JPH04243174A - Ion laser tube - Google Patents

Ion laser tube

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Publication number
JPH04243174A
JPH04243174A JP359991A JP359991A JPH04243174A JP H04243174 A JPH04243174 A JP H04243174A JP 359991 A JP359991 A JP 359991A JP 359991 A JP359991 A JP 359991A JP H04243174 A JPH04243174 A JP H04243174A
Authority
JP
Japan
Prior art keywords
laser tube
laser
opening
cylindrical
tube
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
JP359991A
Other languages
Japanese (ja)
Inventor
Kenji Yamaguchi
山口 兼治
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.)
NEC Corp
Original Assignee
NEC 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 NEC Corp filed Critical NEC Corp
Priority to JP359991A priority Critical patent/JPH04243174A/en
Publication of JPH04243174A publication Critical patent/JPH04243174A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To prevent deterioration of a discharge base and a decrease in insulation by engaging a cylindrical member of alumina ceramic with a central opening of a disclike member. CONSTITUTION:A disclike member 7 has a central opening 10, and a cylindrical member 9 of alumina ceramic is forced into the hole 10. Further, the member 7 has a plurality of openings 11 around the opening 10. A discharge path 12 is formed on the axis of a laser tube with the opening formed by the inner wall of the member 9 of the ceramics engaged with the opening 10 of the member 7. The plurality of openings 11 form a gas return passage 13 for making gas between a cathode 2 and an anode 3 uniform. A cylindrical connecting member 8 is formed of aluminum nitride similarly to the member 7. Both are brought into close contact with one another with low melting point glass, and hermetically sealed therein. Further, a coolant passage is provided in the outside of the tube for forced cooling.

Description

【発明の詳細な説明】[Detailed description of the invention]

【0001】0001

【産業上の利用分野】本発明は、イオンレーザ管に関し
、特にレーザ細管の構造に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to ion laser tubes, and more particularly to the structure of laser tubes.

【0002】0002

【従来の技術】レーザ光線は指向性に優れ、エネルギー
密度の集中化が可能であるため、金属材料の加工,医療
機器,さらには光ファイバーによる通信等の幅広い分野
に応用されている。レーザ光源としては、一般にレーザ
媒質の形態により気体レーザ,液体レーザ,固体レーザ
が知られており、このうち気体レーザは放電励起された
気体原子あるいはイオン等からの放射光を光学系により
共振させてレーザ発振させるものである。
2. Description of the Related Art Laser beams have excellent directivity and can concentrate energy density, so they are applied to a wide range of fields such as processing of metal materials, medical equipment, and even communication using optical fibers. Generally, gas lasers, liquid lasers, and solid-state lasers are known as laser light sources, depending on the form of the laser medium. Among these, gas lasers use an optical system to resonate emitted light from discharge-excited gas atoms or ions. It causes laser oscillation.

【0003】気体レーザの一種であるアルゴンあるいは
クリプトン等のイオンレーザは可視,紫外領域で多数の
発振線が得られ、しかも高出力であるため、ホログラフ
ィ,ラマン分光をはじめとするレーザ分光さらには色素
レーザの励起用光源としての用途がある。イオンレーザ
は高出力であるが、レーザ発振時の放電電流密度が50
0A/cm2 にも達し、消費電力も放電管単位長当り
50W/cmと極めて大きい。このような放電条件下で
、気体放電を維持するレーザ細管も極めて高温度になる
ため、その材料には耐熱性に優れたものが要求される。 また、イオンレーザは上記の温度対策としてレーザ細管
の外周部に冷却水路を配設しているが、その冷却効果を
向上させるためのレーザ細管自身の優れた伝導性も要求
されている。
Ion lasers such as argon or krypton, which are a type of gas laser, can obtain many oscillation lines in the visible and ultraviolet regions, and have high output, so they can be used for laser spectroscopy such as holography, Raman spectroscopy, and even pigmentation. It is used as a light source for laser excitation. Ion lasers have high output, but the discharge current density during laser oscillation is 50
The power consumption reaches 0A/cm2, and the power consumption is extremely high at 50W/cm per unit length of the discharge tube. Under such discharge conditions, the temperature of the laser tube that maintains the gas discharge becomes extremely high, so the material used therefor must have excellent heat resistance. In addition, in the ion laser, a cooling channel is provided on the outer periphery of the laser tube as a countermeasure against the above-mentioned temperature, but the laser tube itself is also required to have excellent conductivity in order to improve its cooling effect.

【0004】従来、上記要求に応え得るイオンレーザ管
として、陽極および陰極間に配置されるレーザ細管に円
筒状の電気的に絶縁性を有し且つ熱伝導性に優れたBe
O(ベリリア),AlN(窒化アルミニウム)等を用い
たものが知られている。また、レーザ細管の放電路およ
び外囲器の一部が、グラファイト製の円板状部材と筒状
の絶縁性部材とをレーザ管の軸方向に交互に連接して構
成されたイオンレーザ管も知られている。
Conventionally, as an ion laser tube that can meet the above requirements, a cylindrical Be material having electrically insulating properties and excellent thermal conductivity is used as a laser tube disposed between an anode and a cathode.
Those using O (beryria), AlN (aluminum nitride), etc. are known. In addition, there is also an ion laser tube in which the discharge path and part of the envelope of the laser tube are constructed by alternately connecting graphite disk-shaped members and cylindrical insulating members in the axial direction of the laser tube. Are known.

【0005】[0005]

【発明が解決しようとする課題】上記した円筒状セラミ
ックスのレーザ細管では、セラミックス材料に窒化アル
ミニウムを用いた場合、レーザ細管内に発生するプラズ
マによって放電路壁がスパッタされる結果、窒化アルミ
ニウムの分解に起因する窒素ガスが発生する問題があっ
た。又ベリリアにおいては公害物質で取扱いが厄介で且
つ高価である問題があった。
[Problems to be Solved by the Invention] In the above-mentioned cylindrical ceramic laser tube, when aluminum nitride is used as the ceramic material, the discharge channel wall is sputtered by the plasma generated in the laser tube, resulting in decomposition of the aluminum nitride. There was a problem that nitrogen gas was generated due to Also, beryllia has the problem of being a polluting substance, difficult to handle, and expensive.

【0006】一方、グラファイト製の円板状部材と絶縁
性部材とを連接したイオンレーザ管においても、放電路
壁のグラファイトがスパッタされ、スパッタされたグラ
ファイトの粉末が陰極および陽極間の絶縁劣化を引き起
すという問題があった。上記の窒素ガスまたはグラファ
イト粉末による問題が生じると、レーザ管は良好な放電
状態を維持できず、しだいにレーザ光出力が低下し、つ
いにはレーザ発振しなくなるという欠点があった。
On the other hand, even in an ion laser tube in which a disc-shaped graphite member and an insulating member are connected, the graphite on the discharge channel wall is sputtered, and the sputtered graphite powder deteriorates the insulation between the cathode and anode. There was a problem with causing it. When the above-mentioned problems caused by nitrogen gas or graphite powder occur, the laser tube cannot maintain a good discharge state, the laser light output gradually decreases, and finally the laser oscillates no longer.

【0007】一方、ベリリアは上記問題については解決
してくれるが、公害物質で取扱いが厄介で且つ高価であ
る問題を抱えている。これら両者の問題を解決し、取扱
いが容易で且つ安価であるとともにレーザ管の寿命をさ
らに延ばす優れた性能のイオンレーザ管が要望されてい
る。
On the other hand, although beryllia solves the above problems, it has the problem of being a polluting substance, difficult to handle, and expensive. There is a need for an ion laser tube that solves both of these problems, is easy to handle, is inexpensive, and has excellent performance that further extends the life of the laser tube.

【0008】[0008]

【課題を解決するための手段】本発明は、中央に放電路
となる開孔を備えるセラミックスの円板状部材とセラミ
ックス製の筒状接続部材とを交互に接続してレーザ細管
部を構成し、その両側に陽極および陰極を設けたイオン
レーザ管において、円板状部材の中央開孔にアルミナセ
ラミックスの筒状部材を嵌着したことを特徴とする。
[Means for Solving the Problems] The present invention constitutes a laser thin tube section by alternately connecting ceramic disc-shaped members with an opening in the center that serves as a discharge path and ceramic cylindrical connecting members. , an ion laser tube having an anode and a cathode on both sides thereof, characterized in that a cylindrical member made of alumina ceramics is fitted into a central opening of a disc-shaped member.

【0009】[0009]

【実施例】次に本発明について図面を参照して詳細に説
明する。図1は、本発明の水冷型イオンレーザ管の一実
施例の断面図を示す。本発明のレーザ管は、コイル状陰
極4を収容するレーザ管陰極部2と、円筒状陽極5を収
容するレーザ管陽極部3と、レーザ管陰極部2および陽
極部3に挟まれたレーザ管中央部1とから主に構成され
ている。レーザ管陰極部2および陽極部3はガラス材料
を成形,加工したものであり、それぞれレーザ管の軸上
であって端部側壁にブリュースタ窓6を装着している。
DESCRIPTION OF THE PREFERRED EMBODIMENTS Next, the present invention will be explained in detail with reference to the drawings. FIG. 1 shows a cross-sectional view of an embodiment of a water-cooled ion laser tube of the present invention. The laser tube of the present invention includes a laser tube cathode section 2 that accommodates a coiled cathode 4, a laser tube anode section 3 that accommodates a cylindrical anode 5, and a laser tube that is sandwiched between the laser tube cathode section 2 and the anode section 3. It is mainly composed of a central part 1. The laser tube cathode section 2 and anode section 3 are formed and processed from a glass material, and each has a Brewster window 6 mounted on the end side wall on the axis of the laser tube.

【0010】レーザ管中央部1は、レーザ管軸方向に窒
化アルミニウム製の円板状部材7および筒状接続部材8
を交互にかつ同軸状に連接した構造を有する。各々の円
板状部材7は中央開孔10を有し、中央開孔10にアル
ミナセラミックス製の筒状部材9が密着して嵌合されて
いる。さらに各々の円板状部材7は中央開孔10の周り
に複数の開孔11を有している。円板状部材7の中央開
孔10に嵌合されたアルミナセラミックス製の筒状部材
9の内側壁によって構成される開孔はレーザ管の軸上に
放電路12を形成している。また、複数の開孔11は、
陰極部2と陽極部3との間のガス圧を均一にするための
ガス帰還路13を形成している。
The central portion 1 of the laser tube includes a disc-shaped member 7 made of aluminum nitride and a cylindrical connecting member 8 in the axial direction of the laser tube.
It has a structure in which these are connected alternately and coaxially. Each disc-shaped member 7 has a central opening 10, into which a cylindrical member 9 made of alumina ceramics is tightly fitted. Furthermore, each disc-shaped member 7 has a plurality of apertures 11 around the central aperture 10. The aperture formed by the inner wall of the alumina ceramic cylindrical member 9 fitted into the central aperture 10 of the disc-shaped member 7 forms a discharge path 12 on the axis of the laser tube. Moreover, the plurality of openings 11 are
A gas return path 13 is formed to equalize the gas pressure between the cathode section 2 and the anode section 3.

【0011】筒状接続部材8は円板状部材7と同様に窒
化アルミニウムで作製しており、両者は互いに低融点ガ
ラスにより密着され内部を気密に維持している。さらに
図示を省略したが、レーザ管の外側には冷却水路が設け
られ強制冷却可能に構成されている。レーザ細管材料は
、電気的に絶縁性を有し、熱伝導性、耐スパッタ性に優
れていることが要求されていることは上記した通りであ
る。
The cylindrical connecting member 8 is made of aluminum nitride similarly to the disc-shaped member 7, and both are closely adhered to each other with low melting point glass to maintain an airtight interior. Further, although not shown in the drawings, a cooling channel is provided on the outside of the laser tube to enable forced cooling. As described above, the laser tube material is required to have electrical insulation, excellent thermal conductivity, and sputter resistance.

【0012】レーザ細管材料にアルミナセラミックスを
選択した理由は、Arイオンを照射して耐スパッタ性を
イオンシニング方法にてベリリアと比較した場合、スパ
ッタ孔断面積〔×103 μm2 〕,スパッタ孔深さ
〔μm〕等においてベリリアと遜色なく且つ無害物質で
安価である特長を有しているからである。一方、熱伝導
性においてはベリリアに比べて約一桁程度アルミナセラ
ミックスの方が劣っており、動作時の温度勾配を小さく
してやる必要があるので、極力肉厚を薄くしてやるなど
の配慮が必要であることは言うまでもない。
[0012] The reason why alumina ceramics was selected as the laser tube material is that when Ar ion irradiation is performed and the sputter resistance is compared with beryllia using the ion thinning method, the sputter hole cross-sectional area [×103 μm2] and the sputter hole depth are This is because it is comparable to beryllia in terms of size [μm], etc., and is a harmless substance and inexpensive. On the other hand, in terms of thermal conductivity, alumina ceramics is about an order of magnitude inferior to beryllia, and it is necessary to reduce the temperature gradient during operation, so consideration must be given to making the wall thickness as thin as possible. Needless to say.

【0013】[0013]

【発明の効果】以上説明したように本発明のイオンレー
ザ管は、プラズマが直接接する放電路をアルミナセラミ
ックス部材で形成しているため、従来問題とされていた
放電気体の劣化および絶縁性低下を防止することができ
る。従って、本発明はレーザ管の寿命を大幅に延ばすこ
とができ、その工業的価値は極めて高い。
[Effects of the Invention] As explained above, in the ion laser tube of the present invention, since the discharge path in direct contact with plasma is formed of an alumina ceramic member, deterioration of the discharge body and decrease in insulation, which have been problems in the past, can be avoided. It can be prevented. Therefore, the present invention can significantly extend the life of the laser tube, and its industrial value is extremely high.

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

【図1】本発明のイオンレーザ管の一実施例の断面図で
ある。
FIG. 1 is a cross-sectional view of an embodiment of an ion laser tube of the present invention.

【符号の説明】[Explanation of symbols]

1    レーザ管中央部 2    レーザ管陰極部 3    レーザ管陽極部 4    陰極 5    陽極 6    ブリュースタ窓 7    円板状部材 8    筒状接続部材 9    アルミナセラミックス製筒状部材10   
 中央開孔 11    開孔 12    放電路 13    ガス帰還路
1 Laser tube central portion 2 Laser tube cathode portion 3 Laser tube anode portion 4 Cathode 5 Anode 6 Brewster window 7 Disk-shaped member 8 Cylindrical connection member 9 Alumina ceramics cylindrical member 10
Central opening 11 Opening 12 Discharge path 13 Gas return path

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】  中央に放電路となる開孔を備えるセラ
ミックス製の円板状部材とセラミックス製の筒状接続部
材とを交互に接続してレーザ細管部を構成し、その両側
に陽極および陰極を設けたイオンレーザ管において、円
板状部材の各々の中央開孔部にアルミナセラミックスの
筒状部材を嵌着したことを特徴とするイオンレーザ管。
Claim 1: A laser capillary section is constructed by alternately connecting a ceramic disc-shaped member with an aperture serving as a discharge path in the center and a ceramic cylindrical connecting member, and an anode and a cathode are arranged on both sides of the laser capillary section. 1. An ion laser tube comprising: an alumina ceramic cylindrical member fitted into the central opening of each disc-shaped member.
JP359991A 1991-01-17 1991-01-17 Ion laser tube Pending JPH04243174A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP359991A JPH04243174A (en) 1991-01-17 1991-01-17 Ion laser tube

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP359991A JPH04243174A (en) 1991-01-17 1991-01-17 Ion laser tube

Publications (1)

Publication Number Publication Date
JPH04243174A true JPH04243174A (en) 1992-08-31

Family

ID=11561950

Family Applications (1)

Application Number Title Priority Date Filing Date
JP359991A Pending JPH04243174A (en) 1991-01-17 1991-01-17 Ion laser tube

Country Status (1)

Country Link
JP (1) JPH04243174A (en)

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