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JPS63239888A - Gas laser oscillator - Google Patents

Gas laser oscillator

Info

Publication number
JPS63239888A
JPS63239888A JP19576287A JP19576287A JPS63239888A JP S63239888 A JPS63239888 A JP S63239888A JP 19576287 A JP19576287 A JP 19576287A JP 19576287 A JP19576287 A JP 19576287A JP S63239888 A JPS63239888 A JP S63239888A
Authority
JP
Japan
Prior art keywords
gas
laser
duct
medium gas
laser medium
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
Application number
JP19576287A
Other languages
Japanese (ja)
Other versions
JPH0666487B2 (en
Inventor
Akihiro Otani
昭博 大谷
Noriaki Sasaki
憲明 佐々木
Kenji Kumamoto
健二 熊本
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric 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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Publication of JPS63239888A publication Critical patent/JPS63239888A/en
Publication of JPH0666487B2 publication Critical patent/JPH0666487B2/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

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Engineering & Computer Science (AREA)
  • Plasma & Fusion (AREA)
  • Optics & Photonics (AREA)
  • Lasers (AREA)

Abstract

PURPOSE:To suppress the absorption of laser light with the laser medium gas of an extension and to stabilize a laser output by disposing external communication means for supplying and exhausting the gas to the extensions of both ends of a discharge tube. CONSTITUTION:A first inlet tube 8a is attached to a duct 2a connected between extension ducts 2 and 2 provided with oblique reflecting mirrors M2, M3. Second and third inlet tubes 8b, 8c are attached to the ducts 2, 2 of remote side from a communication duct 5, and a fourth inlet tube 8d is attached to the duct 2 provided with a reflecting mirror M1 of near side. Accordingly, each time laser medium gas is replaced, the gas of the duct 2 is combined with laser medium gas circulating stream. Thus, the rise of gas temperature due to the absorption of the laser light in the duct 2 can be suppressed to obtain a stable laser output.

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明はガスレーザ発振器に関し、特に安定したレーザ
光を得ることのできるガスレーザ発振器に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a gas laser oscillator, and more particularly to a gas laser oscillator that can provide stable laser light.

[従来の技術] 従来のこの種の装置を第3図に基づいて説明する。同図
は従来装置を示す概略構成図であり、該ガスレーザ発振
器は、2木の放電管(1) 、 (1)を備え、各放電
管(1)両端にはそれぞれ延長部として延長ダクト(2
)が連設され、更に各延長ダクト(2)端にはそれぞれ
反射!(1〜(M4)が取付けられている。
[Prior Art] A conventional device of this kind will be explained based on FIG. This figure is a schematic configuration diagram showing a conventional device, and the gas laser oscillator is equipped with two discharge tubes (1), (1), and extension ducts (2) as extensions at both ends of each discharge tube (1).
) are installed in a row, and each extension duct (2) has a reflection at the end! (1 to (M4) are installed.

また、一方の放電管(1)両端にはこれに直交するダク
ト(3) 、 (4)が上記延長ダクト(2) 、 (
2)に接合するようにして取付けられ、かつ各ダクト(
3)。
Further, at both ends of one discharge tube (1), ducts (3), (4) perpendicular to this are connected to the extension ducts (2), (
2), and each duct (
3).

(4)の延長端は上記放電管(1)に平行した連絡ダク
ト(5)によって連通すべく形成されている。該連絡ダ
クト(5)の略中間には熱交換器(6)及びファン(7
)カ(順次配設され、一方のダクト(4)を介して上記
放電管(1) 、 (1)からの高熱レーザ媒質ガスを
冷却しながら吸引するとともに他方のダクト(3)を介
して冷却レーザ媒質ガスを該放電管(1)。
The extended end of (4) is formed to communicate with the discharge tube (1) through a parallel communication duct (5). A heat exchanger (6) and a fan (7) are installed approximately in the middle of the communication duct (5).
) (arranged sequentially, the high-temperature laser medium gas from the discharge tubes (1), (1) is sucked while cooling through one duct (4), and is cooled through the other duct (3). Laser medium gas into the discharge tube (1).

(1)に循環させるようにしている。(1) is circulated.

更に連絡ダクト(5)にはレーザ媒質ガスを給排するガ
ス導入管(8)及びガス排出管(9)が取付けられ、劣
化したレーザ媒質ガスを適宜更新できるようにしている
Furthermore, a gas introduction pipe (8) and a gas exhaust pipe (9) for supplying and discharging laser medium gas are attached to the communication duct (5), so that deteriorated laser medium gas can be replaced as appropriate.

然して放電管(1) 、 (1)に電圧を印加して放電
エネルギを発生させ放電管(1) 、 (1)内にある
レーザ媒質ガスを励起し、該励起ガスからレーザ光が発
生して放電管(1) 、 (1)での両延長端の反射鏡
(M+)〜(M4)によってボンピングされることにな
る。つまり、反射鏡□L)及び(M2)は連絡ダクト(
5)側の放電管(1)の延長端に配設され、一方の反射
鏡(M、)は放電管(1)の軸芯に対し直交した位置関
係にあり、他方の反射鏡(M2)は45°傾斜した位置
関係にある。従って該放電管(1) において発生した
レーザ光は他方の反射鏡(M2)から他方の放電管(1
)に配設された傾斜反nす鏡(M、)に伝送され、さら
に該反射鏡(M4)に伝送される。かくして発生したレ
ーザ光は反射鏡(M r )ないしくM4)間を往復す
る間に逐次放電エネルギを得て所望のエネルギ値に達し
たレーザ光は部分反射鏡として形成された反射鏡(M4
)から外部へと射出される。
Then, a voltage is applied to the discharge tubes (1), (1) to generate discharge energy and excite the laser medium gas inside the discharge tubes (1), (1), and laser light is generated from the excited gas. Bumping is performed by the reflecting mirrors (M+) to (M4) at both extended ends of the discharge tubes (1) and (1). In other words, the reflecting mirrors □L) and (M2) are connected to the communication duct (
5) is arranged at the extended end of the discharge tube (1), one reflecting mirror (M,) is positioned orthogonal to the axis of the discharge tube (1), and the other reflecting mirror (M2) are inclined at 45 degrees. Therefore, the laser light generated in the discharge tube (1) is transmitted from the other reflecting mirror (M2) to the other discharge tube (1).
), and is further transmitted to the mirror (M4). The thus generated laser beam sequentially obtains discharge energy while reciprocating between the reflecting mirrors (M r ) or M4), and the laser beam that has reached a desired energy value is transferred to the reflecting mirror (M4) formed as a partial reflecting mirror.
) is ejected to the outside.

[発明が解決しようとする問題点] 上記構成によれば、レーザ媒質ガスは、放電管(t)、
(1) 、ダクト(3) 、 (4)及び連絡ダクト(
5)によって形成されるループ内を循環する一方、各延
長ダクト(2)に存するレーザ媒質ガスは循環せずその
殆どが滞留することになる。
[Problems to be Solved by the Invention] According to the above configuration, the laser medium gas is connected to the discharge tube (t),
(1), ducts (3), (4) and connecting ducts (
5), while the laser medium gas existing in each extension duct (2) does not circulate and most of it remains.

上記のようなガスの循環、滞留に関係なくレーザ光は各
部位にあるし−ザ媒質ガスを通過することになる。する
とレーザ光は、レーザ媒質ガス特に滞留したガスに吸収
されてガス温度を上昇させる。ガス温度が上昇する程に
レーザ光の吸収効率が急激に高まることが一般に知られ
ているが、この現象は滞留しているレーザ媒質にも認め
ることができ、滞留しているからこそ漸次ガス塩が上昇
して増々レーザ光を効率よく吸収することになり、この
ことが安定したレーザ光を得るための障害となっていた
Irrespective of the above-mentioned circulation and retention of gas, the laser light is present at each location and passes through the medium gas. Then, the laser light is absorbed by the laser medium gas, particularly the stagnant gas, and increases the gas temperature. It is generally known that the absorption efficiency of laser light increases rapidly as the gas temperature rises, but this phenomenon can also be observed in a stagnant laser medium. increases, and the laser light is absorbed more and more efficiently, which has been an obstacle to obtaining stable laser light.

本発明は叙上の問題点を解決するためになされたもので
、延長ダクト(2)にあるレーザ媒質ガスを滞留させな
いようにすることによって該部分に招けるレーザ光の吸
収を軽減し、安定したレーザ出力の得られるガスレーザ
発振器を提供するものである。
The present invention has been made to solve the above-mentioned problems, and by preventing the laser medium gas in the extension duct (2) from stagnation, the absorption of the laser light invited to the extension duct (2) is reduced, and the laser light is stabilized. The present invention provides a gas laser oscillator that can obtain a high laser output.

[問題点を解決するための手段] 本発明は、延長部におけるレーザ媒質ガスの滞留を解消
すべく該延長部にレーザ媒質ガスを給排する外部連通手
段を配設したものである。
[Means for Solving the Problems] The present invention provides an external communication means for supplying and discharging laser medium gas to and from the extension part in order to eliminate retention of the laser medium gas in the extension part.

[作用] 本発明によれば、延長ダクトに設けた外部連通手段によ
り該延長ダクトのレーザ媒質ガスは循環レーザ媒質ガス
に合流または外部に排出されるため、延長ダクトに該ガ
スが滞留することがなく、したがって延長ダクトのレー
ザ媒質ガスによるレーザ光の吸収を格段に抑制すること
ができ、レーザ出力を安定化することができる。
[Function] According to the present invention, the laser medium gas in the extension duct joins the circulating laser medium gas or is discharged to the outside by the external communication means provided in the extension duct, so that the gas does not stay in the extension duct. Therefore, the absorption of laser light by the laser medium gas in the extension duct can be significantly suppressed, and the laser output can be stabilized.

[実施例] 以下第1図に示す一実施例に基づいて本発明を説明する
。尚、説明の都合上従来と同−又は相当部分には同一符
号を付してその説明を省略し、この実施例の特徴を中心
に説明すると、この実施例に係るガスレーザ発振器は、
放電管(1)に連結した延長ダクト(2)にレーザ媒質
ガスの導入管(8a)〜(8d)を取付けた点に特徴を
有している。即ち、傾斜した反射鏡(M2) 、(M3
)の配設された延長ダクト(2)、(2)間を連通ずる
ダクト(2a)に第1導入管(8a)を取付け、連絡ダ
クト(5)に対して遠い側の延長ダクト(2) 、 (
2)に対して第2、第3導入管(8b) 、 (8c)
を、そしぞ近い側であって放電管(1)の軸芯に直交す
る反射鏡(M+)の配設された延長ダクト(2)に対し
て第4導入管(8d)をそれぞれ取付ける一方、従来連
絡ダクト(5)にあった導入管を省略してレーザ発振器
を構成したものである。
[Example] The present invention will be described below based on an example shown in FIG. For convenience of explanation, parts that are the same or equivalent to the conventional ones are given the same reference numerals and their explanations are omitted, and the description will focus on the features of this embodiment.The gas laser oscillator according to this embodiment is as follows.
It is characterized in that laser medium gas introduction tubes (8a) to (8d) are attached to an extension duct (2) connected to a discharge tube (1). That is, the inclined reflectors (M2), (M3
), the first introduction pipe (8a) is attached to the duct (2a) that communicates between the extension ducts (2) and (2), and the extension duct (2) on the far side from the communication duct (5) is attached. , (
For 2), the second and third introduction pipes (8b) and (8c)
While attaching the fourth introduction pipe (8d) to the extension duct (2) in which the reflector (M+) is arranged, which is on the nearer side and is perpendicular to the axis of the discharge tube (1), The laser oscillator is constructed by omitting the introduction pipe that was conventionally used in the communication duct (5).

従って、上記本実施例のガスレーザ発振器はレーザ媒質
ガスを更新する度毎に各延長ダクト(2)にあるガスを
レーザ媒質ガス循環流に合流させることが可能となり、
該ダクト(2)におけるレーザ光の吸収によるガス温の
上昇を抑制することができ、ひいてはガス温の上昇によ
るレーザ光の吸収効率の急激な上昇を招くことがなく、
常に安定したレーザ出力を確保することができる。
Therefore, in the gas laser oscillator of this embodiment, the gas in each extension duct (2) can be made to join the laser medium gas circulation flow every time the laser medium gas is updated.
It is possible to suppress the rise in gas temperature due to the absorption of laser light in the duct (2), and in turn, the rise in the gas temperature does not cause a rapid increase in the absorption efficiency of laser light.
It is possible to always ensure stable laser output.

第2図は本発明の他の実施例を示すものである。この実
施例のガスレーザ発振器は、上記第1実施例でレーザ媒
質ガスの導入部として用いた導入管(8a)〜(8d)
をそれぞれレーザ媒質ガスの排出管(9a)〜(9d)
に構成した点が上記第1実施例のものと異なっている。
FIG. 2 shows another embodiment of the invention. The gas laser oscillator of this embodiment has the introduction tubes (8a) to (8d) used as the introduction section for the laser medium gas in the first embodiment.
are the laser medium gas exhaust pipes (9a) to (9d), respectively.
This embodiment differs from the first embodiment in that it is configured as follows.

即ち、傾斜した反射鏡(M2)。That is, a tilted reflector (M2).

(M3)の配設された延長ダクト(2) 、 (2)間
を連通ずるダクト(2a)に第1排比管(9a)を取付
け、連絡ダクト(5)に対して遠い側の延長ダクト(2
) 、 (2)に対して第2、第3排出管(9b) 、
 (9c)を、そして近い側であって放電管(1)の軸
芯に直交する反射鏡(Ml)の配設された延長ダクト(
2)に対して第4排出管(9d)それぞれ取付ける一方
、従来連絡ダークト(5)にあった排出管を省略してレ
ーザ発振器を構成したものである。この実施例において
は、延長ダクト(2) 、 (2) に滞留するレーザ
媒質ガスは各排出管(9a)〜(9d)より外部へ排出
されるため、上記第1実施例同様ガス温の上昇を抑制す
ることができ、常に安定したレーザ出力を確保すること
ができる。
(M3), the first ratio pipe (9a) is attached to the duct (2a) that communicates between the extension ducts (2) and (2), and the extension duct (9a) on the far side from the communication duct (5) is attached. 2
), second and third discharge pipes (9b) for (2),
(9c), and an extension duct (on the near side) equipped with a reflector (Ml) perpendicular to the axis of the discharge tube (1).
The laser oscillator is constructed by attaching a fourth exhaust pipe (9d) to 2), while omitting the exhaust pipe that was conventionally used in the connecting dark (5). In this embodiment, the laser medium gas remaining in the extension ducts (2) and (2) is discharged to the outside through each exhaust pipe (9a) to (9d), so that the gas temperature increases as in the first embodiment. can be suppressed, and stable laser output can always be ensured.

[発明の効果] 本発明によれば、レーザ発振器内におけるレーザ媒質ガ
スの部分的滞留をなくすることができ、そのために従来
問題となっていた滞留ガスによる発生レーザ光の吸収を
格段に抑制することができ、安定したレーザ出力を得る
ことができる。
[Effects of the Invention] According to the present invention, it is possible to eliminate partial retention of the laser medium gas within the laser oscillator, thereby significantly suppressing the absorption of the generated laser light by the retained gas, which has been a problem in the past. It is possible to obtain stable laser output.

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

第1図は本発明の一実施例を示すレーザ発振器の概略構
成図、第2図は本発明の他の実施例を示す第1図相当図
、第3図は従来装置を示す第1図相当図である。 図において (1)は放電管、 (2)は延長ダクト(延長部)、 (11!l)ないしくM4)は反射鏡。 なお、各図中、同一符号は同−又は相当部分を示す。 代  理  人   大  岩  増  雑業1図 第2図
FIG. 1 is a schematic configuration diagram of a laser oscillator showing one embodiment of the present invention, FIG. 2 is a diagram equivalent to FIG. 1 showing another embodiment of the invention, and FIG. 3 is a diagram equivalent to FIG. 1 showing a conventional device. It is a diagram. In the figure, (1) is the discharge tube, (2) is the extension duct (extension part), and (11!l) or M4) is the reflector. In each figure, the same reference numerals indicate the same or corresponding parts. Agent Masu Oiwa Miscellaneous work Figure 1 Figure 2

Claims (1)

【特許請求の範囲】[Claims] 放電管両端からの両延長部端に1対の反射鏡が配設され
、該延長部を介してレーザ媒質ガスを上記放電管内に循
環させて該放電管に発生した放電エネルギにより上記レ
ーザ媒質ガスを励起するとともに上記1対の反射鏡によ
るポンピング作用にてレーザ光を発振するガスレーザ発
振器において、上記延長部におけるレーザ媒質ガスの滞
留を解消すべく該延長部にレーザ媒質ガスを給排する外
部連通手段を配設したことを特徴とするガスレーザ発振
器。
A pair of reflecting mirrors are disposed at the ends of both extensions from both ends of the discharge tube, and the laser medium gas is circulated within the discharge tube through the extensions, and the discharge energy generated in the discharge tube causes the laser medium gas to be In a gas laser oscillator that excites the laser beam and oscillates a laser beam by the pumping action of the pair of reflecting mirrors, an external communication supplying and discharging a laser medium gas to and from the extension part in order to eliminate retention of the laser medium gas in the extension part. A gas laser oscillator characterized in that a means is provided.
JP62195762A 1986-11-06 1987-08-05 Gas laser oscillator Expired - Lifetime JPH0666487B2 (en)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
JP61-264469 1986-11-06
JP26446986 1986-11-06

Publications (2)

Publication Number Publication Date
JPS63239888A true JPS63239888A (en) 1988-10-05
JPH0666487B2 JPH0666487B2 (en) 1994-08-24

Family

ID=17403652

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62195762A Expired - Lifetime JPH0666487B2 (en) 1986-11-06 1987-08-05 Gas laser oscillator

Country Status (1)

Country Link
JP (1) JPH0666487B2 (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0444283A (en) * 1990-06-07 1992-02-14 Fanuc Ltd Laser oscillator
JPH0766473A (en) * 1993-08-26 1995-03-10 Matsushita Electric Ind Co Ltd Gas laser oscillator
JP2010171145A (en) * 2009-01-21 2010-08-05 Fanuc Ltd Gas laser oscillator
DE102015010754A1 (en) 2014-08-25 2016-02-25 Fanuc Corporation Laser laser oscillator equipped with laser medium flow path

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS55165690A (en) * 1979-06-11 1980-12-24 Hitachi Ltd Laser oscillator

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS55165690A (en) * 1979-06-11 1980-12-24 Hitachi Ltd Laser oscillator

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0444283A (en) * 1990-06-07 1992-02-14 Fanuc Ltd Laser oscillator
JPH0766473A (en) * 1993-08-26 1995-03-10 Matsushita Electric Ind Co Ltd Gas laser oscillator
JP2010171145A (en) * 2009-01-21 2010-08-05 Fanuc Ltd Gas laser oscillator
DE102015010754A1 (en) 2014-08-25 2016-02-25 Fanuc Corporation Laser laser oscillator equipped with laser medium flow path
US9350134B2 (en) 2014-08-25 2016-05-24 Fanuc Corporation Laser oscillator provided with laser medium flow path

Also Published As

Publication number Publication date
JPH0666487B2 (en) 1994-08-24

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