JPS63253680A - Metal vapor laser device - Google Patents

Metal vapor laser device

Info

Publication number
JPS63253680A
JPS63253680A JP8718487A JP8718487A JPS63253680A JP S63253680 A JPS63253680 A JP S63253680A JP 8718487 A JP8718487 A JP 8718487A JP 8718487 A JP8718487 A JP 8718487A JP S63253680 A JPS63253680 A JP S63253680A
Authority
JP
Japan
Prior art keywords
electrode
core tube
discharge
insulating layer
furnace core
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
JP8718487A
Other languages
Japanese (ja)
Other versions
JPH0636447B2 (en
Inventor
Nobutada Aoki
延忠 青木
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 JP62087184A priority Critical patent/JPH0636447B2/en
Publication of JPS63253680A publication Critical patent/JPS63253680A/en
Publication of JPH0636447B2 publication Critical patent/JPH0636447B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime 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 improve the temperature-rise efficiency of a core tube and laser- oscillation efficiency and to increase an output from a laser device by forming a heat-insulating layer holding discharge heat on the outer circumference of the core tube with an electrode and an electrode support flange and forming a large number of protrusions on the electrode. CONSTITUTION:A positive electrode 3 and a negative electrode 4 are set up oppositely at both end sections of a core tube 2 generating plasma as a laser medium. The positive electrode 3 and the negative electrode 4 are supported and fixed respectively by electrode support flanges 5a, 6a. A large number of protrusions 24 are shaped to the inner circumferential surfaces of the cylindrically formed positive electrode 3 and negative electrode 4. The electrode support flanges 5a, 6a are formed to a tapered shape so as to have inclined planes 25 spreading toward the outside of the core tube and be opposed to the edge faces 9a of a heat-insulating layer 9. Insulators 26 are interposed among the electrode support flanges 5a, 6a and the edge faces 9a of the heat-insulating layer 9. Consequently, discharge is easy to be generated among the tips of the protrusions 24, and discharge on the outside of the core tube is reduced. Accordingly, discharge energy is concentrated effectively into the core tube.

Description

【発明の詳細な説明】 (発明の目的) (産業上の利用分野) 本発明は金属蒸気レーザi!!iに係り、特に炉芯管外
における放電を防止し、放電エネルギの右動活用を図り
、^い効率で高出力のレーザ光を発振し冑る金属蒸気レ
ーザ1A置に関する。
[Detailed description of the invention] (Object of the invention) (Industrial application field) The present invention is a metal vapor laser i! ! In particular, the present invention relates to a metal vapor laser 1A device that prevents discharge outside the furnace core tube, utilizes the discharge energy in the right direction, and oscillates and burns high-output laser light with high efficiency.

(従来の技術) シー11装置は、素材切削加:I、光通(Ω、医療技術
、原子力産業など広い分野で使用されている。
(Prior Art) The Sea 11 device is used in a wide range of fields such as material cutting, optical communication, medical technology, and the nuclear industry.

特に原イカ産業においては、複数のウラン同位体混合物
から特定の1IJ1位体を選択的に励起し分ll!ηる
レーザ法によるウラン同位体の濃縮技術の中核をなして
いる。
Particularly in the raw squid industry, a specific 1IJ1 tope is selectively excited from a mixture of multiple uranium isotopes. This is the core of uranium isotope enrichment technology using the laser method.

ウラン同位体の濃縮において使用する金属蒸気レーデ装
置としては、高効率でjdも高出力のレーザが得られる
銅蒸気レーザ装置が一般に採用されている。この装置は
金属銅に放電エネルギを付与し、高温に加熱して金属蒸
気を形成し、同時にレーザ媒質となるプラズマを生成し
、所定波長を右するレーザ光を発振させるように構成さ
れる。
As a metal vapor radar device used for enriching uranium isotopes, a copper vapor laser device is generally employed because it can provide a laser with high efficiency and high jd output. This device is configured to apply discharge energy to metal copper, heat it to a high temperature to form metal vapor, and simultaneously generate plasma, which serves as a laser medium, to oscillate laser light at a predetermined wavelength.

第51!21は従来のこの秤の金属蒸気レーザ装置の構
成を爪′g断面図である。発振管本体1の中心部には耐
熱性をイjする放電管としてのか芯管2が収容される。
Nos. 51 and 21 are cross-sectional views of the conventional metal vapor laser device of this scale. A core tube 2 serving as a discharge tube with high heat resistance is accommodated in the center of the oscillation tube body 1.

この炉芯管2の両端部には、陽゛市極3および陰tt捗
4が対向して配設され、これらの電極3.4はそれぞれ
電極支持フランジ5.6によって支持され、この電極間
に形成される放電空間7においてパルス二極放電が行な
われる。炉芯管2の内底部には、金属蒸気を生成する例
えば銅粒などの金属蒸気源8が配置される。
At both ends of this furnace core tube 2, a positive electrode 3 and a negative electrode 4 are disposed facing each other, and these electrodes 3.4 are each supported by an electrode support flange 5.6, and between these electrodes A pulsed bipolar discharge occurs in the discharge space 7 formed in the discharge space 7 . At the inner bottom of the furnace core tube 2, a metal vapor source 8, such as copper grains, for generating metal vapor is arranged.

また炉芯管2の外周には、アルミlファイバ等の材料か
ら成る断熱層9が形成され、その断熱層9を所定位置に
固定し保護するために、石英等で形成した保護管10が
断熱層9の外周に設けられている。保護管10と、その
外側に配設された外部真空容器11との間には真空断熱
室12が形成される。この真空断熱室12および炉芯管
2内の放電空間7は排気装置13に接続されて、内部が
真空状態に維持される。
Further, a heat insulating layer 9 made of a material such as aluminum fiber is formed on the outer periphery of the furnace core tube 2, and in order to fix and protect the heat insulating layer 9 in a predetermined position, a protective tube 10 made of quartz or the like is heat insulated. It is provided on the outer periphery of layer 9. A vacuum insulation chamber 12 is formed between the protection tube 10 and an external vacuum container 11 disposed outside of the protection tube 10. The vacuum insulation chamber 12 and the discharge space 7 in the furnace core tube 2 are connected to an exhaust device 13, and the inside thereof is maintained in a vacuum state.

また、陽電極3と陰電極4とを絶縁し、良好な放電を得
るために、外部真空容器11と電極支持フランジ6との
間に、セラミックまたはガラス等の絶縁材で形成したブ
レーク管14が介装されている。
Further, in order to insulate the positive electrode 3 and the negative electrode 4 and obtain good discharge, a break tube 14 made of an insulating material such as ceramic or glass is installed between the external vacuum vessel 11 and the electrode support flange 6. It has been intervened.

レーザ光を発振させる操作は、まず排気装置13を作動
させて真空断熱室12および敢t1空間7内を排気し、
続いて、バッファガス供給源15から放電空間7内にN
e等のバッフ7ガスを導入し、内部を一定圧力に保持づ
る。
To oscillate the laser beam, first operate the exhaust device 13 to exhaust the inside of the vacuum insulation chamber 12 and the space 7,
Subsequently, N is supplied into the discharge space 7 from the buffer gas supply source 15.
A buff 7 gas such as e is introduced to maintain a constant pressure inside.

この状態で高電圧電源16、パルス回路17、パルスド
ライブ電源18を起動Jると、陽電443と陰電極4と
の間にパルス状高電1王が印加されて放電空間7におい
て放電プラズマが生起りる。このtllTiプラズマ中
の自由電子に浮遊状態の金属蒸気が衝突して金属蒸気が
励起され、励起された金属蒸気が低エネルギ単位に遷移
する際に所定波長のレーザ光が発生する。放電空間7内
で発生したレーデ光はブリュースタ窓19.20を通過
し、さらにレーザ光共振器21を構成する出力ミラー2
2および全反射ミラー23で反射する間にその振幅が増
大し、出力ミラー22から発振する。
When the high voltage power source 16, pulse circuit 17, and pulse drive power source 18 are started in this state, a pulsed high electric current is applied between the positive electrode 443 and the negative electrode 4, and discharge plasma is generated in the discharge space 7. Rir. The floating metal vapor collides with the free electrons in this tllTi plasma to excite the metal vapor, and when the excited metal vapor transitions to a lower energy unit, a laser beam of a predetermined wavelength is generated. The Rede light generated in the discharge space 7 passes through the Brewster window 19, 20, and further passes through the output mirror 2 constituting the laser beam resonator 21.
2 and the total reflection mirror 23, its amplitude increases, and the output mirror 22 oscillates.

(発明が解決しようとする問題点) 上述のような従来構造の金属蒸気レーザ装置においては
、両電極間にパルス状高電几を印加り“ることによって
放電空間内に放電プラズマを生成しているが、この放電
現象は、第6図(Δ)に例示ηるように両電極の先端間
のみで発生しているのではなく、実際は第6図(B)で
例示するようにか芯管の外部において6発生している。
(Problems to be Solved by the Invention) In the metal vapor laser device of the conventional structure as described above, a discharge plasma is generated in the discharge space by applying a pulsed high voltage between the two electrodes. However, this discharge phenomenon does not occur only between the tips of the two electrodes, as illustrated in Figure 6 (Δ), but actually occurs between the core tube and the core tube, as illustrated in Figure 6 (B). 6 occurs outside of.

特に、電極支持フランジの最外周部が断熱層の端面と近
接して対向しているため、その間の放電が発生し易く、
断熱層9と保:J!!管10との間隙部を矢印で示すよ
うに放電電流iが流れたり、また断熱層9の内部を直接
通って放電する場合もある。この炉芯管外放電が多発す
ると、放電エネルギは炉芯管内部に付与されずに装d外
に逸散し、炉芯管の昇温効率および装置の運転効率が低
下する。また、炉2.ffi内の金属蒸気を励起する放
電エネルギ゛が不足し、シー11発振がI41難となる
場合がある。
In particular, since the outermost periphery of the electrode support flange faces the end face of the heat insulating layer closely, discharge is likely to occur between them.
Insulation layer 9 and protection: J! ! In some cases, the discharge current i flows through the gap between the tube 10 and the tube 10 as shown by the arrow, or directly passes through the inside of the heat insulating layer 9 and is discharged. If this discharge outside the furnace core tube occurs frequently, the discharge energy is not applied to the inside of the furnace core tube but is dissipated outside the casing, reducing the temperature raising efficiency of the furnace core tube and the operating efficiency of the device. Also, furnace 2. There is a case where the discharge energy to excite the metal vapor in the ffi is insufficient, and the oscillation of the sea 11 becomes difficult.

また、断熱層9に放電電流iが流れるためfllJi熱
材の劣化が促進され、す期に交換が必要となる等の保守
管理上の問題点す発生する。
Further, since the discharge current i flows through the heat insulating layer 9, the deterioration of the fllJi heating material is accelerated, causing problems in terms of maintenance and management, such as the need for frequent replacement.

本発明は上記の問題点を解決するためになされたもので
あり、放電エネルギがか芯管外へ逸rll することを
防止しc′#効に利用されるように構成し、炉芯管の背
温効率の向上を図り、炉芯管内に充満する金属蒸気の励
起割合を増加せしめ、高効率で高出力のレーザ光を発振
することがでさる金属蒸気レーザ装置を提供することを
目的と覆る。
The present invention has been made in order to solve the above problems, and is configured to prevent the discharge energy from escaping outside the core tube and to be used for the c'# effect. The purpose of this invention is to provide a metal vapor laser device that can emit high-efficiency, high-output laser light by improving back-heating efficiency and increasing the excitation rate of the metal vapor filling the furnace core tube. .

〔発明の構成〕 (問題点を解決するための手段) 本発明に係る金属蒸気レーザ′J装置は、金属に放電エ
ネルギを付ちすることによりレーIF媒質となるプラズ
マを発生さUる炉芯管と、この炉芯管の両端部に対向し
て設(Jられ、炉芯管内にパルス放電を行なう一1t 
441と、電極を支持する電気支持フランジと、炉芯管
内の放電熱を保持するために炉芯管の外周に形成された
断熱層とを備え、上記電極に多数の突起を形成したこと
を特徴と16゜(作用) 上記構成の金fIX蒸気し−If装置によれば、炉芯管
の両端に配設した゛電極に、多数の突起を形成している
ため、陽71iNIと陰電極との間の放電が起り易い。
[Structure of the Invention] (Means for Solving the Problems) The metal vapor laser device according to the present invention has a furnace core that generates plasma, which becomes a ray IF medium, by applying discharge energy to a metal. A tube and a tube installed opposite to each other at both ends of the furnace core tube to generate a pulse discharge inside the furnace core tube.
441, an electric support flange for supporting the electrode, and a heat insulating layer formed on the outer periphery of the furnace core tube to retain discharge heat within the furnace core tube, and a large number of protrusions are formed on the electrode. and 16゜(Function) According to the gold fIX steam-If device having the above configuration, a large number of protrusions are formed on the ゛electrodes arranged at both ends of the furnace core tube, so that the contact between the positive 71iNI and the negative electrode is Discharge between the parts is likely to occur.

IJなわら、陽電極に設けた突起の尖端部とli2市捗
に設Uた突起の尖端部とがnいに放電空間を介して対向
ケるため、尖端間における放電がf!1し易い。そのた
め、電極支持フランジから断熱層の内部を通り、または
、断熱層と保護管との間隙部を通って放電バスが形成さ
れることが相対的に抑制され、炉芯管外放11!は大幅
に減少する。
In IJ, the tip of the protrusion provided on the positive electrode and the tip of the protrusion provided on the li2 electrode face each other across a discharge space, so the discharge between the tips is f! 1 is easy. Therefore, formation of a discharge bus from the electrode support flange through the inside of the heat insulating layer or through the gap between the heat insulating layer and the protective tube is relatively suppressed, and the furnace core tube is released 11! decreases significantly.

したが−)て、hk電1ネルギが炉芯管内に41効に集
中化されることにより炉芯管の’f(温効率、レーIF
光撮効率が向トし、レーザの出力増加を図ることがでさ
る。、L /こ、炉芯管外IIl電による断熱材の劣化
が少ないため、断熱Iの交換等に要する保守管理作業が
大幅に簡素化する。
However, by concentrating hk electric energy into 41 effects in the furnace core tube, 'f(thermal efficiency, ray IF) of the furnace core tube
The optical imaging efficiency is improved and the output of the laser can be increased. , L/This, since there is little deterioration of the insulation material due to the insulation outside the furnace core tube, the maintenance work required for replacing the insulation I, etc. is greatly simplified.

(実施例) 以ド、本発明の実施例につい′C添付図向合内照して説
明する。
(Embodiments) Hereinafter, embodiments of the present invention will be described with reference to the accompanying drawings.

第1図は本発明に係る金属蒸気シー11装;νiの一実
施例を示す断面図て・ある。なJ3、本発明に係る金属
蒸気レーデ装置は電極および電極支持フランジの構造に
特徴を有し、それ以外の部分については第5図に示す従
来例の構成要素と同一であるため、同一要素には同一符
号を付して−その詳細説明は省略する。
FIG. 1 is a cross-sectional view showing one embodiment of a metal vapor sheath 11; νi according to the present invention. J3, the metal vapor radar device according to the present invention is characterized by the structure of the electrode and the electrode support flange, and other parts are the same as the components of the conventional example shown in FIG. are denoted by the same reference numerals, and detailed explanation thereof will be omitted.

第1図に示ず本実施例の金属蒸気レーザ装置は、発振管
本体1の中心部に、レーザ媒質となるプラズマを発生さ
せるか芯管2が配設され、この炉芯管2の両端部に、陽
電極3と陰電極4が対向して設けられる。陽電極3と陰
電極4は、それぞれ電極支持フランジ5a、5aによっ
て支持固定される。円筒状に形成された陽電4Ii3と
陰電極4の内周面には多数の突起24が形成される。
The metal vapor laser device of this embodiment, which is not shown in FIG. A positive electrode 3 and a negative electrode 4 are provided facing each other. The positive electrode 3 and the negative electrode 4 are supported and fixed by electrode support flanges 5a, 5a, respectively. A large number of protrusions 24 are formed on the inner peripheral surfaces of the positive electrode 4Ii3 and the negative electrode 4, which are formed in a cylindrical shape.

この突起24は、例えば第2図(A)に示すように、〜
尖端を右する突起要素24aを電l4i3.4の内周面
に多数Jfi設して形成したり、または電極3.4の側
面を三角形状に切込み、その切込み片を電極の中心方向
に折り曲げて尖端部を突設して形成する。また、第2図
(B)に例示するように電極3.4の先端周部を鋸刃状
に切込んで連続的な突起24を形成することもできる。
This protrusion 24 is, for example, as shown in FIG.
A large number of protruding elements 24a forming the right tip of the electrode 3.4 can be formed on the inner peripheral surface of the electrode 3.4, or the side surface of the electrode 3.4 can be cut into a triangular shape and the cut piece can be bent toward the center of the electrode. Formed with a protruding pointed end. Further, as illustrated in FIG. 2(B), the continuous protrusion 24 can be formed by cutting the peripheral portion of the tip end of the electrode 3.4 into a saw blade shape.

または、いわゆるエツチング処即によって、電極表面を
電解により部分的に腐食溶解せしめ、凹凸を形成して突
起とすることもできる。
Alternatively, the electrode surface may be partially corroded and dissolved by electrolysis using a so-called etching process to form irregularities to form protrusions.

1記突起24を形成した電Ij3./Iはそれぞれ電極
支持フランジ5a、6aに一体に接合され、発振管本体
1内の所定位置に支持固定される。ここで、電極支持フ
ランジ5a、5aは、断熱w!J9の端面9aに対向し
、炉芯管外方に拡開する傾斜面25を有するようにデー
パ状に形成される。
Electrical Ij3.1 having the projection 24 formed thereon. /I are integrally joined to electrode support flanges 5a and 6a, respectively, and are supported and fixed at predetermined positions within the oscillation tube body 1. Here, the electrode support flanges 5a, 5a are heat insulated w! It is formed in a tapered shape so as to have an inclined surface 25 facing the end surface 9a of J9 and expanding outward from the furnace core tube.

また、電極支持フランジ5a、6aと断熱WJ9の端面
9aとの間に、絶縁体26を介装している。
Further, an insulator 26 is interposed between the electrode support flanges 5a, 6a and the end surface 9a of the heat insulating WJ9.

絶縁体26は、例えばセラミック、石英、ガラス等の絶
縁材料で構成される。
The insulator 26 is made of an insulating material such as ceramic, quartz, or glass.

本実施例の金属蒸気レーザ装置によれば、放電空間7を
はさみ、対向して配設された電極3.4に多数の突起2
4が形成され(いるため、その突起24の尖端間におい
C放電が起り易い。そのため、電極支持フランジ5a、
6aから断熱層9を通って放電するか芯管外放電の割合
が減少し、放電エネルギが有効に活用される、。
According to the metal vapor laser device of this embodiment, a large number of protrusions 2 are provided on the electrodes 3.4 which are arranged facing each other across the discharge space 7.
4 is formed (therefore, C discharge is likely to occur between the tips of the protrusions 24. Therefore, the electrode support flange 5a,
The ratio of discharge from 6a through the heat insulating layer 9 or discharge outside the core tube is reduced, and the discharge energy is effectively utilized.

また、′tr1極3,4に放電電流を流す杼路となる電
極支持フランジ5a、6aが断熱層9の端面9aに対向
し、外りに拡開する傾斜面25をイjvるようにデーパ
状に形成されるため、°冷極3,4との接a部の外周か
ら平径方向に頽れる程、断熱層端面9aと電極支持フラ
ンジ5a、 6aとの間隔が拡大し、両者間の放電抵抗
がnより、炉芯管外放電は減少する。
Further, the electrode supporting flanges 5a and 6a, which serve as a shed for flowing discharge current to the 'tr1 poles 3 and 4, face the end surface 9a of the heat insulating layer 9, and are tapered so as to extend outwardly from the inclined surface 25. Since the electrode support flanges 5a and 6a are formed in a shape, the distance between the heat insulating layer end face 9a and the electrode support flanges 5a and 6a increases as the distance from the outer periphery of the contact portion with the cold electrodes 3 and 4 increases in the diametrical direction. When the discharge resistance is n, the discharge outside the furnace core tube decreases.

さらに、電極支持フランジ5a、5aと断熱層端面9a
との間に絶縁体26を介装することにより、両−I!i
間の放電をより効里的に防止することができる。したが
って、′rri極3,4問に付すされた放電エネルギが
か芯管2内に有効に集中化されるため、炉芯管2の胃編
効率、レーデ発振効率が向上しレー量!出力の増強を図
ることができる。
Furthermore, the electrode support flanges 5a, 5a and the heat insulating layer end face 9a
By interposing the insulator 26 between both -I! i
It is possible to more effectively prevent discharge between the two. Therefore, the discharge energy applied to the 3 and 4 poles is effectively concentrated within the core tube 2, which improves the gastric efficiency and oscillation efficiency of the furnace core tube 2, and reduces the amount of radiation. It is possible to increase the output.

また・断熱層9内にJ34Jる炉芯管外放電力くなく、
断熱Hの犬化が少イρいため、断熱材の調整交換雪の保
守管理n業がとしくMI系化される1゜次に、本発明の
他の実施例について第3図J7J、び第4図を参照し−
(説明する。第3図の実施例においては、電極4を支持
する電極支持フランジ6bを電極4と−・体に形成し、
その端部を外側に湾曲形成し、湾曲部27をヘッド28
の内面に嵌装することにより電極4を支持固定している
In addition, there is no discharge force outside the furnace core tube inside the heat insulating layer 9,
Since the heat insulation H is less likely to change, the maintenance and management of insulation material adjustment and replacement is more easily integrated into the MI system. Refer to Figure 4-
(This will be explained. In the embodiment shown in FIG. 3, the electrode support flange 6b that supports the electrode 4 is formed integrally with the electrode 4,
The end portion is curved outward, and the curved portion 27 is formed into a head 28.
The electrode 4 is supported and fixed by being fitted onto the inner surface of the electrode.

この場合、湾曲部27と断熱層端部9aとが隔離し゛(
いるため両省間の放電が少ない。また、従来の円板型の
電極支持フランジ6と比較しで、本実施例の電極支持フ
ランジ6bは電極4と−・体に形成され、ヘッド28内
に嵌装するだ【〕で固定することがCさるため、電極部
の着脱作業が容易である。I また、第4図に示す実施例においては、電144を支持
する電極支持フランジ6Cを電極4と一体に形成し、そ
の端部を外側に拡;i1シて形成し、その拡1m部29
をヘッド28内面に嵌装し、さらにヘッド28内面と電
極支持フランジ6Gとの[IMには絶縁体26aが介装
されている。
In this case, the curved portion 27 and the heat insulating layer end portion 9a are separated (
Therefore, there are few discharges between the two provinces. Also, compared to the conventional disk-shaped electrode support flange 6, the electrode support flange 6b of this embodiment is formed in the same body as the electrode 4, and is fixed by fitting into the head 28 with brackets. Since the diameter is C, attachment and detachment of the electrode part is easy. In addition, in the embodiment shown in FIG. 4, the electrode support flange 6C supporting the electrode 144 is formed integrally with the electrode 4, and its end is expanded outward, and the expanded 1m portion 29 is formed integrally with the electrode 4.
is fitted onto the inner surface of the head 28, and an insulator 26a is interposed between the inner surface of the head 28 and the electrode support flange 6G.

この場合b、拡11)1部29と断熱層端部9aとは隔
離しているため両省間におくjる放電間は少ない。
In this case, since the first part 29 and the end part 9a of the heat insulating layer are separated from each other, the discharge interval between the two parts is small.

また、両者間には絶縁体26aが介装されているため、
より効果的に放電が防止される。また、従来の円板型の
電極支持フランジは使用せ1、電極4と一体に形成され
た拡開部29をヘッド28内に嵌装するだけで電極4を
固定り°ることがCきるため、電極部の保守管理が容易
となる。
Furthermore, since the insulator 26a is interposed between the two,
Discharge is more effectively prevented. In addition, the conventional disk-shaped electrode support flange cannot be used, and the electrode 4 can be fixed simply by fitting the expanded portion 29 formed integrally with the electrode 4 into the head 28. , maintenance and management of the electrode section becomes easy.

〔発明の効宋〕[Efficacy of invention Song Dynasty]

以上説明の通り、本発明に係る金属蒸気レーザ装置によ
れば、炉芯管の両端に配設しIC”l1lf極に多数の
突起を形成しているため、l!g電極の突起の尖端部と
陰電極の突起の尖端部との間の放電空間における放電が
発生し易い。そのため、電極支持フランジから断熱層の
内部を通り、ま/jは断熱層と保護管との間隙部を通っ
て、放電パスが形成されることが相対的に抑v1され、
炉芯管外放雷が大幅に減少する。
As explained above, according to the metal vapor laser device according to the present invention, since a large number of protrusions are formed on the IC"l1lf electrode arranged at both ends of the furnace core tube, the tip of the protrusion of the l!g electrode Discharge is likely to occur in the discharge space between the electrode support flange and the tip of the protrusion of the cathode.Therefore, the discharge from the electrode support flange passes through the inside of the heat insulating layer, and the , the formation of a discharge path is relatively suppressed v1,
Lightning outside the core tube is significantly reduced.

したがって、放電エネルギが炉芯管内に有効に供給され
るため、炉芯管の5vi効率、シー1フ’発振効率が向
]二し、レーデ装置の出力増加を図ることができる。ま
た、断熱層における放電が少ないため断熱材の交換等の
保守管理作業か大幅に簡素化する。
Therefore, since the discharge energy is effectively supplied into the furnace core tube, the 5vi efficiency and the 1F' oscillation efficiency of the furnace core tube are improved, and the output of the RADE device can be increased. In addition, since there is little electrical discharge in the heat insulating layer, maintenance work such as replacing the heat insulating material is greatly simplified.

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

第1図は不発Illに係る金属蒸気レーザ装置の第1実
施例を示?jrgi面図、第2図(A>、(B)G;L
それぞれ電極先端部の形状を示す斜視図、第3図は本発
明の第2実施例を示づ一部分断面図、第4図は本発明の
第3実施例を示す部分断面図、第5図は従来の金属然気
レーザ装置の構成を示す断面図、第6図(A)、(B)
はそれぞれ電極間における放電状態をポす断面図である
。 1・・・発振管本体、2・・・炉芯管、3・・・陽電極
、4・・・陰ff1t4i、5.5a、6,6a、6b
、6cm・・電極支持フランジ、7・・・放電空間、8
・・・金属蒸気源、9・・・断熱層、9a・・・断熱層
の端面、10・・・保護管、11・・・外部真空容器、
12・・・真空断熱室、13・・・排気装置、1/l・
・・ブレーク管、15・・・バッフ1ガス供給源、16
・・・高電圧電源、17・・・パルス回路1.18・・
・パルスドライブ電源、19.20・・・ブリュースタ
窓、21・・・レーザ光共振器、22・・・出力ミラー
、23・・・全反射ミラー、2/I・・・突起、24a
・・・突起要素、25・・・傾斜面、26.26a・・
・絶縁体、27・・・湾曲部、28・・・ヘッド、29
・・・拡開部、i・・・放電電流。 出願人代理人   波 多 野   久(A)    
        (B)第2 図 第3関 第4図
FIG. 1 shows a first embodiment of a metal vapor laser device related to unexploded Ill? jrgi side view, Fig. 2 (A>, (B)G;L
FIG. 3 is a partially sectional view showing the second embodiment of the present invention, FIG. 4 is a partially sectional view showing the third embodiment of the present invention, and FIG. 5 is a perspective view showing the shape of the electrode tip, respectively. Cross-sectional views showing the configuration of a conventional metal-gas laser device, FIGS. 6(A) and 6(B)
are sectional views showing the discharge state between the electrodes, respectively. DESCRIPTION OF SYMBOLS 1... Oscillation tube main body, 2... Furnace core tube, 3... Positive electrode, 4... Negative ff1t4i, 5.5a, 6, 6a, 6b
, 6cm... Electrode support flange, 7... Discharge space, 8
... Metal vapor source, 9... Heat insulating layer, 9a... End face of heat insulating layer, 10... Protection tube, 11... External vacuum container,
12... Vacuum insulation chamber, 13... Exhaust device, 1/l.
...Break pipe, 15...Buffer 1 gas supply source, 16
...High voltage power supply, 17...Pulse circuit 1.18...
・Pulse drive power supply, 19.20... Brewster window, 21... Laser light resonator, 22... Output mirror, 23... Total reflection mirror, 2/I... Protrusion, 24a
... Projection element, 25 ... Inclined surface, 26.26a ...
- Insulator, 27... Curved part, 28... Head, 29
. . . Expanded portion, i . . . Discharge current. Applicant's agent Hisashi Hatano (A)
(B) Figure 2 Figure 3 Figure 4

Claims (1)

【特許請求の範囲】 1、金属に放電エネルギを付与することによりレーザ媒
質となるプラズマを発生させる炉芯管と、この炉芯管の
両端部に対向して設けられ、炉芯管内にパルス放電を行
なう電極と、電極を支持する電気支持フランジと、炉芯
管内の放電熱を保持するために炉芯管の外周に形成され
た断熱層とを備え、上記電極に多数の突起を形成したこ
とを特徴とする金属蒸気レーザ装置。 2、電極支持フランジは、断熱層の端面に対向し、炉芯
管外方に拡開する傾斜面を有するようにテーパ状に形成
した特許請求の範囲第1項記載の金属蒸気レーザ装置。 3、電極支持フランジは、電極支持フランジと断熱層の
端面との間に介装した絶縁体を備える特許請求の範囲第
1項記載の金属蒸気レーザ装置。
[Scope of Claims] 1. A furnace core tube that generates plasma to serve as a laser medium by applying discharge energy to metal, and a pulse discharge device provided at opposite ends of the furnace core tube to generate plasma as a laser medium. an electric support flange for supporting the electrode; and a heat insulating layer formed on the outer periphery of the furnace core tube to retain discharge heat within the furnace core tube, and a large number of protrusions are formed on the electrode. A metal vapor laser device featuring: 2. The metal vapor laser device according to claim 1, wherein the electrode support flange is formed in a tapered shape so as to have an inclined surface facing the end face of the heat insulating layer and expanding outward from the furnace core tube. 3. The metal vapor laser device according to claim 1, wherein the electrode support flange includes an insulator interposed between the electrode support flange and the end face of the heat insulating layer.
JP62087184A 1987-04-10 1987-04-10 Metal vapor laser device Expired - Lifetime JPH0636447B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62087184A JPH0636447B2 (en) 1987-04-10 1987-04-10 Metal vapor laser device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62087184A JPH0636447B2 (en) 1987-04-10 1987-04-10 Metal vapor laser device

Publications (2)

Publication Number Publication Date
JPS63253680A true JPS63253680A (en) 1988-10-20
JPH0636447B2 JPH0636447B2 (en) 1994-05-11

Family

ID=13907901

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62087184A Expired - Lifetime JPH0636447B2 (en) 1987-04-10 1987-04-10 Metal vapor laser device

Country Status (1)

Country Link
JP (1) JPH0636447B2 (en)

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS49123965U (en) * 1973-02-20 1974-10-23
JPS6226877A (en) * 1985-07-29 1987-02-04 Toshiba Corp Metal vapor laser oscillation tube

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS49123965U (en) * 1973-02-20 1974-10-23
JPS6226877A (en) * 1985-07-29 1987-02-04 Toshiba Corp Metal vapor laser oscillation tube

Also Published As

Publication number Publication date
JPH0636447B2 (en) 1994-05-11

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