JPS59188189A - Co2 laser device - Google Patents
Co2 laser deviceInfo
- Publication number
- JPS59188189A JPS59188189A JP6172183A JP6172183A JPS59188189A JP S59188189 A JPS59188189 A JP S59188189A JP 6172183 A JP6172183 A JP 6172183A JP 6172183 A JP6172183 A JP 6172183A JP S59188189 A JPS59188189 A JP S59188189A
- Authority
- JP
- Japan
- Prior art keywords
- discharge
- laser
- electrodes
- electrode
- repetition
- 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
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
-
- 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
- H01S3/036—Means for obtaining or maintaining the desired gas pressure within the tube, e.g. by gettering, replenishing; Means for circulating the gas, e.g. for equalising the pressure within the tube
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】
本発明は、高速縁シ返しのパルス発振を得るT Ib
A C(、) 2 v−ザ装置に関するものである○T
I?、A C02レーザにおいては、放電空間内に放
電生成物(主として02分子)が多量になると放電がア
ーク放′YLに移行する。アーク放電はレーザの励起に
不適当な放電であり、アーク放電に移行するとレーザ発
振がとまる。ところでレーザ発振の繰り返しを上げるほ
ど、放電生成物が多量となる。DETAILED DESCRIPTION OF THE INVENTION The present invention provides T Ib
A C(,) 2 ○T related to v-the device
I? , A C02 laser, when a large amount of discharge products (mainly 02 molecules) becomes present in the discharge space, the discharge shifts to arc emission 'YL. Arc discharge is a discharge inappropriate for excitation of a laser, and laser oscillation stops when the discharge shifts to arc discharge. Incidentally, as the number of repetitions of laser oscillation increases, the amount of discharge products increases.
従って、レーザ発振の繰り返えしを上げるとアーク放電
に移行しやすくなるのでレーザ発振の高速繰り返し化の
為には、放電生成物を放電空間外へ除去する方法を講じ
ることが必要となる。Therefore, if the repetition rate of laser oscillation is increased, it becomes easier to shift to arc discharge, so in order to increase the repetition rate of laser oscillation, it is necessary to devise a method for removing discharge products from the discharge space.
従来の高速繰り返しTBAOO2レーザ装置においては
、レーザガスをフローすることにより放電生成物を放電
空間外へ除去していた。ところで、この場合放電電極−
の表面にガスが停滞するか又は非常にゆっ〈シ流れる境
界層(以下単に境界層と称す)ができる。境界層のガス
には放電生成物が含まれているので、レーザガスをフロ
ーしても完全には放電生成物を放電空間外へ除去できな
い。In the conventional high-speed repetition TBAOO2 laser device, discharge products are removed to the outside of the discharge space by flowing laser gas. By the way, in this case the discharge electrode -
A boundary layer (hereinafter simply referred to as boundary layer) is formed on the surface of which gas stagnates or flows very slowly. Since the boundary layer gas contains discharge products, even if the laser gas flows, the discharge products cannot be completely removed from the discharge space.
ただし、境界層の放電生成物はガスフローしない場合に
放電空間内に存在する放電生成物よりは少なく、従って
ガスフローした方がしない場合よりもレーザ発振の高速
繰り返し化が可能である。しかし、よシ高い繰り返しに
すると境界層の放電生成物が多量になシ、アーク放電に
移行する。すなわち繰り返しに限度が生じる。However, the amount of discharge products in the boundary layer is smaller than the amount of discharge products present in the discharge space when there is no gas flow, and therefore, laser oscillation can be repeated at a faster rate with gas flow than without. However, at higher repetition rates, a large amount of discharge products in the boundary layer is produced and the discharge transitions to arc discharge. In other words, there is a limit to repetition.
本発明は、前述のレーザ発振の高速繰り返し化の妨げと
なる放電生成物を放電空間から完全に除去し、レーザ発
振の高速繰り返し化を達成することを目的とする。An object of the present invention is to completely remove the discharge products that impede high-speed repetition of laser oscillation from the discharge space, thereby achieving high-speed repetition of laser oscillation.
本発明によれば、ガスをフローしさらに電極を回転させ
ることにより、電極表面の境界層が形成されることなく
、放電生成物がすみやかに放電空間外へ除去される高速
繰り返し’r EAO02レーザが得られる。According to the present invention, by flowing gas and rotating the electrode, a high-speed repetition 'r EAO02 laser is used in which discharge products are quickly removed out of the discharge space without forming a boundary layer on the electrode surface. can get.
以下、本発明について実施例を示す図面を参照して説明
する。DESCRIPTION OF THE PREFERRED EMBODIMENTS The present invention will be described below with reference to drawings showing embodiments.
第1図は実施例の電極部分を示す斜視図で、第2図はそ
の断面図である。カソード側電極11とアノード側電極
12は各々同形の電極エレメント13を4枚ずつ用いて
構成され、64回転軸14゜15の回りに矢印の向きに
(第2図−)回転する。FIG. 1 is a perspective view showing the electrode portion of the embodiment, and FIG. 2 is a sectional view thereof. The cathode side electrode 11 and the anode side electrode 12 are each constructed using four electrode elements 13 of the same shape, and rotate in the direction of the arrow (FIG. 2-) around a 64 rotation axis 14°15.
1だ放電時においては、アノード側電極11の電極エレ
メントの一つil′j:、常にカソード側電極12の電
極エレメントの一つと放電空間22をはさんで対向する
ようにしている。レーザ用ガスは矢印21の方向に流れ
る。During single discharge, one of the electrode elements il'j of the anode side electrode 11 always faces one of the electrode elements of the cathode side electrode 12 with the discharge space 22 in between. Laser gas flows in the direction of arrow 21.
第1図のT EAOO,レーザにおいて、放電によって
できた放電生成物はレーザ用ガスの流れ21によって放
電空間22の下流側に押し流される。この時、電極11
.12は各々回転軸14.15の回りに回転しているの
で電極表面における境界層が形成されない。したがって
放電生成物が放電空間22に残ることはない。このこと
により高速1、“:Lり返し発振ができる。例えば電極
11’、’12を30回/Sで回転させれば120 I
)I)Sでレーザを発j辰させることができる。なお回
転によるi極13の移動時間は、放電持続時間に比べて
十分長いので、放電が電極の回転によって乱されること
はない。In the TEAOO laser shown in FIG. 1, discharge products produced by discharge are swept downstream of the discharge space 22 by the flow 21 of the laser gas. At this time, electrode 11
.. Since the electrodes 12 are each rotated around the rotation axis 14, 15, no boundary layer is formed on the electrode surface. Therefore, no discharge products remain in the discharge space 22. This allows high-speed 1, ":L repeating oscillation. For example, if the electrodes 11' and '12 are rotated at 30 times/s, 120 I
) I) S can be used to emit a laser. Note that since the movement time of the i-pole 13 due to rotation is sufficiently longer than the discharge duration, the discharge is not disturbed by the rotation of the electrode.
電極11.12を、もっと多数の電極エレメント13を
用いて構成するか、電極の回転軸の回転数をもっと上げ
るかすれば、ガスの流速を上げなくとも数百ppsでレ
ーザ発振を得ることができる。By configuring the electrodes 11 and 12 using a larger number of electrode elements 13 or by increasing the rotational speed of the rotation axis of the electrode, it is possible to obtain laser oscillation at several hundred pps without increasing the gas flow rate. .
またガスの流路に乱流発生器を置く必要がないので、ガ
スの受ける抵抗が小さく、同じガス流速を得る場合、本
装置の方が、電力が小さくてすむ。Furthermore, since there is no need to place a turbulence generator in the gas flow path, the resistance experienced by the gas is small, and to obtain the same gas flow rate, this device requires less power.
第1図は本発明の実施例を示す電極部の斜視図であり、
第2図はその断面図である。
11・・・カソード側電極、12・・・アノード側電極
、13・・・電極エレメント、14.15・・・回転軸
、21・、・ガスの流れの方向、22・・・放電空間。FIG. 1 is a perspective view of an electrode section showing an embodiment of the present invention,
FIG. 2 is a sectional view thereof. DESCRIPTION OF SYMBOLS 11... Cathode side electrode, 12... Anode side electrode, 13... Electrode element, 14.15... Rotation shaft, 21... Gas flow direction, 22... Discharge space.
Claims (1)
された放電管と、放電管中に互いに対向して設置された
電極とを備えたC02レーザ装置において、レーザガス
をフローしさらにアノード側電極とカソード側電極の少
なくともどちらが一方を回転させることを特徴とするC
02レーザ装置。In a C02 laser device equipped with a pair of reflecting mirrors constituting a resonator, a discharge tube installed between the reflecting mirrors, and electrodes placed opposite each other in the discharge tube, a laser gas is caused to flow and further C, characterized in that at least one of the anode side electrode and the cathode side electrode rotates one of the electrodes.
02 laser device.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP6172183A JPS59188189A (en) | 1983-04-08 | 1983-04-08 | Co2 laser device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP6172183A JPS59188189A (en) | 1983-04-08 | 1983-04-08 | Co2 laser device |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS59188189A true JPS59188189A (en) | 1984-10-25 |
Family
ID=13179365
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP6172183A Pending JPS59188189A (en) | 1983-04-08 | 1983-04-08 | Co2 laser device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS59188189A (en) |
-
1983
- 1983-04-08 JP JP6172183A patent/JPS59188189A/en active Pending
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| JP2009162224A (en) | Method of forming cooling hole and turbine airfoil with hybrid-formed cooling holes | |
| JPH11505889A (en) | Screen and manufacturing method | |
| US6765946B2 (en) | Fan for gas discharge laser | |
| JPS59188189A (en) | Co2 laser device | |
| US6023486A (en) | Soldered fan assembly for electric discharge laser | |
| JP2002524861A (en) | Vibration control of cross flow fan cut-off assembly and discharge laser | |
| US6195378B1 (en) | Twisted blade tangential fan for excimer laser | |
| JPS6028288A (en) | Orthogonal gas laser oscillator | |
| WO2000070720A1 (en) | Tangential fan with cutoff assembly and vibration control for electric discharge laser | |
| US6618151B2 (en) | Ring laser gyroscope with offset aperture | |
| JPH0387081A (en) | Ring laser gyro | |
| JPS60178681A (en) | Gas laser device | |
| CN114204386B (en) | Increasing transverse excitation atmospheric pressure CO 2 Device and method for laser repetition frequency | |
| JPH03185885A (en) | Pulsed gas laser | |
| JP2001223415A (en) | Gas laser device | |
| JPH0760910B2 (en) | Gas laser device | |
| JPH06237029A (en) | Discharge excited excimer laser device | |
| JP2685946B2 (en) | Gas laser oscillation device | |
| JP2000263275A (en) | Multiple slit type air blow nozzle system | |
| JPH0317233B2 (en) | ||
| WO1988009577A1 (en) | Laser oscillator | |
| JPH07135363A (en) | Discharge pumped excimer laser | |
| JPH0325956B2 (en) | ||
| JPS59208890A (en) | High speed axial flow type gas laser tube | |
| JPS639177A (en) | Gas laser oscillator |