ceramic tube 1 where these are located are cooled. For this reason, a temperature gradient was created in which the axially intermediate portion of the ceramic tube 1 was at a high temperature and the opposite ends thereof were at a low temperature.

その結果、次のような問題があった。As a result, the following problems occurred.

第1に、例えば金属蒸気源が銅である場合、最大のレー
タ“光出力が得られるセラミック管1の温度範囲が14
50〜1500℃のかなり独歩な温度ダ11成にあるた
めに、レー+7装置としてのゲイン領域が非tニジに独
歩であった。
First, if the metal vapor source is copper, for example, the temperature range of the ceramic tube 1 in which the maximum light output is obtained is 14
Since the temperature range was 50 to 1,500°C, which was quite unique, the gain range as a +7 device was unique.

第2に、セラミック管1の両端部の低一部分に蒸発した
銅等の金属が凝結し−(J11槓し、レーザ光路を閉塞
して出力低下の原因の1つを形成していIご 。
Second, evaporated metal such as copper condenses on the lower parts of both ends of the ceramic tube 1, blocking the laser optical path and forming one of the causes of output reduction.

第3に、セラミック管1の中央部の高調部分では、高温
のために軟化して曲がりを生じ、レーザ出力口を閉塞し
、レーザ光出力を低下さけていた。
Thirdly, the high-pitched portion in the center of the ceramic tube 1 softens and bends due to the high temperature, which blocks the laser output port and prevents the laser light output from decreasing.

(発明の目的〕 本発明は上記事情を考;還してなされたもので、その目
的は、高い電子温)αを1hつ高密度で一様なプラズマ
領域を拡大し、金属酒気を安定しで生成することによっ
て、高出力が安定し−C得られる長寿命の金属蒸気シー
11装置を提供することにある。
(Object of the Invention) The present invention was made in consideration of the above circumstances, and its purpose is to expand a high-density and uniform plasma region by 1h (high electron temperature) α, and to stabilize metal alcohol. The object of the present invention is to provide a long-life metal vapor sea 11 device that can stably produce high output by generating -C.

〔発明の概要〕[Summary of the invention]

上記[1的を達成リ−るために本発明は、金属粒子を内
蔵する放電管に放゛5u用バッファガスを供給して放電
さげ、この11i電管の外周に真空断熱室を設ける金属
蒸気レーザ装置にJ5いて、上記放電管を、上記金属粒
子を内蔵して一対の補助電極を内部に対向配量する内管
と、この内管をスペーりを介して軸方向摺動自在に収容
して上記真空断熱室を気密にシールリ−る中間管と、こ
の中間管の外周に密着して外1べされる高融点金J11
′!IJの外管とで多重管に構成したことに特徴がある
In order to achieve the above-mentioned [1], the present invention supplies a 5U buffer gas to a discharge tube containing metal particles to reduce the discharge, and provides a vacuum insulation chamber around the outer periphery of the 11I electric discharge tube. J5 is installed in the laser device, and the discharge tube is housed in an inner tube containing the metal particles and having a pair of auxiliary electrodes disposed therein so as to be slidable in the axial direction through a space. An intermediate tube that airtightly seals the vacuum insulation chamber, and a high melting point gold J11 that is tightly attached to the outer periphery of the intermediate tube.
′! The feature is that it is configured into a multiple tube with the outer tube of the IJ.

〔発明の実施例〕[Embodiments of the invention]

以下、本発明の実施例について第1図および第2図を参
照して説明づる。なお、図中、第3図とJ(通する部分
には同一・符号をイリして、その重複した部分の説明【
、1省略する。
Embodiments of the present invention will be described below with reference to FIGS. 1 and 2. In addition, in the figure, the same reference numerals are omitted for the parts that pass through Figure 3 and J (explanation of the overlapping parts [
, 1 omitted.

第1図は本発明の一実施例の全体構成を示し、外囲容器
であるケーシング9内の中央部に放電管20を同軸状に
収容している。
FIG. 1 shows the overall configuration of an embodiment of the present invention, in which a discharge tube 20 is housed coaxially in the center of a casing 9, which is an outer envelope.

放雷管20は第2図の要部拡大縦断面図に示寸ように内
管2OAと中間管20Bと外管20Gとを順次同軸状に
収容する3車管に構成されている。
The detonator 20 is configured as a three-tube tube that sequentially accommodates an inner tube 2OA, an intermediate tube 20B, and an outer tube 20G in a coaxial manner, as shown in the enlarged vertical cross-sectional view of the principal part in FIG.

内管20△は金属粒子8の沸点温度まで使用可能な^耐
熱f1セラミックスにJ:り円管状に形成され、その内
部に金属粒子8を配置して放電部2を形成し、その両開
口端部には短軸円筒状の一対の補助電極21a、21b
を密着させて内嵌している。一対の補助電極21a、2
1bはタングステン、タンタルもしくはモリブデン等の
高融点金属よりなり、内管20△内の放電部2において
所要゛の間隔をおいて左右に対向させて配置される。各
補助電極21a、21bは放電FIs2に発生する放電
プラズマにより加熱されると共に、その熱を内管20△
の両開口端部に伝熱して内管2OAの温度分布の均一化
を図っている。
The inner tube 20△ is made of heat-resistant f1 ceramics that can be used up to the boiling point temperature of the metal particles 8, and is formed into a circular tube shape. A pair of short-axis cylindrical auxiliary electrodes 21a and 21b are provided in the part.
It is fitted tightly inside. A pair of auxiliary electrodes 21a, 2
The members 1b are made of a high melting point metal such as tungsten, tantalum, or molybdenum, and are arranged to face each other left and right with a required interval in the discharge section 2 within the inner tube 20Δ. Each auxiliary electrode 21a, 21b is heated by the discharge plasma generated in the discharge FIs2, and the heat is transferred to the inner tube 20△
Heat is transferred to both open ends of the inner tube 2OA, thereby making the temperature distribution of the inner tube 2OA uniform.

内管2OAの外側方では、この内管20Δとほぼ同一径
の円筒状の陽極5J′3よび陰極6が内管20△と軸方
向に所要の間隔をおいて対向配回されている。内管20
△はこれより大径かつ長軸の高耐熱性ヒラミックス装の
中間管20B内に、リング状の複数のスペーサ22を介
して軸方向[習動自在にかつ同軸状に収容され、内管2
OAの軸方向の熱伸縮をフリーにしている。スペーサ2
2は熱伝導性が低いセラミックスよりなり、内管20△
と中間管20Bとのある程度の断熱を図っている。
On the outside of the inner tube 20A, a cylindrical anode 5J'3 and a cathode 6 having substantially the same diameter as the inner tube 20Δ are disposed opposite to the inner tube 20Δ at a required distance in the axial direction. Inner tube 20
△ is housed in the intermediate tube 20B of the highly heat-resistant Hiramix device with a larger diameter and longer axis in the axial direction [moveable and coaxially] through a plurality of ring-shaped spacers 22, and the inner tube 2
Thermal expansion and contraction in the axial direction of the OA is freed. Spacer 2
2 is made of ceramics with low thermal conductivity, and the inner tube is 20△
A certain degree of heat insulation is provided between the intermediate pipe 20B and the intermediate pipe 20B.

中間管20Bの各間口端部は陽極5と陰極6の先端部外
周までそれぞれ伸びており、両省間には環状の間隙、す
なわち、11i電用バツフアガスを介在さけるためのガ
スギVツブ5Δ、6Aを設定している。また、中間管2
0Bの各開口端部外周に外■されたOリング17の外周
には、さらに外リング23が外嵌され、外リング23は
ベローズ14を介して真空断熱v23を区画する隔壁に
伸縮自在に接続されている。これにより、中間管20B
は真空断熱室13の中央部を気密にシールしている。
Each front end of the intermediate tube 20B extends to the outer periphery of the tip of the anode 5 and the cathode 6, respectively, and there is an annular gap between the two, that is, a gas gear V-tube 5Δ, 6A to prevent the 11i electric buffer gas from intervening. It is set. Also, intermediate pipe 2
An outer ring 23 is further fitted on the outer periphery of the O-ring 17 that is placed on the outer periphery of each opening end of 0B, and the outer ring 23 is telescopically connected to the partition wall that partitions the vacuum insulation v23 via the bellows 14. has been done. As a result, the intermediate pipe 20B
The central part of the vacuum insulation chamber 13 is hermetically sealed.

中間管20Bの軸方向中間部外周には内管20Aとほぼ
等しい長さの外管20 Ch<密に外嵌されている。外
管20Cはタングステン、タンタルまたはモリブデン等
の高融点金属に」:り円管状に形成され、放電部2の放
電時における中間管20Bの曲げ等の熱変形を防止する
と共に、高い熱伝導性により中間管20Bの温度分布の
均一化を図る。
An outer tube 20 having substantially the same length as the inner tube 20A is tightly fitted onto the outer periphery of the axially intermediate portion of the intermediate tube 20B. The outer tube 20C is made of a high melting point metal such as tungsten, tantalum, or molybdenum and is formed into a circular tube shape to prevent thermal deformation such as bending of the intermediate tube 20B during discharging in the discharge section 2, and has high thermal conductivity. This aims to make the temperature distribution of the intermediate tube 20B uniform.

次に、本実施例の作用について述べる。Next, the operation of this embodiment will be described.

まず、放電部2と真空断熱室13とを各ロータリポンプ
4.15にJ、リイれぞれ排気する。次にガス供給系3
 /Jl rら内管2OA内にNe等の放電用バッファ
ガスを供給して、陽極5ど陰極6とにパルス高電圧電源
7のパルス高電斤を印加し、セラミックス製の内管2O
A内の放電部2で放電させる。この放電時に生ずる放電
プラズマにより内管20Δが加熱され、例えば銅蒸気レ
ー11の場合、この内管20△の軸方向中間部がレーザ
発振に最適な1 /I 50〜1500’Cに加熱され
る。
First, the discharge section 2 and the vacuum insulation chamber 13 are evacuated using the rotary pumps 4 and 15, respectively. Next, gas supply system 3
/Jl r etc. A discharge buffer gas such as Ne is supplied into the inner tube 2OA, and a pulsed high voltage from a pulsed high voltage power source 7 is applied to the anode 5 and cathode 6, and the ceramic inner tube 2OA is
Discharge is performed in the discharge section 2 in A. The inner tube 20Δ is heated by the discharge plasma generated during this discharge, and for example, in the case of the copper vapor beam 11, the axially intermediate portion of the inner tube 20Δ is heated to 1/I 50 to 1500'C, which is optimal for laser oscillation. .

このとぎ、内管20△は、熱伝導性の悪いセラミックス
製のスペーサ゛22によってのみ支持されているので、
管内の温度分布は放電プラズマからの熱負向が一定のた
めに、はぽ均一・となる。
At this point, the inner tube 20△ is supported only by the spacer 22 made of ceramics with poor thermal conductivity.
The temperature distribution inside the tube is uniform because the negative heat from the discharge plasma is constant.

また、内管20△の両開口端部では開口しているために
、fIi射冷却により多少冷却されるが、熱伝導性の良
9JIな左右一対の補助電極21a、21bを介して内
管2OA内の熱が両開口端部に伝熱されて加熱するので
、内管20Δ内の淘度分イFが均一となる。これにより
、レー會ア装置としてのゲイン領域が非常に広くなり、
大幅な出力上背を図ることができる。
In addition, since both opening ends of the inner tube 20Δ are open, they are somewhat cooled by fIi radiation cooling, but the inner tube 2OA is Since the heat inside is transferred to both open ends and heated, the degree of stagnation F within the inner tube 20Δ becomes uniform. As a result, the gain range as a laser device becomes extremely wide.
It is possible to achieve a significant increase in output.

また、補助電極21a、21bは、陰極6と陽極5との
放電時には、内管2OA内部に敢°市Jるだめの室内電
極として作用ヅる。つまり、放電プラズマは左右一対の
補助電極21a、21bの内側に発生Jる。
Further, when the cathode 6 and the anode 5 are discharging, the auxiliary electrodes 21a and 21b function as indoor electrodes inside the inner tube 2OA. In other words, discharge plasma is generated inside the pair of left and right auxiliary electrodes 21a and 21b.

内管2OAは放7t? IL5に熱膨張ηるが、一対の
電極5,6とは軸方向に充分な間隔が設定されているの
で、電極5,6に衝当して損傷を与えることはない。
Is the inner tube 2OA 7t? Although the IL5 undergoes thermal expansion η, since a sufficient distance is set between the pair of electrodes 5 and 6 in the axial direction, the IL5 will not be damaged by hitting the electrodes 5 and 6.

また、内管20△はスベー1す22により1習初自在に
支持されているので、内’Q 20△の軸方向伸縮がフ
リーどなる。
Moreover, since the inner tube 20Δ is freely supported by the base 122, the inner tube 20Δ can freely expand and contract in the axial direction.

陽極5および陰J46の先端部外周と中間管20B内周
とにはガスギ11ツブ5△、6Aを有してJ3す、各1
1i極5,6先端部が高温に加熱しても中間管20Bの
両開口端部が熱的影響を受けることがなく、中間管20
[3の長寿命を図ることができる。
The outer periphery of the tip of the anode 5 and the negative J46 and the inner periphery of the intermediate tube 20B are provided with gas hooks 11, 5△, 6A, respectively.
Even if the tips of the 1i poles 5 and 6 are heated to a high temperature, both open ends of the intermediate tube 20B are not thermally affected, and the intermediate tube 20
[3] Long life can be achieved.

イして、中間管20Bの外周にはPl融点金属製の外T
120 Cを[iさせて外1良しているので、この外管
20Cの熱伝導により外管20Cの長さ分は中間管20
[3内の温度を均一に保持することができる。また、内
管2OAが高温で軟化しても外管20Cにより支持され
ているので、曲げを防止することができる。
The outer periphery of the intermediate tube 20B is made of an outer T made of Pl melting point metal.
Since the outer tube 20C has a heat conduction of 120C, the length of the outer tube 20C is the same as that of the intermediate tube 20.
[The temperature within 3 can be maintained uniformly. Further, even if the inner tube 2OA softens at high temperatures, it is supported by the outer tube 20C, so bending can be prevented.

なお、本発明は上述実施例に限定されるものではなく、
例えば内管2OAを分割構造にしたり、外管20Cの外
周にさらにセラミックス製の円管を外嵌してもよい。
Note that the present invention is not limited to the above-mentioned embodiments,
For example, the inner tube 2OA may have a divided structure, or a circular ceramic tube may be further fitted around the outer circumference of the outer tube 20C.

(発明の効果) 以上説明したように本発明は、金属粒子を内蔵する放電
管にIIi電川バ用フ?ガスを供給して放゛心さぜ、こ
の放電管の外周に真空断熱室を設Eノる金属蒸気レーI
F装置において、上記敢雷管を、上記金属粒子を内蔵し
て一対の補助電極を内部に対向配置する内管と、この内
管をスベーVを介し−C軸方向摺動自在に収容して上記
真2断熱窄を気密にシールする中間管と、この中間管の
外周に密着して外嵌される高融点金属製の外管とで多重
管に構成した。
(Effects of the Invention) As explained above, the present invention provides a discharge tube containing metal particles with a tube for use in the IIi electric current bar. After supplying gas, a vacuum insulation chamber was installed around the outer periphery of the discharge tube.
In the F device, the detonator is housed in an inner tube in which the metal particles are built in and a pair of auxiliary electrodes are disposed facing each other inside, and the inner tube is accommodated in a slidable manner in the -C axis direction via a sub-V. A multi-tube structure was constructed with an intermediate tube that airtightly sealed the double insulation constriction, and an outer tube made of a high-melting point metal that was tightly fitted around the outer periphery of the intermediate tube.

したがって、本発明にJ、れば、金属粒子を内蔵して放
電部を右する内管の温度分布の均一化を全長に口って図
ることができるので、高温高密度のプラズマ領域を内管
のほぼ全長に亘ってほぼ均一に分布させることができる
Therefore, according to the present invention, it is possible to make the temperature distribution of the inner tube containing metal particles and forming the discharge part uniform over the entire length, so that the high-temperature and high-density plasma region can be transferred to the inner tube. can be distributed almost uniformly over almost the entire length.

これにより、レーザ光出力の大幅な上背と安定性の向上
とを図ることができる。
Thereby, it is possible to significantly increase the laser light output and improve stability.

また、中間管の曲げを防止し、健全性を維持することが
できるので、放電管としての寿命の延長を図ることがで
き、信頼性と稼動率の向上を図ることができる。
Furthermore, since the intermediate tube can be prevented from being bent and its integrity can be maintained, the life of the discharge tube can be extended, and reliability and operating efficiency can be improved.

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

第1図は本発明に係る金属蒸気レーザ装置の一実施例の
全体構成を一部断面で承り全体構成図、第2図は第1図
で示1要部の拡大m所面図、第3図は従来の金属蒸気シ
ー11装置の全体構成を一部断面C承り全体構成図であ
る。 1.20・・・放電管、2・・・放電部、3・・・ガス
供IM、4,15・・・ロータリポンプ、5・・・陽極
、6・・・陰極、8・・・金属粒子、13・・・真空断
熱室、20A・・・内管、20B・・・中間管、20C
・・・外管、21a、21b・・・補助電極。
Fig. 1 is a partial cross-sectional view of the entire structure of an embodiment of a metal vapor laser device according to the present invention; Fig. 2 is an enlarged cross-sectional view of the main parts shown in Fig. 1; The figure is a partial cross-sectional view of the overall configuration of a conventional metal vapor sear 11 device. 1.20...Discharge tube, 2...Discharge part, 3...Gas supply IM, 4,15...Rotary pump, 5...Anode, 6...Cathode, 8...Metal Particles, 13... Vacuum insulation chamber, 20A... Inner tube, 20B... Intermediate tube, 20C
... Outer tube, 21a, 21b... Auxiliary electrode.

Claims (1)

【特許請求の範囲】 1、金属粒子を内蔵する放電管に放電用バッファガスを
供給して放電させ、この放電管の外周に真空断熱室を設
ける金属蒸気レーザ装置において、上記放電管を、上記
金属粒子を内蔵して一対の補助電極を内部に対向配置す
る内管と、この内管をスペーサを介して軸方向摺動自在
に収容して上記真空断熱室を気密にシールする中間管と
、この中間管の外周に密着して外嵌される高融点金属製
の外管とで多重管に構成したことを特徴とする金属蒸気
レーザ装置。 2、内管、中間管およびスペーサがセラミックスよりな
る特許請求の範囲1項に記載の金属蒸気レーザ装置。
[Scope of Claims] 1. A metal vapor laser device in which a discharge buffer gas is supplied to a discharge tube containing metal particles for discharge, and a vacuum insulation chamber is provided around the outer periphery of the discharge tube. an inner tube that contains metal particles and has a pair of auxiliary electrodes disposed therein facing each other; an intermediate tube that accommodates the inner tube so as to be slidable in the axial direction via a spacer and airtightly seals the vacuum insulation chamber; A metal vapor laser device characterized in that the intermediate tube is configured with a multi-tube structure including an outer tube made of a high melting point metal that is tightly fitted around the outer periphery of the intermediate tube. 2. The metal vapor laser device according to claim 1, wherein the inner tube, intermediate tube, and spacer are made of ceramics.
JP23948485A 1985-10-28 1985-10-28 Metal vapor laser apparatus Pending JPS62101093A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP23948485A JPS62101093A (en) 1985-10-28 1985-10-28 Metal vapor laser apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP23948485A JPS62101093A (en) 1985-10-28 1985-10-28 Metal vapor laser apparatus

Publications (1)

Publication Number Publication Date
JPS62101093A true JPS62101093A (en) 1987-05-11

Family

ID=17045460

Family Applications (1)

Application Number Title Priority Date Filing Date
JP23948485A Pending JPS62101093A (en) 1985-10-28 1985-10-28 Metal vapor laser apparatus

Country Status (1)

Country Link
JP (1) JPS62101093A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01151281A (en) * 1987-12-09 1989-06-14 Toshiba Corp Metal vapor laser device
JP2007198291A (en) * 2006-01-27 2007-08-09 Shimadzu Corp Rotating equipment

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01151281A (en) * 1987-12-09 1989-06-14 Toshiba Corp Metal vapor laser device
JP2007198291A (en) * 2006-01-27 2007-08-09 Shimadzu Corp Rotating equipment

Similar Documents

Publication Publication Date Title
US3274429A (en) High frequency electron discharge device with heat dissipation means
US3970891A (en) Electron collector for an electron beam tube
JPS62101093A (en) Metal vapor laser apparatus
JP3038830B2 (en) Conduction-cooled multistage collector
US4912719A (en) Ion laser tube
JP2598009B2 (en) Metal vapor laser oscillation tube
US3448325A (en) Linear beam tube having a beam collector cooled by radiation through an infrared window
US4945545A (en) Cold electrode metal vapor laser
JPS6226878A (en) Metal vapor laser oscillation tube
US3448313A (en) Efficient radiation cooled beam collector for linear beam devices
US3275866A (en) Magnetron cathode structures
JPS6226877A (en) Metal vapor laser oscillation tube
JPS61180488A (en) Ion laser tube
JPS63199471A (en) Metallic vapor laser oscillating tube
JP2538590B2 (en) Metal vapor laser device
JP3083390B2 (en) Metal vapor laser equipment
US4821279A (en) Gas laser
JPH01228183A (en) Metal vapor laser oscillator
JPS6197883A (en) Metallic vapor laser
JPS63252490A (en) Metal vapor laser device
JPS5918696Y2 (en) ion laser tube
JP2971595B2 (en) Metal vapor laser oscillation tube
JPS5918695Y2 (en) ion laser tube
JPH05110163A (en) Laser tube
JPS5826767B2 (en) Rod hot cathode assembly