JPS63239881A - Metal vapor laser oscillator - Google Patents

Metal vapor laser oscillator

Info

Publication number
JPS63239881A
JPS63239881A JP7161287A JP7161287A JPS63239881A JP S63239881 A JPS63239881 A JP S63239881A JP 7161287 A JP7161287 A JP 7161287A JP 7161287 A JP7161287 A JP 7161287A JP S63239881 A JPS63239881 A JP S63239881A
Authority
JP
Japan
Prior art keywords
electrode
plate
discharge tube
tube
discharge
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
JP7161287A
Other languages
Japanese (ja)
Inventor
Naoto Nishida
直人 西田
Jun Sakuma
純 佐久間
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 JP7161287A priority Critical patent/JPS63239881A/en
Publication of JPS63239881A publication Critical patent/JPS63239881A/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 shorten a time from the start of discharge to a laser oscillation by composing an electrode section of an electrode connected to the end of a discharge tube, a plate secured through a thermal insulator having heat resistance, and a conductive member for electrically connecting the electrode to the plate. CONSTITUTION:Electrode sections 21a, 21b are composed of an electrode 22 engaged with the end of a discharge tube 2, a plate 24 secured through a thermal insulator 23 having heat resistance to the electrode 22, and a thin plate 25 made of high melting point V, Mo as a conductive member for electrically connecting the electrode 22 to the plate 24. Thus, the escape of the heat of the tube 2 through the sections 21a, 21b can be suppressed, and the heating time of the tube 2 from the start of discharge to the laser oscillation can be shortened. The heat escaping from the tube 2 is increased at the ratio of radially radiating, the temperature distribution of the tube 2 in the lengthwise direction becomes substantially uniform, and the whole exciting region is allowed to gain access to the optimal temperature of the laser oscillation, thereby increasing laser output.

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発振装置に関し、待に電極部に
改良を施した金属蒸気レーザ発振装置に係わる。
DETAILED DESCRIPTION OF THE INVENTION [Object of the Invention] (Industrial Application Field) The present invention relates to a metal vapor laser oscillation device, and more particularly, to a metal vapor laser oscillation device in which an electrode portion is improved.

(従来の技術) 従来、金属蒸気レーザ発振装置としては、例えば第3図
に示すものが知られている。
(Prior Art) Conventionally, as a metal vapor laser oscillation device, one shown in FIG. 3, for example, is known.

図中の1は、レーザ装置本体である。この装置本体1に
は耐高温性のセラミックスなどからなる放電管2が設け
られ、該放電管2の両端には高融点のタングステンある
いはモリブデンからなるつば付電極3,4が設けられて
いる。また、前記装置本体1の所定の位置には、ガス供
給装置5.真空ポンプ6が連結されている。更に、前記
装置本体1の長手方向に沿う両端部には、0リング7゜
7を介して!’8.9が夫々設けられている。これら窓
8,9を通る直線上つまりレーザ光の発振光路上には、
高反射ミラー10.出力ミラー11が設けられている。
1 in the figure is the main body of the laser device. The device main body 1 is provided with a discharge tube 2 made of high temperature resistant ceramics, etc., and flanged electrodes 3, 4 made of high melting point tungsten or molybdenum are provided at both ends of the discharge tube 2. Further, at a predetermined position of the apparatus main body 1, a gas supply device 5. A vacuum pump 6 is connected. Furthermore, O-rings 7.7 are provided at both longitudinal ends of the device main body 1. '8.9 are provided respectively. On the straight line passing through these windows 8 and 9, that is, on the oscillation optical path of the laser beam,
High reflective mirror 10. An output mirror 11 is provided.

前記電極3.4間には電′a12が設けられている。ま
た、前記放電管2の外周で前記装置本体1の外管1aと
の間には、筒状の熱絶縁物13がその一部が電極3.4
を囲むように設けられている。
An electric wire 'a12 is provided between the electrodes 3 and 4. Further, between the outer circumference of the discharge tube 2 and the outer tube 1a of the device main body 1, there is a cylindrical thermal insulator 13, a part of which is connected to the electrode 3.
It is set up to surround.

一方の前記電極3の端部と前記外壁1a間には、環状の
高電圧絶縁体14がOリング15を介して熱絶縁物13
の一部を囲むように設けられている。
A ring-shaped high voltage insulator 14 is connected to a thermal insulator 13 between the end of one of the electrodes 3 and the outer wall 1a via an O-ring 15.
It is set up to surround a part of the

更に、前記装置本体1の外周で電極4.5の近くには、
高温になった装置本体1を冷却する冷却パイプ16が設
けられている。
Furthermore, near the electrode 4.5 on the outer periphery of the device main body 1,
A cooling pipe 16 is provided to cool down the device main body 1 which has reached a high temperature.

こうした構造の装置において、放電管2の内部には例え
ば同等の金属レーザ媒質17が載置される。そして、放
電管2内を例えば10〜20T orrのNeガスで満
たし、放電させると、放電のエネルギにより放電管2が
加熱され、その温度が手数百度に達する。この時、上記
媒質17の蒸気が所定の圧力に達し、金属蒸気が放電に
より励起され、レーザ発振が生ずる。
In a device having such a structure, for example, an equivalent metal laser medium 17 is placed inside the discharge tube 2. Then, when the inside of the discharge tube 2 is filled with Ne gas of, for example, 10 to 20 Torr and discharged, the discharge tube 2 is heated by the energy of the discharge, and its temperature reaches several hundred degrees. At this time, the vapor in the medium 17 reaches a predetermined pressure, the metal vapor is excited by discharge, and laser oscillation occurs.

ところで、金属蒸気レーザの発振線のエネルギ準位の上
準位の寿命は非常に短く、そのため励起のための放電も
立上がりを速くしなければならない。従って、レーザ装
置の放電管2と外管1aが同軸構造をとり、インダクタ
ンスをできるだけ小ざくしなければならない。それ故、
従来は、第3図に示すように、電極3.4がそのまま放
電管2及び外管1aのシールのためのフランジを兼ねる
構造となっており、0リング7の保護のため7ランジ近
傍は冷却される。
By the way, the lifetime of the upper energy level of the oscillation line of a metal vapor laser is very short, and therefore the discharge for excitation must rise quickly. Therefore, the discharge tube 2 and the outer tube 1a of the laser device must have a coaxial structure and the inductance must be made as small as possible. Therefore,
Conventionally, as shown in Fig. 3, the structure was such that the electrode 3.4 also served as a flange for sealing the discharge tube 2 and the outer tube 1a, and the area around the 7 lange was cooled to protect the 0 ring 7. be done.

しかしながら、従来装置によれば、電極3.4の部材が
比較的大きな熱伝導度を有する^融点のタングステンな
どからなるため、放電管2の熱は電極3,4を通じて外
部に逃げ、放電を開始してからレーザ発振が生ずるまで
の時間、即ち金属蒸気を発生させるための温度に放電管
2が加熱される時間が通常0.5〜1.5時間と、他の
レーザと比較して非常に長いという問題点を有する。
However, according to the conventional device, since the electrodes 3 and 4 are made of tungsten, which has a relatively high thermal conductivity and has a melting point, the heat of the discharge tube 2 escapes to the outside through the electrodes 3 and 4, and the discharge starts. The time from when the discharge tube 2 is heated to the temperature required to generate metal vapor until laser oscillation occurs is usually 0.5 to 1.5 hours, which is very long compared to other lasers. It has the problem of being long.

(発明が解決しようとする問題点) 本発明は上記事情に鑑みてなされたもので、放電開始か
らレーザ発振までの時間を短縮し得る金属レーザ発振装
置を提供することを目的とする。
(Problems to be Solved by the Invention) The present invention has been made in view of the above circumstances, and an object of the present invention is to provide a metal laser oscillation device that can shorten the time from the start of discharge to laser oscillation.

[発明の構成] (問題点を解決するための手段) 本発明は、両端に一対の電極部を有した放電管内部に金
属レーザ媒質を配置し、前記放電管内部を放電により高
温状態として前記媒質を蒸気化してレーザ発振を行う金
属蒸気レーザ発振装置にが゛ おいて、前記電極部を、放電管の端部に連結された電極
と、この電極に耐熱性を有する熱絶縁物を介して固定さ
れた板体と、前記電極と板体を電気的に接続する導電性
部材とから構成されることを要旨とする。
[Structure of the Invention] (Means for Solving the Problems) The present invention provides a method for disposing a metal laser medium inside a discharge tube having a pair of electrode portions at both ends, and bringing the inside of the discharge tube into a high temperature state by electric discharge. In a metal vapor laser oscillation device that vaporizes a medium and performs laser oscillation, the electrode portion is connected to an electrode connected to an end of a discharge tube, and a heat insulator having heat resistance is connected to this electrode. The gist is that it is composed of a fixed plate and a conductive member that electrically connects the electrode and the plate.

(作用) 本発明によれば、 (イ)電極部の一部である電極と板体の接続に低熱伝導
率のバナジウム等からなる薄状板を用いるため、放電管
の熱が電極部を通じて外部に逃げることが抑制できる。
(Function) According to the present invention, (a) Since a thin plate made of vanadium or the like with low thermal conductivity is used to connect the electrode and the plate, which are part of the electrode part, the heat of the discharge tube is transferred to the outside through the electrode part. It is possible to prevent people from escaping.

従って、放電開始時に放電管にある程度の熱が残されて
おり、放電開始からレーザ発振可能となるまでの放電管
の加熱時間が短縮される。
Therefore, a certain amount of heat remains in the discharge tube at the start of discharge, and the heating time of the discharge tube from the start of discharge until laser oscillation becomes possible is shortened.

(ロ)放電管の両端から逃げる熱が減少するため、放電
管から逃げる熱は半径方向への輻射による割合が大きく
なり、放電管の艮ざ方向の濃度分布は従来の装置より一
様に近くなる。
(b) Since the heat escaping from both ends of the discharge tube is reduced, a larger proportion of the heat escaping from the discharge tube is radiated in the radial direction, and the concentration distribution in the direction of the discharge tube is more uniform than in conventional devices. Become.

(ハ)一般に金属蒸気レーザの場合、その発振出力は媒
質雰囲気の温度に大きく依存する。従って、本発明の場
合放電管内の温度分布が一様に近くなることにより、全
励起領域をレーザ発振の最適温度に近づけることができ
、レーザ出力を増大できる。
(c) Generally, in the case of a metal vapor laser, its oscillation output largely depends on the temperature of the medium atmosphere. Therefore, in the case of the present invention, the temperature distribution within the discharge tube becomes nearly uniform, so that the entire excitation region can be brought close to the optimum temperature for laser oscillation, and the laser output can be increased.

(実施例) 以下、本発明の一実施例を第1図及び第2因を参照して
説明する。ここで、第1図は本発明に係る金属蒸気レー
ザ発振装置の全体を示す断面図、第2図は同装置の電極
部の各部材を切り離した斜視図である。但し、同装置は
従来装置(第3図)と電極部を除いて同様な構造となっ
ているため、同部材は同符号を付して説明を省略する。
(Example) Hereinafter, an example of the present invention will be described with reference to FIG. 1 and the second factor. Here, FIG. 1 is a sectional view showing the entire metal vapor laser oscillation device according to the present invention, and FIG. 2 is a perspective view in which each member of the electrode section of the device is cut away. However, since this device has the same structure as the conventional device (FIG. 3) except for the electrode section, the same members will be given the same reference numerals and explanations will be omitted.

図中の21a、21bは、夫々放電管2の両端に取付け
られた電極部である。この電極部21a。
21a and 21b in the figure are electrode parts attached to both ends of the discharge tube 2, respectively. This electrode portion 21a.

21bは、夫々放電管2の端部に嵌合された電極22と
、この電極22に耐熱性を有する熱絶縁物23を介して
固定された板体24と、前記電極22と板体24を電気
的に接続する導−電性部材としての薄状板25とから構
成される。ここで、前記熱絶縁物23は、例えば環状の
セラミックス板である。前記板体24は例えばSUSな
どの金属製の部材からなり、一方の電極部21aの板体
24は高圧N源の高電圧側に、他方の電極部21bの板
体24は高圧電源の低電圧側に接続されている。前記薄
状板25はU字環状をなし、例えばバナジウム、モリブ
デン等の耐高熱性の材料からなる。また、電極22及び
固定用のネジ(図示せず)は夫々モリブデンからなる。
21b includes an electrode 22 fitted to the end of the discharge tube 2, a plate 24 fixed to the electrode 22 via a heat insulating material 23 having heat resistance, and a structure in which the electrode 22 and the plate 24 are connected to each other. It is composed of a thin plate 25 as a conductive member for electrical connection. Here, the thermal insulator 23 is, for example, an annular ceramic plate. The plate body 24 is made of a metal member such as SUS, for example, the plate body 24 of one electrode part 21a is connected to the high voltage side of the high voltage N source, and the plate body 24 of the other electrode part 21b is connected to the low voltage side of the high voltage power source. connected to the side. The thin plate 25 has a U-shaped annular shape and is made of a highly heat-resistant material such as vanadium or molybdenum. Further, the electrode 22 and the fixing screw (not shown) are each made of molybdenum.

ここで、電極22と熱絶縁物23.熱絶縁物23と板体
24との固定は夫々別のネジにより行われ、ネジを通し
て熱が逃げないようにされている。
Here, the electrode 22 and the thermal insulator 23. The heat insulator 23 and the plate 24 are fixed using separate screws, so that heat does not escape through the screws.

上記実施例によれば、電極部21−a、21bが夫々放
電管2の端部に嵌合された電極22と、この電極22に
耐熱性を有する熱絶縁物23を介して固定された板体2
4と、前記電極22と板体24を電気的に接続する導電
性部材としての高融点のモリブデンなどからなる薄状板
25とから構成された構造となっているため、以下に述
べる効果を有する。
According to the above embodiment, the electrode parts 21-a and 21b each include an electrode 22 fitted to the end of the discharge tube 2, and a plate fixed to the electrode 22 via a heat-resistant thermal insulator 23. body 2
4 and a thin plate 25 made of molybdenum with a high melting point as a conductive member that electrically connects the electrode 22 and the plate 24, so that it has the following effects. .

(イ)電極22と板体24の接続に低熱伝導率のバナジ
ウム等からなる薄状板25を用いるため、放電管2の熱
が電極部21a、21bを通じて外部に逃げることが抑
制できる。従って、放電開始時に放電管2にある程度の
熱が残されており、放電開始からレーザ発掘可能となる
までの放電管3の加熱時間が短縮される。
(a) Since the thin plate 25 made of vanadium or the like having low thermal conductivity is used to connect the electrode 22 and the plate 24, it is possible to suppress heat from the discharge tube 2 from escaping to the outside through the electrode parts 21a and 21b. Therefore, a certain amount of heat remains in the discharge tube 2 at the start of discharge, and the heating time of the discharge tube 3 from the start of discharge to the time when laser excavation becomes possible is shortened.

(ロ)放電管2の両端から逃げる熱が減少するため、放
電管2から逃げる熱は半径方向への輻射による割合が大
きくなり、放電管2の長さ方向の温度分布は従来の装置
より一様に近くなる。
(b) Since the heat escaping from both ends of the discharge tube 2 is reduced, a larger proportion of the heat escaping from the discharge tube 2 is due to radiation in the radial direction, and the temperature distribution in the length direction of the discharge tube 2 is more uniform than in conventional devices. become closer to you.

(ハ)一般に金属蒸気レーザの場合、その発振出力は媒
質雰囲気の温度に大きく依存する。従って、本発明の場
合放電管内の温度分布が一様に近くなることにより、全
励起領域をレーザ発振の最適温度に近づけることができ
、レーザ出力を増大できる。
(c) Generally, in the case of a metal vapor laser, its oscillation output largely depends on the temperature of the medium atmosphere. Therefore, in the case of the present invention, the temperature distribution within the discharge tube becomes nearly uniform, so that the entire excitation region can be brought close to the optimum temperature for laser oscillation, and the laser output can be increased.

なお、上記実施例では、導電性部材としてU字環状のバ
ナジウム等からなる薄状板を用いる場合について述べた
が、これに限らず、全体としてU字環状を構成する複数
のへ2箔等の薄状板、あるいは放射状のワイヤなどを用
いても良い。但し、材料は実施例と同材料とする。
In the above embodiment, a case was described in which a U-shaped ring-shaped thin plate made of vanadium or the like was used as the conductive member, but the present invention is not limited to this. A thin plate or radial wire may also be used. However, the material is the same as in the example.

[発明の効果コ 以上詳述した如く本発明によれば、放電開始からレーザ
発振までの時間を短縮し得るとともに、放電管の長さ方
向の温度分布を一様にしかつレーザ出力を増大し得る金
属レーザ発振装置を提供できる。
[Effects of the Invention] As detailed above, according to the present invention, the time from the start of discharge to laser oscillation can be shortened, the temperature distribution in the length direction of the discharge tube can be made uniform, and the laser output can be increased. A metal laser oscillation device can be provided.

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

第1図は本発明の一実施例に係る金属蒸気レーザ発振装
置の断面図、第2図は同装置の電極部の斜視図、第3図
は従来の金属蒸気レーザ発振装置の断面図である。 1・・・レーザ装置本体、1a・・・外管、2・・・放
電管、5・・・ガス供給装置、6・・・真空ポンプ、7
・・・出力ミラー、8,9・・・窓、10・・・高反射
ミラー、11・・・出力ミラー、12・・・電源、13
・・・熱絶縁物、14・・・高電圧絶縁体、17・・・
冷却パイプ、21a。 21b・・・電極部、22・・・電極、23・・・導電
性部材、24・・・板体、25・・・薄状板。
FIG. 1 is a sectional view of a metal vapor laser oscillation device according to an embodiment of the present invention, FIG. 2 is a perspective view of an electrode section of the same device, and FIG. 3 is a sectional view of a conventional metal vapor laser oscillation device. . DESCRIPTION OF SYMBOLS 1... Laser device main body, 1a... Outer tube, 2... Discharge tube, 5... Gas supply device, 6... Vacuum pump, 7
... Output mirror, 8, 9... Window, 10... High reflection mirror, 11... Output mirror, 12... Power supply, 13
...Thermal insulator, 14...High voltage insulator, 17...
Cooling pipe, 21a. 21b... Electrode portion, 22... Electrode, 23... Conductive member, 24... Plate body, 25... Thin plate.

Claims (2)

【特許請求の範囲】[Claims] (1)両端に一対の電極部を有した放電管内部に金属レ
ーザ媒質を配置し、前記放電管内部を放電により高温状
態として前記媒質を蒸気化してレーザ発振を行う金属蒸
気レーザ発振装置において、前記電極部が、放電管の端
部に連結された電極と、この電極に耐熱性を有する熱絶
縁物を介して固定された板体と、前記電極と板体を電気
的に接続する導電性部材とから構成されることを特徴と
する金属蒸気レーザ発振装置。
(1) A metal vapor laser oscillation device in which a metal laser medium is disposed inside a discharge tube having a pair of electrode portions at both ends, and the inside of the discharge tube is brought into a high temperature state by discharge to vaporize the medium and perform laser oscillation, The electrode part includes an electrode connected to an end of the discharge tube, a plate fixed to the electrode via a heat-resistant thermal insulator, and a conductive member that electrically connects the electrode and the plate. A metal vapor laser oscillation device comprising:
(2)前記導電性部材が薄状板又は放射状のワイヤであ
ることを特徴とする特許請求の範囲第1項記載の金属蒸
気レーザ発振装置。
(2) The metal vapor laser oscillation device according to claim 1, wherein the conductive member is a thin plate or a radial wire.
JP7161287A 1987-03-27 1987-03-27 Metal vapor laser oscillator Pending JPS63239881A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP7161287A JPS63239881A (en) 1987-03-27 1987-03-27 Metal vapor laser oscillator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7161287A JPS63239881A (en) 1987-03-27 1987-03-27 Metal vapor laser oscillator

Publications (1)

Publication Number Publication Date
JPS63239881A true JPS63239881A (en) 1988-10-05

Family

ID=13465645

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7161287A Pending JPS63239881A (en) 1987-03-27 1987-03-27 Metal vapor laser oscillator

Country Status (1)

Country Link
JP (1) JPS63239881A (en)

Similar Documents

Publication Publication Date Title
JPH03505506A (en) Integrated solid state laser
JPS63239881A (en) Metal vapor laser oscillator
JP2725493B2 (en) Air-cooled argon ion laser tube
US5777437A (en) Annular chamber flashlamp including a surrounding, packed powder reflective material
US5113407A (en) Discharge tube for laser oscillator
JPS63239882A (en) Metal vapor laser
JPH03237777A (en) Metal vapor laser equipment
JPS6226877A (en) Metal vapor laser oscillation tube
JPS62595B2 (en)
JPH02281773A (en) Metal vapor laser oscillating tube
JPS5918695Y2 (en) ion laser tube
JPH01238079A (en) Metallic vapor laser equipment
JPS62159483A (en) Metallic vapor laser oscillation device
JPH07307505A (en) Gas laser device
JPH02148777A (en) Metal vapor laser oscillation tube
JPS5839082A (en) Ion laser tube
JPH0317257A (en) Material vapor generator
JPS62242380A (en) Metallic vapor laser apparatus
JPH08293637A (en) Laser
JPS63239993A (en) Metal vapor laser device
JPH0231473A (en) Metal vapor laser apparatus
JPH03237778A (en) Metal vapor laser equipment
JPS62101092A (en) Metal vapor laser apparatus
JPH05243642A (en) Metal vapor laser equipment
JPH02281671A (en) Gas laser oscillation device