JPH0754862B2 - CO 2 Lower laser oscillator - Google Patents

CO 2 Lower laser oscillator

Info

Publication number
JPH0754862B2
JPH0754862B2 JP19326986A JP19326986A JPH0754862B2 JP H0754862 B2 JPH0754862 B2 JP H0754862B2 JP 19326986 A JP19326986 A JP 19326986A JP 19326986 A JP19326986 A JP 19326986A JP H0754862 B2 JPH0754862 B2 JP H0754862B2
Authority
JP
Japan
Prior art keywords
gas
laser oscillator
laser
cathode
mirror
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.)
Expired - Lifetime
Application number
JP19326986A
Other languages
Japanese (ja)
Other versions
JPS6348879A (en
Inventor
節夫 寺田
修三 ▲吉▼住
均 本宮
秀彦 唐崎
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP19326986A priority Critical patent/JPH0754862B2/en
Publication of JPS6348879A publication Critical patent/JPS6348879A/en
Publication of JPH0754862B2 publication Critical patent/JPH0754862B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime 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
    • H01S3/036Means 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

Description

【発明の詳細な説明】 産業上の利用分野 本発明は切断,溶接,熱処理等の工業用や、医療用とし
て利用されるレーザを出力するCO2レーザ発振装置に関
するものである。
TECHNICAL FIELD The present invention relates to a CO 2 laser oscillator for outputting a laser used for industrial purposes such as cutting, welding, heat treatment, etc., and for medical purposes.

従来の技術 従来のこの種のCO2レーザ発振装置について、第4図を
参照して説明する。
2. Description of the Related Art A conventional CO 2 laser oscillator of this type will be described with reference to FIG.

この第4図において、1は陰極、2は陽極、3は全反射
ミラー、3′は部分透過ミラーであり、これらによりレ
ーザ発振器を構成している。4はHeガスボンベ、5はN2
ガスボンベ、6はCO2ガスボンベであり、これらのHeガ
スボンベ4,N2ガスボンベ5,CO2ガスボンベ6から供給さ
れるHeガス,N2ガス,CO2ガスはレーザガス媒体として
全反射ミラー3および部分透過ミラー3′の近傍の供給
口からレーザ発振器内に導入される。7はレーザ発振器
とともにレーザガス媒体の循環路を形成し、レーザ発振
器内のレーザガス媒体を循環させるブロアである。8は
レーザガス媒体の循環路に接続された真空ポンプであ
り、循環路内を一定圧力に保つ。循環路内のレーザガス
媒体は図示矢印方向に流れ、レーザ発振器内では陰極1
から陽極2へと軸流方向に流れる。
In FIG. 4, 1 is a cathode, 2 is an anode, 3 is a total reflection mirror, and 3'is a partial transmission mirror, and these constitute a laser oscillator. 4 is He gas cylinder, 5 is N 2
Gas cylinder, 6 is a CO 2 gas cylinder, these He gas cylinder 4, N 2 gas cylinder 5, He gas supplied from the CO 2 gas cylinder 6, N 2 gas, CO 2 gas is the total reflection mirror 3 and partially transmitted as the laser gas medium It is introduced into the laser oscillator from a supply port near the mirror 3 '. A blower 7 forms a laser gas medium circulation path together with the laser oscillator and circulates the laser gas medium in the laser oscillator. Reference numeral 8 denotes a vacuum pump connected to the circulation path of the laser gas medium, which maintains a constant pressure in the circulation path. The laser gas medium in the circulation path flows in the direction of the arrow in the figure, and in the laser oscillator, the cathode 1
To the anode 2 in the axial direction.

上記構成において、陰極1と陽極2との間に直流電圧を
印加すると、レーザ発振器内で放電が生じ、部分透過ミ
ラー3′を透過するレーザ出力が得られる。
In the above structure, when a DC voltage is applied between the cathode 1 and the anode 2, a discharge is generated in the laser oscillator and a laser output transmitted through the partial transmission mirror 3'is obtained.

発明が解決しようとする問題点 しかしながら、上記構成においては、レーザ発振器内の
陰極1と陽極2との間で放電するだけでなく、陰極1と
全反射ミラー3の間や、陽極2と部分透過ミラー3′と
の間でも放電が時折発生していた。この際、全反射ミラ
ー3や部分透過ミラー3′が電極として作用してしまう
ため、全反射ミラー3の表面や部分透過ミラー3′の表
面の損傷が激しく、反射率が低下し、レーザ出力が低下
してしまうという欠点があった。
DISCLOSURE OF THE INVENTION Problems to be Solved by the Invention However, in the above configuration, not only the discharge is generated between the cathode 1 and the anode 2 in the laser oscillator, but also between the cathode 1 and the total reflection mirror 3 and between the anode 2 and the partial transmission. Electric discharge sometimes occurred between the mirror 3 '. At this time, since the total reflection mirror 3 and the partial transmission mirror 3 ′ act as electrodes, the surface of the total reflection mirror 3 and the partial transmission mirror 3 ′ are severely damaged, the reflectance is lowered, and the laser output is reduced. There was a drawback that it would decrease.

問題点を解決するための手段 上記問題点を解決するため、本発明のCO2レーザ発振装
置は、レーザ発振器の陰極近傍にHeガスの一部を導入す
る第1供給口を設け、レーザ発振器の部分透過ミラー,
折返しミラー,全反射ミラー等のミラー部の近傍にN2
ス,CO2ガスおよびHeガスの一部を導入する第2供給口
を設けてなるものである。
Means for Solving the Problems In order to solve the above problems, the CO 2 laser oscillation apparatus of the present invention is provided with a first supply port for introducing a part of He gas near the cathode of the laser oscillator, Partially transparent mirror,
A second supply port for introducing a part of N 2 gas, CO 2 gas and He gas is provided in the vicinity of the mirror part such as the folding mirror and the total reflection mirror.

作用 上記構成において、レーザ発振器内の陰極と陽極の間以
外の部分での放電を防止することによりミラー表面の品
質維持を行ない、レーザ出力の低下を防止するととも
に、第1供給口からレーザ発振器内に導入されるHeガス
によって陰極の冷却を行ない、放電の安定性を良くし、
安定したレーザ出力を得る。
Function In the above-mentioned configuration, the quality of the mirror surface is maintained by preventing the discharge in a portion other than between the cathode and the anode in the laser oscillator, the decrease in the laser output is prevented, and the laser power is supplied from the first supply port to the inside of the laser oscillator. The cathode is cooled by the He gas introduced into, improving the stability of the discharge,
Obtain stable laser output.

実施例 以下、本発明の実施例について第1図乃至第3図を参照
して説明する。
Embodiments Embodiments of the present invention will be described below with reference to FIGS. 1 to 3.

第1図は本実施例のブロック図であり、この第1図にお
いて、第4図に示した構成と同一の構成部分について同
一番号を付し、説明を省略する。
FIG. 1 is a block diagram of the present embodiment. In FIG. 1, the same components as those shown in FIG. 4 are designated by the same reference numerals and the description thereof will be omitted.

第1図において、9はレーザ発振器の陰極1近傍に設け
られた第1供給口であり、Heガスボンベ4から供給され
るHeガスの一部がこの第1供給口9からレーザ発振器内
に導入される。10はレーザ発振器の全反射ミラー3近傍
および部分透過ミラー3′近傍に設けられた第2供給口
であり、Heガスボンベ4から供給されるHeガスの他の一
部およびN2ガスボンベ5から供給されるN2ガスおよびCO
2ガスボンベ6から供給されるCO2ガスがこの第2供給口
10からレーザ発振器内に導入される。11はレーザ発振器
の陽極2近傍に設けられた第3供給口であり、Heガスボ
ンベ4から供給されるHeガスがこの第3供給口11からレ
ーザ発振器内に導入される。
In FIG. 1, reference numeral 9 is a first supply port provided in the vicinity of the cathode 1 of the laser oscillator, and a part of He gas supplied from the He gas cylinder 4 is introduced into the laser oscillator from the first supply port 9. It A second supply port 10 is provided in the vicinity of the total reflection mirror 3 and the partial transmission mirror 3'of the laser oscillator, and is supplied from another part of the He gas supplied from the He gas cylinder 4 and the N 2 gas cylinder 5. N 2 gas and CO
The CO 2 gas supplied from the 2 gas cylinder 6 is the second supply port.
It is introduced into the laser oscillator from 10. Reference numeral 11 denotes a third supply port provided in the vicinity of the anode 2 of the laser oscillator, and He gas supplied from the He gas cylinder 4 is introduced into the laser oscillator through the third supply port 11.

上記構成において、陰極1と陽極2との間に直流電圧を
印加すると、レーザ発振器内の陰極1と陽極2の間でグ
ロー放電が発生する。
In the above structure, when a DC voltage is applied between the cathode 1 and the anode 2, glow discharge is generated between the cathode 1 and the anode 2 in the laser oscillator.

HeガスはHeガス,N2ガス,CO2ガス中、レーザ媒体の冷
却作用を有しているが、Heガスの一部を陰極1の近傍の
第1供給口9からレーザ発振器内に導入することによ
り、陰極1の冷却効果を増す。また、HeガスはN2ガスや
CO2ガスに比較して放電しやすいガスであり、陰極1と
陽極2との間のグロー放電の維持を容易にしている。さ
らに、第2供給口10からレーザ発振器内に導入されるHe
ガスの他の一部およびN2ガスおよびCO2ガスよりなるレ
ーザガス媒体はHeガスの比率が小さくなっているため、
放電開始電圧が非常に高くなり、陰極1と全反射ミラー
3との間や、陽極2と部分透過ミラー3′との間での放
電を防止することができる。
He gas has a cooling effect on the laser medium in He gas, N 2 gas, and CO 2 gas, but a part of He gas is introduced into the laser oscillator from the first supply port 9 near the cathode 1. As a result, the cooling effect of the cathode 1 is increased. He gas is N 2 gas or
It is a gas that discharges more easily than CO 2 gas and facilitates the maintenance of glow discharge between the cathode 1 and the anode 2. Further, He introduced into the laser oscillator from the second supply port 10
Since the proportion of He gas in the laser gas medium consisting of the other part of the gas and N 2 gas and CO 2 gas is small,
The discharge start voltage becomes extremely high, and it is possible to prevent discharge between the cathode 1 and the total reflection mirror 3 and between the anode 2 and the partial transmission mirror 3 '.

なお、本実施例においては、レーザガス媒体のガス比率
がHe:N2:CO2=70:20:10とし、陰極1と陽極2間の放電
長を30cm、陰極1と全反射ミラー3の間および陽極2と
部分透過ミラー3′の間の無放電長を15cmとすると、放
電開始電圧は約20kVであったが、従来例においてはパル
ス放電時に無放電部で放電が生じた。
In this example, the gas ratio of the laser gas medium was He: N 2 : CO 2 = 70: 20: 10, the discharge length between the cathode 1 and the anode 2 was 30 cm, and the distance between the cathode 1 and the total reflection mirror 3 was 30 cm. When the non-discharge length between the anode 2 and the partial transmission mirror 3'is 15 cm, the discharge start voltage was about 20 kV, but in the conventional example, discharge occurred at the non-discharge part during pulse discharge.

本実施例の様にHeガスの一部を陰極1近傍の第1供給口
9から導入し、Heガスの残りの一部およびN2ガスおよび
CO2ガスを全反射ミラー3の近傍および部分透過ミラー
3′の近傍の第2供給口10から導入した場合の、無放電
部での放電発生割合と、長時間使用後のレーザ出力の低
下割合を調べた。この結果を第2図,第3図に示す。
As in this embodiment, a part of He gas is introduced from the first supply port 9 in the vicinity of the cathode 1, and the remaining part of He gas and N 2 gas and
When CO 2 gas is introduced from the second supply port 10 in the vicinity of the total reflection mirror 3 and the partial transmission mirror 3 ', the discharge generation rate in the non-discharge part and the reduction rate of the laser output after long-term use I checked. The results are shown in FIGS. 2 and 3.

第3図,第4図より明らかなように、第1供給口9から
導入するHeガスの割合を多くすることにより、パルス放
電時の無放電部での放電発生率が著しく低下し、さら
に、長時間使用後のレーザ出力の低下割合が極端に小さ
くなる。
As is clear from FIGS. 3 and 4, by increasing the proportion of He gas introduced from the first supply port 9, the discharge occurrence rate in the non-discharge part during pulse discharge is significantly reduced, and further, The reduction rate of the laser output after using for a long time becomes extremely small.

これは、Heガスによる陰極1の冷却効果が上がり、陰極
1の表面酸化が低減しているためである。特に、両者と
も、第1供給口9から導入されるHeガスの割合が30%以
上の場合に顕著であった。
This is because the cooling effect of the cathode 1 by the He gas is enhanced and the surface oxidation of the cathode 1 is reduced. In particular, both were remarkable when the ratio of He gas introduced from the first supply port 9 was 30% or more.

なお、上記実施例においては全反射ミラー3,部分透過ミ
ラー3′をミラー部として備えている場合について説明
したが、レーザ発振器の構成によっては、ミラー部とし
て終段反射ミラー,折り返しミラー等であっても良い。
In the above embodiment, the case where the total reflection mirror 3 and the partial transmission mirror 3'are provided as the mirror portion has been described. However, depending on the configuration of the laser oscillator, the final reflection mirror, the folding mirror or the like may be used as the mirror portion. May be.

発明の効果 以上のように本発明によれば、レーザガス媒体中、Heガ
スの一部を陰極近傍の第1供給口からレーザ発振器内に
導入し、Heガスの残りの一部およびN2ガスおよびCO2
スをミラー部近傍の第2供給口からレーザ発振器内に導
入する構成としたことにより、無放電部での放電の発生
率を低下し、ミラー表面の損傷を防止するとともに、陰
極Heガスにて冷却することにより陰極の寿命を長くし、
長時間安定したレーザ出力を得ることができる。
As described above, according to the present invention, in the laser gas medium, a part of He gas is introduced into the laser oscillator from the first supply port near the cathode, and the remaining part of He gas and N 2 gas and By introducing CO 2 gas into the laser oscillator from the second supply port near the mirror part, the discharge rate in the non-discharge part is reduced, damage to the mirror surface is prevented, and cathode He gas By extending the life of the cathode by cooling
A stable laser output can be obtained for a long time.

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

第1図は本発明の一実施例を示すCO2レーザ発振装置の
ブロック回路図、第2図は同CO2レーザ発振装置におけ
る全Heガス中、陰極近傍より供給する割合と無放電部で
の放電発生割合の関係を示す特性図、第3図は同CO2
ーザ発振装置における全Heガス中、陰極近傍より供給す
る割合と初期値に対する出力低下率の関係を示す特性
図、第4図は従来のCO2レーザ発振装置のブロック回路
図である。 1……陰極、2……陽極、3……全反射ミラー、3′…
…部分透過ミラー、4……Heガスボンベ、5……N2ガス
ボンベ、6……CO2ガスボンベ、9……第1供給口、10
……第2供給口。
FIG. 1 is a block circuit diagram of a CO 2 laser oscillator showing an embodiment of the present invention, and FIG. 2 is a proportion of all He gas in the same CO 2 laser oscillator supplied from near the cathode and in a non-discharge part. Fig. 3 is a characteristic diagram showing the relationship of the discharge generation rate. Fig. 3 is a characteristic diagram showing the relationship between the ratio of the gas supplied from the vicinity of the cathode in all the He gas in the CO 2 laser oscillator and the output reduction rate with respect to the initial value. FIG. 11 is a block circuit diagram of a conventional CO 2 laser oscillator. 1 ... Cathode, 2 ... Anode, 3 ... Total reflection mirror, 3 '...
… Partial transmission mirror, 4 …… He gas cylinder, 5 …… N 2 gas cylinder, 6 …… CO 2 gas cylinder, 9 …… First supply port, 10
...... Second supply port.

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】レーザ発振器の陰極近傍に、レーザガス媒
体となるHeガスの一部を導入する第1供給口を設け、レ
ーザ発振器の共振器を構成している部分透過ミラー,折
返しミラー,全反射ミラー等のミラー部の近傍にN2
ス,CO2ガスおよびHeガスの他の一部を導入する第2供
給口を設けてなるCO2レーザ発振装置。
1. A partial transmission mirror, a folding mirror, and a total reflection which constitute a resonator of a laser oscillator by providing a first supply port for introducing a part of He gas serving as a laser gas medium near the cathode of the laser oscillator. A CO 2 laser oscillator comprising a second supply port for introducing another part of N 2 gas, CO 2 gas and He gas near the mirror part such as a mirror.
【請求項2】レーザガス媒体の流れ方向を陰極より陽極
への軸流方向とした特許請求の範囲第1項記載のCO2
ーザ発振装置。
2. The CO 2 laser oscillator according to claim 1, wherein the flow direction of the laser gas medium is an axial flow direction from the cathode to the anode.
【請求項3】第1供給口から導入されるHeガスの一部
は、レーザ発振器に導入されるHeガス全体の30%以上と
した特許請求の範囲第1項記載のCO2レーザ発振装置。
3. The CO 2 laser oscillator according to claim 1, wherein a part of the He gas introduced from the first supply port is 30% or more of the whole He gas introduced into the laser oscillator.
JP19326986A 1986-08-19 1986-08-19 CO 2 Lower laser oscillator Expired - Lifetime JPH0754862B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP19326986A JPH0754862B2 (en) 1986-08-19 1986-08-19 CO 2 Lower laser oscillator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP19326986A JPH0754862B2 (en) 1986-08-19 1986-08-19 CO 2 Lower laser oscillator

Publications (2)

Publication Number Publication Date
JPS6348879A JPS6348879A (en) 1988-03-01
JPH0754862B2 true JPH0754862B2 (en) 1995-06-07

Family

ID=16305127

Family Applications (1)

Application Number Title Priority Date Filing Date
JP19326986A Expired - Lifetime JPH0754862B2 (en) 1986-08-19 1986-08-19 CO 2 Lower laser oscillator

Country Status (1)

Country Link
JP (1) JPH0754862B2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0714089B2 (en) * 1987-05-18 1995-02-15 ファナック株式会社 Laser oscillator and method for enclosing laser gas in laser oscillator
CN104676248B (en) * 2014-12-26 2017-03-22 西南石油大学 Helium circulating system

Also Published As

Publication number Publication date
JPS6348879A (en) 1988-03-01

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