JPH02194577A - Metal steam laser oscillation tube - Google Patents
Metal steam laser oscillation tubeInfo
- Publication number
- JPH02194577A JPH02194577A JP1184189A JP1184189A JPH02194577A JP H02194577 A JPH02194577 A JP H02194577A JP 1184189 A JP1184189 A JP 1184189A JP 1184189 A JP1184189 A JP 1184189A JP H02194577 A JPH02194577 A JP H02194577A
- Authority
- JP
- Japan
- Prior art keywords
- inner tube
- tube
- insulating material
- laser oscillation
- heat
- 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
Links
- 230000010355 oscillation Effects 0.000 title claims description 21
- 239000002184 metal Substances 0.000 title claims description 20
- 229910052751 metal Inorganic materials 0.000 title claims description 20
- MCMNRKCIXSYSNV-UHFFFAOYSA-N Zirconium dioxide Chemical compound O=[Zr]=O MCMNRKCIXSYSNV-UHFFFAOYSA-N 0.000 claims abstract description 25
- 239000011810 insulating material Substances 0.000 claims abstract description 21
- PNEYBMLMFCGWSK-UHFFFAOYSA-N aluminium oxide Inorganic materials [O-2].[O-2].[O-2].[Al+3].[Al+3] PNEYBMLMFCGWSK-UHFFFAOYSA-N 0.000 claims abstract description 11
- 239000000470 constituent Substances 0.000 abstract 2
- 229910052593 corundum Inorganic materials 0.000 abstract 1
- 229910001845 yogo sapphire Inorganic materials 0.000 abstract 1
- 239000012774 insulation material Substances 0.000 description 3
- 230000001681 protective effect Effects 0.000 description 3
- 230000002159 abnormal effect Effects 0.000 description 2
- 239000000919 ceramic Substances 0.000 description 2
- 230000005684 electric field Effects 0.000 description 2
- 239000003574 free electron Substances 0.000 description 2
- 238000009413 insulation Methods 0.000 description 2
- 239000002923 metal particle Substances 0.000 description 2
- 230000003287 optical effect Effects 0.000 description 2
- 238000009412 basement excavation Methods 0.000 description 1
- 239000004020 conductor Substances 0.000 description 1
- 229910052802 copper Inorganic materials 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000010292 electrical insulation Methods 0.000 description 1
- 230000005611 electricity Effects 0.000 description 1
- 229910052737 gold Inorganic materials 0.000 description 1
- 239000012212 insulator Substances 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 239000002245 particle Substances 0.000 description 1
- 230000002093 peripheral effect Effects 0.000 description 1
Landscapes
- Lasers (AREA)
Abstract
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管に関する。[Detailed description of the invention] [Purpose of the invention] (Industrial application field) The present invention relates to a metal vapor laser oscillator tube.
(従来の技術)
従来の金属レーザ発振管は、例えば第2図に示すように
構成されている。即ち、耐熱性に優れたセラミックから
成る内管1の両側には、軸方向に沿って内管1とほぼ同
じ径に形成された円筒状の陽極2と陰極3が配設され、
内管1、陽極2、陰極3の外周面には軸方向に沿って断
熱材4を充填した保護管5が配設されている。(Prior Art) A conventional metal laser oscillation tube is configured as shown in FIG. 2, for example. That is, on both sides of an inner tube 1 made of ceramic with excellent heat resistance, a cylindrical anode 2 and a cathode 3, which are formed to have approximately the same diameter as the inner tube 1 along the axial direction, are arranged.
A protective tube 5 filled with a heat insulating material 4 is disposed along the axial direction on the outer peripheral surfaces of the inner tube 1, anode 2, and cathode 3.
また、保護管5の外側には導電体から成る外管6a、6
bが配設されており、陽極2、陰極3、保護管5は外管
5a 、5bの両端で支持されている。また、外管6a
、6b間には、陽極2側と陰極3側とを電気的に分離
する絶縁管7が配設され、外管5a 、5bの両端部に
は、それぞれブリュースタ窓8a、8bが取付けられて
いる。、9はレーザ媒質である金属粒子(例えばAIJ
、 CIJ等)である。Further, on the outside of the protective tube 5, outer tubes 6a and 6 made of a conductor are provided.
b, and the anode 2, cathode 3, and protective tube 5 are supported at both ends of the outer tubes 5a and 5b. In addition, the outer tube 6a
, 6b is provided with an insulating tube 7 for electrically separating the anode 2 side and the cathode 3 side, and Brewster windows 8a, 8b are attached to both ends of the outer tubes 5a, 5b, respectively. There is. , 9 is a metal particle that is a laser medium (for example, AIJ
, CIJ, etc.).
従来の金属蒸気レーザ発振管は前記のように構成されて
おり、レーザ発掘を行うには先ず、内管1内をロータリ
ーポンプ(不図示)等により排気して高真空に保持し、
内管1内にHeやNe等の放電用バッファガスを供給す
る。そして、外管6a、5bを介して陽極2と陰極3間
に、高電圧パルスをパルス高電圧電源(不図示)から印
加することにより、陽11i2と陰極3間に放電プラズ
マ中なる金属蒸気を生成する。そして、この金属蒸気を
放電プラズマ中の自由電子により励起することによって
、その金属特有の波長の光を発光し、ブリュースタ窓8
a 、8bを通してその外側に配置される光共振器(不
図示)で増幅され、レーザ光どなってR,据される。A conventional metal vapor laser oscillation tube is constructed as described above, and in order to carry out laser excavation, the inside of the inner tube 1 is first evacuated using a rotary pump (not shown) or the like to maintain a high vacuum.
A discharge buffer gas such as He or Ne is supplied into the inner tube 1. Then, by applying a high voltage pulse from a pulsed high voltage power source (not shown) between the anode 2 and the cathode 3 via the outer tubes 6a and 5b, metal vapor in the discharge plasma is introduced between the anode 11i2 and the cathode 3. generate. By exciting this metal vapor with free electrons in the discharge plasma, light with a wavelength unique to the metal is emitted, and the Brewster window 8
The laser beam is amplified by an optical resonator (not shown) disposed outside of the laser beam R, through which the laser beam passes through a and 8b.
ところで、前記した従来の金属蒸気レーザ発振管では、
レーザ発振時に陽極2と陰極3間に高電圧を印加してプ
ラズマ放電を行うので、内管1内は1500℃程度の高
温になる。この時、内管1は両端が開放状態なので、内
管1内の熱は両端から外へ逃げるため、内管1内の温度
は中央部近傍より両端近傍方が低くなる。よって、レー
ザ発振時に、陽極2と陰極3間のh!i電に寄与する有
効な高温領域(約1500℃)は内管1内の中央部近傍
だけとなるので、有効な高温領域が狭くなり、効率の良
いレーザ出力を得ることができなかった。By the way, in the conventional metal vapor laser oscillation tube mentioned above,
During laser oscillation, a high voltage is applied between the anode 2 and the cathode 3 to generate plasma discharge, so the inside of the inner tube 1 reaches a high temperature of about 1500°C. At this time, since both ends of the inner tube 1 are open, the heat inside the inner tube 1 escapes from both ends, so that the temperature inside the inner tube 1 becomes lower near both ends than near the center. Therefore, during laser oscillation, h! between the anode 2 and the cathode 3. Since the effective high-temperature region (approximately 1500° C.) that contributes to i-electricity is only near the center of the inner tube 1, the effective high-temperature region becomes narrow, making it impossible to obtain efficient laser output.
このため、従来は第2図に示すように、断熱材4の中央
部近傍の厚さを両端近傍よりも薄くすることにより中央
部近傍の熱の逃げを大きくし、断熱材4の軸方向の熱伝
導が均一になるようにして、内管1内の温度の均一化を
図っていた。For this reason, conventionally, as shown in FIG. 2, by making the thickness near the center of the heat insulating material 4 thinner than near both ends, the escape of heat near the center is increased, and the thickness of the heat insulating material 4 in the axial direction is increased. The temperature inside the inner tube 1 was made uniform by making heat conduction uniform.
(発明が解決しようとする課題)
しかしながら、断熱材4の中央部近傍を薄くするとその
部分に空間10が形成されることになるので、レーザ発
振時に内管1内が高温になると、断熱材4から発生する
ガスが空間10内に溜まって異常放電が発生ずる恐れが
ある。(Problem to be Solved by the Invention) However, if the area near the center of the heat insulator 4 is made thinner, a space 10 will be formed in that area. There is a risk that the gas generated from the above may accumulate in the space 10 and cause abnormal discharge.
また、内管1内に溜まるガスの氾が増えると、ガスが対
流を起こし、ガスの熱伝導度と相まって断熱特性を損な
い、内管1内の中央部近傍の温度が上昇して内管1内の
温度の均一化を図ることができなくなる。Furthermore, when the amount of gas accumulated in the inner tube 1 increases, the gas causes convection, which, combined with the thermal conductivity of the gas, impairs the insulation properties, causing the temperature near the center of the inner tube 1 to rise. It becomes impossible to equalize the internal temperature.
本発明は上記した課題を解決する目的でなされ、内管内
の温度を略均−にして有効な高温領域を広くとり、効率
の良いレーザ出力を得ることができる金属蒸気レーザ発
振管を提供しようとするものである。The present invention has been made to solve the above-mentioned problems, and it is an object of the present invention to provide a metal vapor laser oscillation tube that can substantially equalize the temperature inside the inner tube, widen the effective high temperature region, and obtain efficient laser output. It is something to do.
[発明の構成]
(課題を解決するための手段)
前記した課題を解決するために本発明は、電極がその内
側又は両側に配設される内管の外周に、軸方向に沿って
断熱材が配設される金属蒸気レーザ発振管において、前
記内管の中央部側に配設される断熱材はアルミナを主成
分としてなり、前記内管の両端部側に配設される断熱材
はジルコニアを主成分としてなることを特徴とする。[Structure of the Invention] (Means for Solving the Problems) In order to solve the above-mentioned problems, the present invention provides a method in which a heat insulating material is provided along the axial direction on the outer periphery of the inner tube in which the electrodes are disposed inside or on both sides. In a metal vapor laser oscillation tube in which a metal vapor laser oscillation tube is provided, the heat insulating material provided at the center of the inner tube is mainly composed of alumina, and the heat insulating material provided at both ends of the inner tube is zirconia. It is characterized by having as a main component.
(作用)
本発明によれば、両端部側のジルコニアを主成分とする
断熱材は、中央部側のアルミナを主成分とする断熱材よ
り断熱特性が優れているので、内管の中央部近傍からの
熱の逃げが大きくなって温度上昇が抑制されて、内管内
の軸方向の温度が略均−になり、効率の良いレーザ出力
が得られる。(Function) According to the present invention, the heat insulating material mainly composed of zirconia on both end sides has better heat insulating properties than the heat insulating material mainly composed of alumina on the center side. The escape of heat from the inner tube is increased, the temperature rise is suppressed, the temperature in the axial direction within the inner tube becomes approximately equal, and efficient laser output can be obtained.
(実施例)
以下、本発明を図示の一実施例に基づいて詳細に説明す
る。尚、従来と同一部材には同一符号を付して説明する
。(Example) Hereinafter, the present invention will be described in detail based on an illustrated example. In addition, the same reference numerals are attached to the same members as in the conventional case for explanation.
第1図は本発明に係る金属蒸気レーザ発振管を示す概略
断面図である。この図に示すように、金属粒子(例えば
Au 、Cu等)9が内部に配置されるセラミックから
成る内管1の両端には円筒状のi極2ど陰極3が配設さ
れ、内管1、陽極2、陰極3の外側には略同心円状に保
護管5と外管6a、6bが配設されている。内管1、陽
極2、陰極3と保護管5との間には、中央部側にアルミ
ナ(A愛2o3″″′)を主成分とする断熱材4aが配
設され、両端部側にジルコニア(Zr02)を主成分と
する断熱材4bが配設されている。ジルコニアはアルミ
ナよりも断熱特性は優れているが、電気絶1揄性では劣
っている。FIG. 1 is a schematic sectional view showing a metal vapor laser oscillation tube according to the present invention. As shown in this figure, a cylindrical i-electrode 2 and a cathode 3 are disposed at both ends of an inner tube 1 made of ceramic in which metal particles (for example, Au, Cu, etc.) 9 are arranged. , a protection tube 5 and outer tubes 6a and 6b are arranged approximately concentrically outside the anode 2 and cathode 3. Between the inner tube 1, the anode 2, the cathode 3, and the protection tube 5, a heat insulating material 4a mainly composed of alumina (Aai2o3'''') is provided in the center, and zirconia is provided in both ends. A heat insulating material 4b containing (Zr02) as a main component is provided. Zirconia has better thermal insulation properties than alumina, but is inferior in electrical insulation properties.
また、外管6a、6bは絶縁管7によって絶縁状態で接
続され、外管管6a 、6bの両端にはそれぞれブリュ
ースタ窓3a 、 8bが取付けられている。Further, the outer tubes 6a and 6b are connected in an insulated manner by an insulating tube 7, and Brewster windows 3a and 8b are attached to both ends of the outer tubes 6a and 6b, respectively.
本発明に係る金属蒸気レーザ発振管は蒸気のように構成
されており、レーザ発振を行う時には、内管1内をロー
タリーポンプ(不図示)の排気によって高真空に保持し
て、HeやNe等の放電用バッフ7ガスを供給する。そ
の後、陽極2と陰極3間に、パルス高電圧電源(不図示
)から高電圧パルスを外管6a 、6bを介して印加す
ることにより、陽極2と陰極3間に放電プラズマを発生
させて金属粒子8を蒸気化し、レーザ媒質となる金属蒸
気を生成する。ぞして、この金属蒸気を陽極2と陰極3
間に発生される放電プラズマ中の自由電子により励起し
、ブリュースタ窓8a、8bの外側に配設される光共振
器(不図示)で増幅して、レーザ光なって発振される。The metal vapor laser oscillation tube according to the present invention has a vapor-like structure, and when performing laser oscillation, the inside of the inner tube 1 is maintained at a high vacuum by exhausting with a rotary pump (not shown), and He, Ne, etc. The discharge buff 7 gas is supplied. Thereafter, a high voltage pulse is applied between the anode 2 and the cathode 3 from a pulsed high voltage power source (not shown) through the outer tubes 6a and 6b, thereby generating discharge plasma between the anode 2 and the cathode 3, and causing the metal to melt. The particles 8 are vaporized to generate metal vapor that becomes a laser medium. Then, this metal vapor is transferred to anode 2 and cathode 3.
It is excited by free electrons in the discharge plasma generated during this period, is amplified by an optical resonator (not shown) disposed outside the Brewster windows 8a and 8b, and is oscillated as a laser beam.
この時、内管1の両端部側に配設されているジルコニア
を主成分とする断熱材4bは中央部側に配設されるアル
ミナを主成分とする断熱材4aよりも断熱特性が優れて
いるので、内管1の中央部近傍からの熱の逃げが大きく
なって温度上昇が抑t++され、内管1内の温度は略均
−になる。At this time, the heat insulating material 4b mainly composed of zirconia disposed at both ends of the inner tube 1 has better heat insulating properties than the heat insulating material 4a mainly composed of alumina disposed at the center. Therefore, the escape of heat from the vicinity of the center of the inner tube 1 becomes large, the temperature rise is suppressed t++, and the temperature inside the inner tube 1 becomes approximately equal to -.
よって、レーザ発振時に陽極2と陰極3間の放電に寄与
する有効な高温領域が内管1の両端部近傍まで広がり、
高効率のレーザ発振を行うことができる。Therefore, the effective high-temperature region that contributes to the discharge between the anode 2 and the cathode 3 during laser oscillation extends to the vicinity of both ends of the inner tube 1,
Highly efficient laser oscillation can be performed.
また、陽極2と陰極3間にパルス高電圧が印加されると
、陽極2と陰極3の先端部に電場が集中して断熱材4b
@損匍させる恐れがあるが、断熱材4bに高温で電気伝
導性のあるジルコニアを用いたことにより、陽極2と陰
極3の先端部での電場が緩和されるので、断熱材4bの
野全が長くなる。Further, when a pulsed high voltage is applied between the anode 2 and the cathode 3, the electric field is concentrated at the tips of the anode 2 and the cathode 3, and the insulation material 4b
@Although there is a risk of damage, by using zirconia, which is electrically conductive at high temperatures, for the insulation material 4b, the electric field at the tips of the anode 2 and cathode 3 is relaxed, so the field of the insulation material 4b is becomes longer.
更に、断熱材4a 、4bにはガスが溜まる空間が形成
されていので、レーザ発振時に異常tIl電が起こるこ
とはない。Furthermore, since the heat insulating materials 4a and 4b have spaces in which gas accumulates, abnormal tIl electricity will not occur during laser oscillation.
尚、前記した実施例では、内管1の両端側に陽極2と陰
極3が配設されている金属蒸気シー11発振管であった
が、陽極2と陰極3が内管1内に配設される金属蒸気レ
ーザ発振管でも良い。In the above-mentioned embodiment, the metal vapor seam 11 oscillation tube has an anode 2 and a cathode 3 disposed at both ends of the inner tube 1, but an anode 2 and a cathode 3 are disposed inside the inner tube 1. A metal vapor laser oscillation tube may also be used.
[発明の効果]
以上、実施例に基づいて具体的に説明したように本発明
によれば、内管の外周の中央部側にはアルミナを主成分
とする断熱口を配設し、両端部側にはジルコニアを主成
分とする断熱材を配設したことによって内情の中央部近
傍からの熱の逃げが大きくなり、レーザ発振時に、内管
内の温度を略均−にして有効な高温領域を広くとること
ができるので、高効率で安定したレーザ発振時行うこと
ができる。[Effects of the Invention] As described above in detail based on the embodiments, according to the present invention, a heat insulating hole mainly composed of alumina is provided on the central part side of the outer periphery of the inner tube, and By arranging a heat insulating material mainly composed of zirconia on the side, the escape of heat from the vicinity of the center of the inner tube is increased, and during laser oscillation, the temperature inside the inner tube is approximately equalized and an effective high temperature area is created. Since it can be made wide, highly efficient and stable laser oscillation can be performed.
振管を示す概略断面図である。 It is a schematic sectional view showing a swing tube.
Claims (1)
方向に沿って断熱材が配設される金属蒸気レーザ発振管
において、前記内管の中央部側に配設される断熱材はア
ルミナを主成分としてなり、前記内管の両端部側に配設
される断熱材はジルコニアを主成分としてなることを特
徴とする金属蒸気レーザ発振管。In a metal vapor laser oscillation tube in which a heat insulating material is disposed along the axial direction on the outer periphery of an inner tube in which electrodes are disposed inside or on both sides, the heat insulating material is disposed on the center side of the inner tube. A metal vapor laser oscillation tube characterized in that the main component is alumina, and the heat insulating material provided at both ends of the inner tube is mainly zirconia.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1184189A JPH02194577A (en) | 1989-01-23 | 1989-01-23 | Metal steam laser oscillation tube |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1184189A JPH02194577A (en) | 1989-01-23 | 1989-01-23 | Metal steam laser oscillation tube |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH02194577A true JPH02194577A (en) | 1990-08-01 |
Family
ID=11788954
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP1184189A Pending JPH02194577A (en) | 1989-01-23 | 1989-01-23 | Metal steam laser oscillation tube |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH02194577A (en) |
-
1989
- 1989-01-23 JP JP1184189A patent/JPH02194577A/en active Pending
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