JPS58119689A - Gas laser tube which is continuously oscillated in lateral direction - Google Patents
Gas laser tube which is continuously oscillated in lateral directionInfo
- Publication number
- JPS58119689A JPS58119689A JP158882A JP158882A JPS58119689A JP S58119689 A JPS58119689 A JP S58119689A JP 158882 A JP158882 A JP 158882A JP 158882 A JP158882 A JP 158882A JP S58119689 A JPS58119689 A JP S58119689A
- Authority
- JP
- Japan
- Prior art keywords
- discharge
- electrode
- cathode electrode
- laser tube
- gas laser
- 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
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES 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
- H01S3/00—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
- H01S3/02—Constructional details
- H01S3/03—Constructional details of gas laser discharge tubes
- H01S3/038—Electrodes, e.g. special shape, configuration or composition
Landscapes
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Engineering & Computer Science (AREA)
- Plasma & Fusion (AREA)
- Optics & Photonics (AREA)
- Lasers (AREA)
Abstract
Description
【発明の詳細な説明】
この発明は、横方向放電を用いたレーザ管に関するもの
である。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a laser tube using lateral discharge.
連続発振の分子ガスレーザではレーザガスを冷却し、レ
ーザ作用に有効な分子数を増して大出力化をはかるため
、光軸に垂直にガスを流すことが行われる。この時、放
電は光軸に垂直でガス流と平行に行うか、両者にともに
垂直かの2つの場合がある。いずれの場合も光軸にそっ
て大面積で一様に放電させることが重要であ4このため
カソード電極を多数のビンに分割し、それぞれに安定抵
抗体をつけるのが普通である。In continuous wave molecular gas lasers, the gas is flowed perpendicular to the optical axis in order to cool the laser gas and increase the number of effective molecules for laser action, thereby increasing output. At this time, there are two cases: the discharge is perpendicular to the optical axis and parallel to the gas flow, or the discharge is perpendicular to both. In either case, it is important to uniformly discharge a large area along the optical axis.4For this reason, it is common practice to divide the cathode electrode into a number of bins and attach a stabilizing resistor to each bin.
従来の横方向放電分子ガスレーザでは、通常、第7図や
第2図に示すような構成をとっている。Conventional lateral discharge molecular gas lasers usually have a configuration as shown in FIG. 7 or FIG. 2.
すなわち、これらの図で、lはアノード電極、コは多数
植立されたビンで、カソード電極を構成している。3は
安定抵抗体で、各ビン2に直列に接続される。ダは電源
で、アノード電極lとビンコとの間に接続される。jは
レーザビーム、6はガス流、7は外囲器を示す。That is, in these figures, l is an anode electrode, and c is a large number of planted bottles, which constitute a cathode electrode. 3 is a stabilizing resistor, which is connected to each bin 2 in series. DA is a power supply, which is connected between the anode electrode l and the binco. j indicates the laser beam, 6 indicates the gas flow, and 7 indicates the envelope.
第1図はガス流乙の方向と放電の方向が同一の場合で、
パイプ状の7ノード電極lと紙面に垂直方向に多数並べ
たビン2との間で放電すム第λ図は放電方向とガス流乙
の方向が垂直な場合で、やはり板状(パイプ状にする場
合もある)のアノード電極lと多数のビンコとの間で放
電する。これらのピンコはいずれも安定抵抗体9を通し
て電源参につながっている。レーザの光軸は紙面に垂直
方向にあり、これにそってビンコは多数並んでいる。さ
らに、大出力の場合はこれが複数列となり数700本に
およぶ。Figure 1 shows the case where the direction of gas flow and the direction of discharge are the same.
Figure λ shows the case where the discharge direction is perpendicular to the direction of the gas flow between the pipe-shaped 7-node electrode 1 and a large number of bottles 2 arranged perpendicularly to the plane of the paper, and the plate-shaped (pipe-shaped) A discharge occurs between the anode electrode l of the battery (in some cases) and a large number of bins. All of these pins are connected to a power source through a stabilizing resistor 9. The optical axis of the laser is perpendicular to the plane of the paper, and many binos are lined up along this axis. Furthermore, in the case of high output, this becomes multiple rows, reaching up to several 700 lines.
この発明は上記の点に鑑みなされたもので、カソード電
極としてスパイラル状またはリング状の導体の線または
欅を用いることにより電極を少数化し、従って、製作が
容易で、しかも、放電の安定性の優れた横方向放電連続
発振ガスレーザ管を提供する目的でなされたものである
・以下、この発明について説明す、J0
第3図、第参図はこの発明のS4施例を示す側面図であ
る。これらの図でカッ−ド電極lはガス流乙に対する抵
抗を減らし乱流の発生を少なくシ、放電が一様になり、
アーク化がおさえられるようスパイラル状、リング状ま
たは半リング状に丸められる。カソード電極lは安定抵
抗体3を通じて電源参に接続する構成である。このカソ
ード電極tとアノード電極lとの間で放電し、レーザガ
スを励起する。大出力が必要な時には放電断面を大きく
することがしばしば必要となるが、この時数列のビン電
極を用いる代りに、本発明によるスパイラル電極tを用
いる・このようにすると広い範囲に安定に放電するため
、カソード電極lの数を大巾に減らすことができる。従
って、抵抗の数も減らすことができるので製作が容易に
なり経済的となる・さらに、複数個のスパイラル電極l
を一直線にせず、千鳥状に出し入れして配置すれば、放
電はさらに一様になるとともに、相互間の作用も減るた
め放電はより安定になる。This invention was made in view of the above points, and by using a spiral or ring-shaped conductor wire or zelkova as a cathode electrode, the number of electrodes is reduced, and therefore manufacturing is easy and the stability of discharge is improved. This invention was made for the purpose of providing an excellent lateral discharge continuous wave gas laser tube. This invention will be explained below. FIG. 3 is a side view showing an S4 embodiment of the invention. In these figures, the quad electrode 1 reduces the resistance to the gas flow, reduces the occurrence of turbulence, and makes the discharge uniform.
It is rolled into a spiral, ring, or half-ring shape to prevent arcing. The cathode electrode 1 is connected to a power source through a stabilizing resistor 3. A discharge is generated between the cathode electrode t and the anode electrode l to excite the laser gas. When a large output is required, it is often necessary to enlarge the discharge cross section, but instead of using a series of bottle electrodes, the spiral electrode t according to the present invention is used. In this way, stable discharge can be achieved over a wide range. Therefore, the number of cathode electrodes l can be greatly reduced. Therefore, the number of resistors can be reduced, making manufacturing easier and more economical.Furthermore, multiple spiral electrodes can be used.
If they are arranged in a staggered manner instead of in a straight line, the discharge becomes more uniform and the interaction between them is reduced, making the discharge more stable.
なお、カソード電極lのアノード電極/側の形状が主に
特性に影響するので、第1II!i!i7示のように、
半リング形にしてもよいことはもちろんである。この半
リング形の方が/ターンで線を太くした場合には製造が
容易である。同図では、上方からカソード電極tを接線
することのみを示しているが、実際には、一つおきに上
下から接線した方が放電の一様性が優れたものになるこ
とは明らかである。Note that the shape of the anode electrode/side of the cathode electrode l mainly affects the characteristics, so the first II! i! As shown in i7,
Of course, it may be formed into a half-ring shape. This half-ring shape is easier to manufacture if the wire is made thicker at the turn. Although the figure only shows that the cathode electrodes t are tangential from above, it is clear that the uniformity of the discharge will be better if every other electrode is tangential from above and below. .
以上説明したように、本発明は数列のビン電極を用いる
代りに、スパイラル状、リング状または半リング状のカ
ソード電極を用いることにより、放電を分散し、一様化
する優れた効果を有するものである。そのため使用する
カソード電極の数を減らし製作を容易にすることができ
る利点がある〇As explained above, the present invention has an excellent effect of dispersing and uniformizing the discharge by using a spiral, ring or half ring cathode electrode instead of using several rows of bottle electrodes. It is. This has the advantage of reducing the number of cathode electrodes used and making production easier.
第7図、f$2図はそれぞれガス流方向と放電方向が平
行な場合と重直な場合とにおける従来のビンからなるカ
ソード電極を用いたレーザ管を示す断面図、第3図、第
4!図は本発明の実施例を示す断面の略図である。
図中、lはアノード電極、コはビン電極、3は安定抵抗
体、lは電源、Sはレーザビーム、≦はガス流、7は外
囲器、tはカソード電極である。Figure 7 and Figure f$2 are cross-sectional views showing a laser tube using a conventional bottle-shaped cathode electrode when the gas flow direction and the discharge direction are parallel and perpendicular, respectively, Figures 3 and 4 ! The figure is a schematic cross-sectional view showing an embodiment of the invention. In the figure, l is an anode electrode, C is a bottle electrode, 3 is a stable resistor, l is a power source, S is a laser beam, ≦ is a gas flow, 7 is an envelope, and t is a cathode electrode.
Claims (1)
、レーザ発振を行なう横方向放電連続発振ガスレーザ管
において、前記カソード電極にスパイラル状またはリン
グ状にまいた導体の線または棒を用いたことを特徴とす
る横方向放電連続発振ガスレーザ管。In a lateral discharge continuous wave gas laser tube that generates a discharge between a seven-node electrode and a cathode electrode to perform laser oscillation, the cathode electrode is provided with a conductor wire or rod sown in a spiral or ring shape. A lateral discharge continuous wave gas laser tube.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP158882A JPS5847878B2 (en) | 1982-01-08 | 1982-01-08 | Lateral continuous wave gas laser tube |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP158882A JPS5847878B2 (en) | 1982-01-08 | 1982-01-08 | Lateral continuous wave gas laser tube |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS58119689A true JPS58119689A (en) | 1983-07-16 |
JPS5847878B2 JPS5847878B2 (en) | 1983-10-25 |
Family
ID=11505668
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP158882A Expired JPS5847878B2 (en) | 1982-01-08 | 1982-01-08 | Lateral continuous wave gas laser tube |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5847878B2 (en) |
Families Citing this family (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH0362384U (en) * | 1989-10-20 | 1991-06-18 | ||
JPH03223784A (en) * | 1990-01-29 | 1991-10-02 | Sanseishiya:Kk | Manufacture of label |
JPH03105874U (en) * | 1990-02-16 | 1991-11-01 | ||
JPH03105873U (en) * | 1990-02-16 | 1991-11-01 |
-
1982
- 1982-01-08 JP JP158882A patent/JPS5847878B2/en not_active Expired
Also Published As
Publication number | Publication date |
---|---|
JPS5847878B2 (en) | 1983-10-25 |
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