JPH03109784A - Gas laser oscillator - Google Patents

Gas laser oscillator

Info

Publication number
JPH03109784A
JPH03109784A JP24641189A JP24641189A JPH03109784A JP H03109784 A JPH03109784 A JP H03109784A JP 24641189 A JP24641189 A JP 24641189A JP 24641189 A JP24641189 A JP 24641189A JP H03109784 A JPH03109784 A JP H03109784A
Authority
JP
Japan
Prior art keywords
cathode
tube
anode
insulation
laser oscillator
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
JP24641189A
Other languages
Japanese (ja)
Inventor
Tomotaka Miyazaki
友孝 宮崎
Saburo Sato
三郎 佐藤
Shinji Okuma
慎治 大熊
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 JP24641189A priority Critical patent/JPH03109784A/en
Publication of JPH03109784A publication Critical patent/JPH03109784A/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
    • H01S3/038Electrodes, e.g. special shape, configuration or composition

Abstract

PURPOSE:To improve resistance against earthquake and insulation characteristics of an insulation tube to stabilize laser oscillation by constituting a cathode of a pair of electrode rods, an insulation plate provided on one side of the cathode rods and a trigger steel plate provided between the cathode rods on the other side. CONSTITUTION:A cathode 10 and an anode 3 are placed in parallel inside an arc tube 1 while an insulation tube 4a is placed on a surface facing the anode 3. The cathode 10 is constituted of a pair of electrode rods 10a, 10b, an insulating plate 10c provided on one side of the electrode rods, and a trigger steel plate 2b provided between the electrode rods on the other side. That is, the insulation tube 4a is fixed to the insulation plate 10c while the insulation tube 4a is made outside a region of glow discharge. Thus resistance against earthquake and insulation property can be improved and stable laser oscillation can be performed as well.

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、ガスレーザ発振器に関する。[Detailed description of the invention] [Purpose of the invention] (Industrial application field) The present invention relates to a gas laser oscillator.

(従来の技術) 従来のガスレーザ発振器の一例を示す第4図において、
電源8に電源側が接続されたパルス電源6の負荷側には
、負電圧側に陰極2が、他側に陽8i!3がそれぞれ接
続されている。
(Prior Art) In FIG. 4 showing an example of a conventional gas laser oscillator,
On the load side of the pulse power supply 6 whose power supply side is connected to the power supply 8, the cathode 2 is connected to the negative voltage side and the positive electrode 8i! is connected to the other side. 3 are connected to each other.

このうち、陰極2の陽極3との対置面には、同図紙面直
交方向に長いV字状の複数の溝2aが形成され、この溝
2aの内側には、軸心に芯線4bが設けられたガラス管
4aでなるトリガ電極4がそれぞれ設けられ、ガラス管
4aの両端は図示しない取付具で陰極2の端部に支えら
れ、芯線4bは陽極3に接続されている。
Among these, a plurality of long V-shaped grooves 2a are formed on the surface of the cathode 2 facing the anode 3 in a direction perpendicular to the plane of the figure, and a core wire 4b is provided at the axis inside the grooves 2a. Trigger electrodes 4 each made of a glass tube 4a are provided, both ends of the glass tubes 4a are supported by the ends of the cathode 2 with fixtures (not shown), and the core wire 4b is connected to the anode 3.

又、陰極2と陽極3との間には、これらと並列にピーキ
ングコンデンサ5が接続されて、このピーキングコンデ
ンサ5と陰極2、陽極3とトリガ電極4は、同図紙面直
交方向に長い筒状の放電管1内に設けられて、この放電
管1内には更にガスレーザ媒質としてのガスが封入され
ている。
A peaking capacitor 5 is connected in parallel between the cathode 2 and anode 3, and the peaking capacitor 5 and the cathode 2, as well as the anode 3 and the trigger electrode 4, have a long cylindrical shape in the direction perpendicular to the plane of the drawing. The discharge tube 1 is provided in a discharge tube 1, and a gas as a gas laser medium is further sealed inside the discharge tube 1.

さて、このように構成されたガスレーザ発振器において
は、パルス電源6で発生された電圧パルスは、ピーキン
グコンデンサ5に充電され、この充電された電荷の放電
で陰極2の溝2aの表面と芯線4bとの間でコロナ放電
が発生して、溝2aの表面近傍が予備電離状態となる。
Now, in the gas laser oscillator configured in this way, the voltage pulse generated by the pulse power source 6 charges the peaking capacitor 5, and the discharge of this charged charge causes the surface of the groove 2a of the cathode 2 and the core wire 4b to connect. A corona discharge occurs between the grooves 2a, and the vicinity of the surface of the groove 2a becomes pre-ionized.

続いて、陰極2と陽極3との間が放電開始電圧になると
、陰極2と陽極3間で主放電としてのグロー放電となっ
て、放電管1内のレーザガスは励起され、レーザ光が放
出される。
Subsequently, when the discharge starting voltage is reached between the cathode 2 and anode 3, a glow discharge as a main discharge occurs between the cathode 2 and anode 3, the laser gas in the discharge tube 1 is excited, and laser light is emitted. Ru.

ところが、このように構成されたレーザ発振器では、ト
リガ電極4が溝2aの表面近傍に設けられているので、
効率よく予備放電を発生させることはできるが、陰極2
の主放電領域内に位置しているので、ガラス管4aはグ
ロー放電で表面が汚れて沿面耐電値が落ちてくる。
However, in the laser oscillator configured in this way, since the trigger electrode 4 is provided near the surface of the groove 2a,
Although preliminary discharge can be generated efficiently, the cathode 2
Since the glass tube 4a is located within the main discharge area, the surface of the glass tube 4a becomes dirty due to the glow discharge and the creeping electric strength value decreases.

又、もし、何らかの原因でグロー放電が不安定になって
、瞬間的なアーク放電に移行すると、ガラス管4aが破
損するおそれもある。
Furthermore, if the glow discharge becomes unstable for some reason and shifts to an instantaneous arc discharge, there is a risk that the glass tube 4a may be damaged.

更に、トリガ電極4の芯線4bは折れ易いのでトリガ電
極4の固定が弱いと振動で折損するおそれもある。
Furthermore, since the core wire 4b of the trigger electrode 4 is easily broken, if the trigger electrode 4 is not firmly fixed, there is a risk of it being broken due to vibration.

そこで、第5図に示すレーザ発振器が考えられる。Therefore, a laser oscillator shown in FIG. 5 can be considered.

同図において、陰極9は開口側が陽極3側に向いた逆U
字状になっていて、このU字状の四部9a内には、トリ
ガ電極4がその部分詳細図を示す第6図のように、凹部
9aの底に近接して設けられ、凹部9aの開口端には、
小さい穴2b1が隣接して設けられた網状のトリガ鋼板
2bが取付られている。
In the figure, the cathode 9 is an inverted U with the opening side facing the anode 3 side.
The trigger electrode 4 is provided in the four U-shaped parts 9a close to the bottom of the recess 9a, as shown in FIG. At the end,
A net-like trigger steel plate 2b with adjacent small holes 2b1 is attached.

このように構成されたレーザ発振器では、予備放電は、
芯線4bと四部9aの底面及びトリガ網板2bの間で発
生し、主放電は、トリガ鋼板2bと陽極3の間で発生す
るので、主放電時にはガラス管4aは放電領域の範囲外
となる。
In a laser oscillator configured in this way, the preliminary discharge is
The main discharge occurs between the core wire 4b, the bottom surface of the four parts 9a, and the trigger mesh plate 2b, and the main discharge occurs between the trigger steel plate 2b and the anode 3, so the glass tube 4a is outside the discharge area during the main discharge.

ところが、このように構成されたレーザ発振器では、発
明者らの実験結果では、予備放電量が不足して主放電へ
の移行がまだ不安定であった。
However, in the laser oscillator configured as described above, according to the experimental results of the inventors, the preliminary discharge amount was insufficient and the transition to the main discharge was still unstable.

そこで本発明の目的は、耐震性と絶縁耐力を上げ、安定
したレーザ発振を行うことのできるガスレーザ発振器を
得ることである。
Therefore, an object of the present invention is to obtain a gas laser oscillator that has improved earthquake resistance and dielectric strength and can perform stable laser oscillation.

[発明の構成] (課題を解決するための手段と作用) 本発明は、放電管内に陰極と陽極が平行に対置され、陰
極の陽極との対置面に平行に芯線を内蔵した絶縁管が対
置されたガスレーザ発振器において、陰極を、一対の電
極棒とこの陰極棒の片側面に設けられた絶縁板と陰極棒
の他側間に設けられたトリガ鋼板で構成することで1、
絶縁管の耐震性と絶縁特性を上げレーザ発振を安定化し
たガスレーザ発振器である。
[Structure of the Invention] (Means and Effects for Solving the Problems) The present invention is characterized in that a cathode and an anode are placed parallel to each other in a discharge tube, and an insulated tube with a built-in core wire is placed parallel to the surface of the cathode facing the anode. In the gas laser oscillator, the cathode is composed of a pair of electrode rods, an insulating plate provided on one side of the cathode rods, and a trigger steel plate provided between the other side of the cathode rods.
This is a gas laser oscillator that stabilizes laser oscillation by improving the earthquake resistance and insulation properties of the insulating tube.

(実施例) 以下、本発明のガスレーザ発振器の一実施例を図面を参
照して説明する。但し、第4〜6図と重複する場合は省
く。
(Example) Hereinafter, an example of the gas laser oscillator of the present invention will be described with reference to the drawings. However, if it overlaps with Figures 4 to 6, it will be omitted.

第1図において、陰極IOだけが従来と異なっている。In FIG. 1, only the cathode IO is different from the conventional one.

すなわち、陰極IOは、左右に平行に対置された断面略
三角形の電極棒10a、 lObと、この電極棒10a
、 10bの上端間に両側の電極棒10bと結合して設
けられた短冊板状の絶縁板10cと、左右の電極棒10
a、10bの下端間に電極棒10bと結合され絶縁板1
0cと対置して設けられトリガ電極4を絶縁板10c間
に挟んだトリガ綱板2bで構成している。
That is, the cathode IO consists of electrode rods 10a and 1Ob having a substantially triangular cross section, which are arranged parallel to each other on the left and right, and the electrode rods 10a.
, a rectangular insulating plate 10c connected to the electrode rods 10b on both sides between the upper ends of the electrode rods 10b, and the electrode rods 10 on the left and right sides.
The insulating plate 1 is connected to the electrode rod 10b between the lower ends of the electrodes a and 10b.
0c, the trigger electrode 4 is constituted by a trigger wire plate 2b sandwiched between insulating plates 10c.

このように構成されたレーザ発振−器では、ガラク管4
aは、トリガ網板2bと絶縁板10cとで上下方向から
挟まれているので機械的に強固に固定できるのでもし、
この発振器が車両などに搭載されても振動でずれること
はない。
In the laser oscillator configured in this way, the galac tube 4
Since a is sandwiched from above and below between the trigger net plate 2b and the insulating plate 10c, it can be mechanically fixed firmly.
Even if this oscillator is mounted on a vehicle, it will not shift due to vibration.

更に、トリガ網板2bの裏側に位置しているので、トリ
ガ鋼板2bと陽極3とのグロー放電にさらされないので
、放電で表面は劣化せず、もし、万一陰極lOと陽極3
間がアーク放電に移行しても、これ又、アークにさらさ
れることがない。
Furthermore, since it is located on the back side of the trigger mesh plate 2b, it is not exposed to the glow discharge between the trigger steel plate 2b and the anode 3, so the surface will not deteriorate due to discharge, and in the event that the cathode lO and anode 3
Even if the interval shifts to arc discharge, there is no exposure to arc.

又、第1図及び第1図の要部を示す第2図において、ピ
ーキングコンデンサ5に充電された電荷の放電ルートは
、芯線4bとトリガ網板2b間の第2図で示す電界E方
向だけとなるので、第5図、第6図で示す電界E1+E
2方向にトリガ網板2bと陰極9とに分流する場合に比
べて、放電電荷量は約2倍に増やすことができるので、
グロー放電への移行をスムーズに行うことができ、レー
ザ発振が安定する。
In addition, in FIG. 1 and FIG. 2 showing the main part of FIG. 1, the discharge route of the charge charged in the peaking capacitor 5 is only in the direction of the electric field E shown in FIG. 2 between the core wire 4b and the trigger screen plate 2b. Therefore, the electric field E1+E shown in FIGS. 5 and 6
Compared to the case where the current is split in two directions between the trigger mesh plate 2b and the cathode 9, the amount of discharged charge can be approximately doubled, so
The transition to glow discharge can be performed smoothly, and laser oscillation is stabilized.

更に、陰極10の断面形状は、電極棒LOa、 10b
と絶縁板10cとトリガ網板2bとで箱状となるので、
震動で変形しない高剛性の構造となる。
Furthermore, the cross-sectional shape of the cathode 10 is as follows: electrode rods LOa, 10b
Since the insulating plate 10c and the trigger mesh plate 2b form a box shape,
It has a highly rigid structure that does not deform due to vibrations.

因みに、第2図と第6図において、ガラス管4aの誘電
率をε、同じく長さをΩ、内径をaと、外径をbとする
と、芯線4bとガラス管4a表面内の等価容ff1Cは
、同心円筒コンデンサと仮定して、となり、これに見合
った電流が第2図では芯線4bとトリガ網板2b間に流
れることになるので、第2図の場合は第6図に比べて鋼
板2bに流れる電荷量は2倍となる。
Incidentally, in FIGS. 2 and 6, if the permittivity of the glass tube 4a is ε, the length is Ω, the inner diameter is a, and the outer diameter is b, the equivalent volume between the core wire 4b and the surface of the glass tube 4a is ff1C. is assumed to be a concentric cylindrical capacitor, and a current commensurate with this will flow between the core wire 4b and the trigger mesh plate 2b in Fig. 2, so the steel plate in Fig. 2 is smaller than that in Fig. 6. The amount of charge flowing to 2b is doubled.

第3図は、本発明のガスレーザ発振器の他の実施例を示
す。
FIG. 3 shows another embodiment of the gas laser oscillator of the present invention.

同図においては、ガラス管7は断面長円形で、芯線7は
短冊板状となっている。この場合には、放電電極面積が
増えるので、予備放電の発生が更に容易となる利点があ
る。
In the figure, the glass tube 7 has an oval cross section, and the core wire 7 has a rectangular plate shape. In this case, since the area of the discharge electrode increases, there is an advantage that preliminary discharge can be generated more easily.

又、上記実施例では、芯線の外周をガラス管としたが、
アルミナ、ベリリヤ、ジルコニヤ、マイカ、ちり化アル
ミニウム、炭化シリコンなど耐熱性、耐アーク性絶縁材
料であればそれにしてもよい。
In addition, in the above embodiment, the outer periphery of the core wire was made of a glass tube, but
Any heat-resistant, arc-resistant insulating material such as alumina, beryllia, zirconia, mica, aluminum dust, or silicon carbide may be used.

[発明の効果コ 以上、本発明によれば、放電管の内部に陰極と陽極が平
行に対置され、陰極の陽極との対置面に平行に芯線が内
蔵された絶縁管が対置されたガスレーザ発振器において
、陰極を、一対の電極棒とこの電極棒の片側間に設けら
れた絶縁板と、電極棒間の他側に設けられたトリガ鋼板
で構成することで、絶縁管を絶縁板に固定し、かつ、絶
縁管をグロー放電の領域の外としたので、耐震性と絶縁
特性を上げ、安定したレーザ発振を行うことのできるガ
スレーザ発振器を得ることができる。
[Effects of the Invention] According to the present invention, there is provided a gas laser oscillator in which a cathode and an anode are placed parallel to each other inside a discharge tube, and an insulating tube with a built-in core wire is placed parallel to the surface of the cathode facing the anode. In this method, the cathode is composed of a pair of electrode rods, an insulating plate provided between one side of the electrode rods, and a trigger steel plate provided on the other side between the electrode rods, and the insulating tube is fixed to the insulating plate. Moreover, since the insulating tube is placed outside the glow discharge area, it is possible to obtain a gas laser oscillator that has improved earthquake resistance and insulation properties and can perform stable laser oscillation.

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

第1図は本発明のガスレーザ装置の一実施例を示す図、
第2図は第1図の要部を示す断面図、第3図は本発明の
ガスレーザ装置の他の実施例を示す図、第4図は従来の
ガスレーザ装置を示す図、第5図は第4図と異なる従来
のガスレーザ装置を示す図、第6図は第5図の要部を示
す断面図である。 ・・放電管 3・・・陽極 4a・・・絶縁管 4b・・・芯線 9・・・陰極 (8733)
FIG. 1 is a diagram showing an embodiment of the gas laser device of the present invention,
2 is a sectional view showing the main part of FIG. 1, FIG. 3 is a view showing another embodiment of the gas laser device of the present invention, FIG. 4 is a view showing a conventional gas laser device, and FIG. 5 is a sectional view showing the main part of FIG. 4 is a diagram showing a conventional gas laser device different from FIG. 4, and FIG. 6 is a sectional view showing the main part of FIG. 5. ...Discharge tube 3...Anode 4a...Insulation tube 4b...Core wire 9...Cathode (8733)

Claims (1)

【特許請求の範囲】[Claims] 放電管内に陰極と陽極が平行に対置され、前記陰極の前
記陽極との対置面に平行に内部に芯線が設けられた絶縁
管が対置されたガスレーザ発振器において、前記陰極を
、電極棒とこの電極棒の片側面に設けられた絶縁板と、
前記電陰棒間の他側に設けられた網板で構成し、前記絶
縁管を、前記絶縁板と前記トリガ網板間に設けたことを
特徴とするガスレーザ発振器。
In a gas laser oscillator in which a cathode and an anode are placed parallel to each other in a discharge tube, and an insulated tube having a core wire provided inside is placed parallel to the surface of the cathode facing the anode, the cathode is connected to an electrode rod and the electrode. An insulating plate provided on one side of the rod,
A gas laser oscillator comprising a mesh plate provided on the other side between the negative bars, and the insulating tube is provided between the insulating plate and the trigger mesh plate.
JP24641189A 1989-09-25 1989-09-25 Gas laser oscillator Pending JPH03109784A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP24641189A JPH03109784A (en) 1989-09-25 1989-09-25 Gas laser oscillator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP24641189A JPH03109784A (en) 1989-09-25 1989-09-25 Gas laser oscillator

Publications (1)

Publication Number Publication Date
JPH03109784A true JPH03109784A (en) 1991-05-09

Family

ID=17148091

Family Applications (1)

Application Number Title Priority Date Filing Date
JP24641189A Pending JPH03109784A (en) 1989-09-25 1989-09-25 Gas laser oscillator

Country Status (1)

Country Link
JP (1) JPH03109784A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7306551B2 (en) 2002-12-13 2007-12-11 Matsushita Electric Industrial Co., Ltd. Tool exchange device and tool
JP2008172163A (en) * 2007-01-15 2008-07-24 Yamaha Motor Co Ltd Nozzle exchange unit and mounting machine with nozzle exchange unit

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US7306551B2 (en) 2002-12-13 2007-12-11 Matsushita Electric Industrial Co., Ltd. Tool exchange device and tool
US7452315B2 (en) 2002-12-13 2008-11-18 Panasonic Corporation Tool exchange device and tool
JP2008172163A (en) * 2007-01-15 2008-07-24 Yamaha Motor Co Ltd Nozzle exchange unit and mounting machine with nozzle exchange unit

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