JPH0414272A - Laser oscillating equipment - Google Patents

Laser oscillating equipment

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Publication number
JPH0414272A
JPH0414272A JP11647790A JP11647790A JPH0414272A JP H0414272 A JPH0414272 A JP H0414272A JP 11647790 A JP11647790 A JP 11647790A JP 11647790 A JP11647790 A JP 11647790A JP H0414272 A JPH0414272 A JP H0414272A
Authority
JP
Japan
Prior art keywords
laser
discharge tube
medium gas
cavity resonator
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.)
Pending
Application number
JP11647790A
Other languages
Japanese (ja)
Inventor
Hiroaki Shimazutsu
島筒 博章
Takao Abe
隆夫 阿部
Teruyuki Matsumoto
松本 輝幸
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 Heavy Industries Ltd
Original Assignee
Mitsubishi Heavy Industries 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 Mitsubishi Heavy Industries Ltd filed Critical Mitsubishi Heavy Industries Ltd
Priority to JP11647790A priority Critical patent/JPH0414272A/en
Publication of JPH0414272A publication Critical patent/JPH0414272A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To obtain large output laser light in the state that high laser oscillation efficiency is maintained, by installing a discharge tube extention part in the downstream of laser medium gas flow, which part is constituted by extending a discharge tube by a specified length determined by the pumping life of laser medium gas and the average gas flow velocity. CONSTITUTION:A discharge tube 2 is arranged so as to penetrate a cavity resonator. The length of the tube is extended by a specified length, toward the downstream of laser medium gas flow in the discharge tube from the end portion of the resonator, which specified length is determined by the pumping life tau of medium gas and the average gas flow velocity (upsilon). Hence, in the cavity resonator 1, adequate discharge suitable for laser oscillation is obtained, and the laser medium gas 6 contained in the cavity resonator 1 is utilized for laser oscillation. The laser medium gas contained in the discharge tube extention part 11 outside the cavity resonator is not heated by microwave because said gas exists outside the resonator. Said gas is in the pumping state, and therefore can be effectively used for laser oscillation.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、マイクロ波領域の電磁波によって励起される
放電を利用したレーザー発振装置に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a laser oscillation device that utilizes discharge excited by electromagnetic waves in the microwave region.

〔従来の技術〕[Conventional technology]

従来から実施されているマイクロ波を利用したレーザ発
振装置の概要を第3図によって説明する。
An outline of a conventional laser oscillation device using microwaves will be explained with reference to FIG.

第3図に於て1は空胴共振器、2は空胴共振器を貫通し
てこの内部に収容されたガラス管等の誘電体によって作
られた放電管であり、放電管2の両端部には互いに対向
して全反射鏡3と部分透過鏡4とが装置されて光共振器
を構成している。放電管2とこの放電管2の両端部を連
通させる連通管5内には、レーザ媒質ガス6が封入され
ており、このレーザ媒質ガス6は連通管5に装置された
熱交換器7によって冷却され。
In Fig. 3, 1 is a cavity resonator, 2 is a discharge tube made of a dielectric material such as a glass tube that penetrates the cavity resonator and is housed inside the cavity, and both ends of the discharge tube 2 are A total reflection mirror 3 and a partial transmission mirror 4 are arranged to face each other and constitute an optical resonator. A laser medium gas 6 is sealed in a communication tube 5 that communicates the discharge tube 2 with both ends of the discharge tube 2, and this laser medium gas 6 is cooled by a heat exchanger 7 installed in the communication tube 5. It is.

さらに送風機8によって例えば矢印方向に循環される。Further, the air is circulated by a blower 8, for example in the direction of the arrow.

9はマイクロ波発生器であり、マイクロ波発生器9から
出力されたマイクロ波は導波管(マイクロ波伝送路)1
0によって前記空胴共振器1に導かれる。なお、導波管
10はマイクロ波発生器9から出力されるマイクロ波の
伝送に適した仕様となっており、空胴共振器1はマイク
ロ波の周波数に共振するように構成されている。
9 is a microwave generator, and the microwave output from the microwave generator 9 is transmitted through a waveguide (microwave transmission line) 1.
0 into the cavity resonator 1. Note that the waveguide 10 has specifications suitable for transmitting microwaves output from the microwave generator 9, and the cavity resonator 1 is configured to resonate at the frequency of the microwaves.

すなわち、従来のレーザ発振装置は、マイクロ波発生器
9から出力されるマイクロ波電力が空胴共振器1内で共
振することによってその電界強度が高められ、放電管2
内において放電が発生する。この放電によってレーザ媒
質ガス6が励起され、全反射鏡3と部分透過鏡4との間
に光共振現象が発生し、レーザ媒質ガスの仕様によって
決まるレーザ光11が出力される。
That is, in the conventional laser oscillation device, the microwave power output from the microwave generator 9 resonates within the cavity resonator 1 to increase its electric field strength, and the discharge tube 2
Electric discharge occurs within the chamber. The laser medium gas 6 is excited by this discharge, an optical resonance phenomenon occurs between the total reflection mirror 3 and the partial transmission mirror 4, and a laser beam 11 determined by the specifications of the laser medium gas is output.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

従来のレーザー発振装置は上記のように構成されている
ので、レーザー光の高出力化に関して下記に示す問題点
がある。
Since the conventional laser oscillation device is configured as described above, there are the following problems with regard to increasing the output of laser light.

即ち、高出力のレーザー光を得る為には、空胴共振器1
に入力するマイクロ波電力を大きくするか、あるいは空
胴共振器1及び放電管2を長尺化してレーザー発振に利
用できるレーザー媒質ガス量を増加する必要がある。し
がしながら。
That is, in order to obtain high-power laser light, the cavity resonator 1
It is necessary to increase the amount of laser medium gas that can be used for laser oscillation by increasing the microwave power input to the laser oscillator, or by increasing the length of the cavity resonator 1 and the discharge tube 2. While doing so.

(1)空胴共振器1に入力するマイクロ波電力を大きく
しすぎると、レーザー媒質ガス6の温度が上昇し1例え
ばCO鵞レーザー発振装置に於ては9発振効率が低下し
て、レーザー光出力はかえって減少してしまう場合があ
る。
(1) If the microwave power input to the cavity resonator 1 is too large, the temperature of the laser medium gas 6 will rise and, for example, in a CO laser oscillator, the oscillation efficiency will decrease, causing the laser beam to become The output may actually decrease.

(2)また、空胴共振器1を長くしすぎると、放電管2
内での放電発生の不安定化、マイクロ波で加熱される領
域が長くなることによるレーザー媒質ガス6の温度上昇
等の問題が発生し。
(2) Also, if the cavity resonator 1 is made too long, the discharge tube 2
Problems such as destabilization of discharge generation within the laser medium and an increase in the temperature of the laser medium gas 6 due to the length of the region heated by microwaves occur.

発振効率が低下して、(1)と同様にレーザー光出力は
かえって減少してしまう場合がある。
The oscillation efficiency may decrease, and the laser light output may even decrease as in (1).

(3)空胴共振器1が長い状態で使用しているレーザー
発振装置はど、上記(11,+21の傾向は著しい。
(3) In a laser oscillation device in which the cavity resonator 1 is used in a long state, the above-mentioned tendency (11, +21) is remarkable.

本発明は上記問題点に鑑みてなされたもので。The present invention has been made in view of the above problems.

従来装置の欠点である6高いレーザー発振効率を保った
状態で高出力のレーザー光を得ることが困難”という問
題点を解消し、′高いレーザー発振効率を保った状態で
高出力のレーザー光を得ることができるレーザー発振装
置を提供する”ことを目的とするものである。
We have solved the problem of 6.Difficulty in obtaining high-output laser light while maintaining high laser oscillation efficiency, which is a drawback of conventional devices. The purpose is to provide a laser oscillation device that can be obtained.

〔課題を解決するための手段〕[Means to solve the problem]

すなわち本発明に係るレーザー発振装置は。 That is, the laser oscillation device according to the present invention is as follows.

マイクロ波入力の増加によるレーザー媒質ガス温度の上
昇を極小化しつつレーザー発振に利用できるレーザー媒
質ガス量を増加することによって、高いレーザー発振効
率を保った状態で高出力のレーザー光を得ることができ
るレーザー発振装置を提供するものである。即ち2本発
明は、マイクロ波領域の交播電界を発生するマイクロ波
発生器と、該マイクロ波発生器が発生するマイクロ波を
受け入れ、マイクロ波領域の交播電界強度を高める空胴
共振器と、該空胴共振器を貫通して配置され、レーザー
媒質ガスが封入されて前記マイクロ波の交播電界によっ
て放電を発生する放電管と、該放電管の一端及び他端部
との間でレーザー光を所定方向に反射させて共振させる
光共振器と、前記放電管にレーザー媒質ガスを循環供給
する連通手段とを具備してなるレーザー発振装置に於て
、前記空胴共振器端部から前記レーザー媒質ガス流れの
下流側に、レーザー媒質ガスの励起寿命と平均ガス流速
とによって定まる所定長さ部分だけ前記放電管の長さを
延長した放電管延長部を設けたことを特徴とするレーザ
ー発振装置を提供するものである。
By minimizing the rise in laser medium gas temperature due to an increase in microwave input and increasing the amount of laser medium gas that can be used for laser oscillation, it is possible to obtain high-output laser light while maintaining high laser oscillation efficiency. The present invention provides a laser oscillation device. That is, two aspects of the present invention include a microwave generator that generates an alternating electric field in the microwave region, and a cavity resonator that receives the microwaves generated by the microwave generator and increases the intensity of the alternating electric field in the microwave region. , a discharge tube that is disposed through the cavity resonator, is filled with a laser medium gas, and generates a discharge by the alternating electric field of the microwave; and one end and the other end of the discharge tube. In a laser oscillation device comprising an optical resonator that reflects light in a predetermined direction to cause resonance, and a communication means for circulating and supplying a laser medium gas to the discharge tube, Laser oscillation characterized in that a discharge tube extension part is provided on the downstream side of the laser medium gas flow, in which the length of the discharge tube is extended by a predetermined length determined by the excitation life of the laser medium gas and the average gas flow velocity. It provides equipment.

〔作用〕[Effect]

本発明のレーザー発振装置に於ては、レーザー発振に適
した適正な放電が得られるように調整された空胴共振器
を貫通して放電管が配置され、かつ放電管の長さを、空
胴共振器端部から放電管中でのレーザー媒質ガス流れの
下流側にレーザー媒質ガスの励起寿命と平均ガス流速と
によって定まる所定量だけ延長した構成となっており、
(1)空胴共振器内ではレーザー発振に適した適正な放
電が得られ、空胴共振器内部に含まれるレーザー媒質ガ
スはレーザー発振に有効に利用される。及び(2)空胴
共振器外部の延長された放電管内部に含まれるレーザー
媒質ガスはそれが空胴共振器外部にある為マイクロ波に
よって加熱されることなく、かつ励起状態にある為レー
ザー発振に有効に利用することができるものであり、こ
のため従来装置に比べて、レーザー媒質ガスが加熱され
る領域を増加させることなく、レーザー発振に有効なレ
ーザー媒質ガス量を増加させることができ、高出力のレ
ーザー光を得ることができる。
In the laser oscillation device of the present invention, the discharge tube is arranged to pass through a cavity resonator that is adjusted to obtain an appropriate discharge suitable for laser oscillation, and the length of the discharge tube is The structure extends from the end of the body resonator to the downstream side of the laser medium gas flow in the discharge tube by a predetermined amount determined by the excitation life of the laser medium gas and the average gas flow velocity.
(1) An appropriate discharge suitable for laser oscillation is obtained within the cavity resonator, and the laser medium gas contained within the cavity resonator is effectively used for laser oscillation. and (2) the laser medium gas contained inside the extended discharge tube outside the cavity resonator is not heated by the microwave because it is outside the cavity resonator, and is in an excited state, so it oscillates as a laser. Therefore, compared to conventional devices, the amount of laser medium gas effective for laser oscillation can be increased without increasing the area where the laser medium gas is heated. High-power laser light can be obtained.

〔実施例〕〔Example〕

本発明のレーザー発振装置の実施例を第1図によって説
明する。第3図と同一の番号を付したものは第3図での
それと同一機能を有する構成要素であるので、そのまま
引用し説明を割愛する。
An embodiment of the laser oscillation device of the present invention will be described with reference to FIG. Components with the same numbers as in FIG. 3 are components having the same functions as those in FIG. 3, so they will be quoted as is and their explanation will be omitted.

第1図に於て、11は本発明のレーザー発振装置の特徴
である放電管延長部であり、レーザー媒質ガス流れ方向
の下流側でかつ空胴共振器1の外側に設けられている。
In FIG. 1, reference numeral 11 denotes a discharge tube extension, which is a feature of the laser oscillation device of the present invention, and is provided on the downstream side in the flow direction of the laser medium gas and outside the cavity resonator 1.

放電管延長部の長さlは1例えばレーザー媒質ガスの励
起寿命τと放電管2内でのガス流速Vとの積τVとする
ことが考えられる。即ち、空胴共振器1内の放電管2内
に発生した放電によってレーザー発振有効エネルギー準
位に励起されたレーザー媒質ガスの平均励起寿命をτと
すると、/=τ×v内の放電管延長部11中に含まれる
レーザー媒質ガスは、平均的にレーザー発振有効エネル
ギー準位上にあり、レーザー発振に有効に利用すること
ができる。
It is conceivable that the length l of the discharge tube extension is 1, for example, the product τV of the excitation life τ of the laser medium gas and the gas flow velocity V in the discharge tube 2. That is, if the average excitation life of the laser medium gas excited to the laser oscillation effective energy level by the discharge generated in the discharge tube 2 in the cavity resonator 1 is τ, then the discharge tube extension within /=τ×v The laser medium gas contained in the portion 11 is on average above the laser oscillation effective energy level and can be effectively used for laser oscillation.

例えばCoto−レーザー質ガス(Co雪、N雪、 H
eの混合ガス)の場合の励起寿命は約1 m 式(ミリ
秒)といわれており、この時ガス流速を200m/就(
メーター7秒)であるとすれば/=200閣となる。
For example, Coto-laser gas (Co snow, N snow, H
It is said that the excitation life in the case of a mixed gas of
7 seconds), then /=200 kaku.

第2図は9本発明の効果を示す試験結果の一例であり2
図中Δ印はレーザー光出力を増大させる為に従来装置の
空胴共振器長さを(L+/)とした時のマイクロ波入力
電力(5)とレーザー光出力(5)の関係を示したもの
であり、○印は1本発明の方式によって、空胴共振器の
長さはそのままで、放電管延長部11を追加した時のも
のである。
Figure 2 is an example of test results showing the effects of the present invention.
In the figure, the Δ mark indicates the relationship between the microwave input power (5) and the laser light output (5) when the cavity length of the conventional device is set to (L+/) in order to increase the laser light output. 1, and the mark ◯ shows the result when the length of the cavity resonator remains unchanged and the discharge tube extension 11 is added according to the method of the present invention.

マイクロ波入力が大きくなると従来法によるレーザー光
出力強度と本発明の方式によるレーザー光出力強度とが
逆転し2本発明による方式の効果があられれているのが
わかる。
It can be seen that when the microwave input increases, the laser light output intensity according to the conventional method and the laser light output intensity according to the method of the present invention are reversed, indicating that the two methods according to the present invention are effective.

以上説明のレーザー発振装置に於ては、レーザー発振に
適した適正な放電が得られるように調整された空胴共振
器を貫通して放電管が配置され、かつ放電管の長さを空
胴共振器端部から放電管中でのレーザー媒質ガス流れの
下流側にレーザー媒質ガスの励起寿命τと平均ガス流速
Vとによって定まる所定量だけ延長した放電管延長部1
1を設けた構成となっているので空胴共振器1内ではレ
ーザー発振に適した適正な放電が得られ、空胴共振器内
部1に含まれるレーザー媒質ガス6はレーザー発振に利
用され、又空胴共振器外部の延長された放電管延長部1
1の内部に含まれるレーザー媒質ガス6は、それが空胴
共振器外部にある為、マイクロ波によって加熱されるこ
となく、かつ励起状態にある為レーザー発振に有効に利
用することができる。
In the laser oscillation device described above, the discharge tube is arranged to pass through the cavity resonator which is adjusted to obtain an appropriate discharge suitable for laser oscillation, and the length of the discharge tube is A discharge tube extension part 1 extends from the resonator end to the downstream side of the laser medium gas flow in the discharge tube by a predetermined amount determined by the excitation life τ of the laser medium gas and the average gas flow velocity V.
1, an appropriate discharge suitable for laser oscillation can be obtained within the cavity resonator 1, and the laser medium gas 6 contained within the cavity resonator 1 is used for laser oscillation. Extended discharge tube extension 1 outside the cavity resonator
Since the laser medium gas 6 contained inside the cavity 1 is outside the cavity resonator, it is not heated by the microwaves and is in an excited state, so it can be effectively used for laser oscillation.

即ち、このような構成にしたことにより従来装置に比べ
て、レーザー媒質ガス6が加熱される領域を増加させる
ことなく、レーザー発振に有効なレーザー媒質ガス量を
増加させることができ、高出力のレーザー光を得ること
ができるものである。
That is, by adopting such a configuration, compared to the conventional device, it is possible to increase the amount of laser medium gas effective for laser oscillation without increasing the area where the laser medium gas 6 is heated. It is possible to obtain laser light.

〔発明の効果〕〔Effect of the invention〕

本発明のレーザー発振装置によれば、出力レーザー強度
を増加させる際に、放電管延長部を設けたことにより空
胴共振器を大きくすることなくマイクロ波入力の増加に
よるレーザー媒質ガス温度の上昇を極小化しつつレーザ
ー発振に利用できるレーザー媒質ガス量を増加させるこ
とができるので、高いレーザー発振効率を保った状態で
高出力のレーザー光を得ることが出来るものである。
According to the laser oscillation device of the present invention, when increasing the output laser intensity, the increase in laser medium gas temperature due to an increase in microwave input can be prevented without enlarging the cavity resonator by providing the discharge tube extension. Since it is possible to increase the amount of laser medium gas that can be used for laser oscillation while minimizing the amount, it is possible to obtain high-output laser light while maintaining high laser oscillation efficiency.

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

第1図は9本発明の実施例に係るレーザー発振装置の基
本構成図、第2図は本発明の効果を示す試験結果例を示
すグラフ、第3図は従来装置の基本構成図である。 1・・・空胴共振器、2・・・放電管、5・・・連通管
。 6・・・レーザー媒質ガス、9・・・マイクロ波発生器
。 10・・導波管(マイクロ波電送路)、11・・・放電
管延長部。
FIG. 1 is a basic configuration diagram of a laser oscillation device according to an embodiment of the present invention, FIG. 2 is a graph showing an example of test results showing the effects of the present invention, and FIG. 3 is a basic configuration diagram of a conventional device. 1...Cavity resonator, 2...Discharge tube, 5...Communication tube. 6...Laser medium gas, 9...Microwave generator. 10... Waveguide (microwave transmission line), 11... Discharge tube extension.

Claims (1)

【特許請求の範囲】[Claims] マイクロ波領域の交播電界を発生するマイクロ波発生器
と、該マイクロ波発生器が発生するマイクロ波を受け入
れ、マイクロ波領域の交播電界強度を高める空胴共振器
と、該空胴共振器を貫通して配置され、レーザー媒質ガ
スが封入されて前記マイクロ波の交播電界によって放電
を発生する放電管と、該放電管の一端及び他端部との間
でレーザー光を所定方向に反射させて共振させる光共振
器と、前記放電管にレーザー媒質ガスを循環供給する連
通手段とを具備してなるレーザー発振装置に於て、前記
空胴共振器端部から前記レーザー媒質ガス流れの下流側
にレーザー媒質ガスの励起寿命と平均ガス流速とによっ
て定まる所定長さ部分だけ前記放電管の長さを延長した
放電管延長部を設けたことを特徴とするレーザー発振装
置。
A microwave generator that generates an alternating electric field in the microwave region; a cavity resonator that receives the microwaves generated by the microwave generator and increases the intensity of the alternating electric field in the microwave region; and the cavity resonator. a discharge tube that is placed through the tube, is filled with a laser medium gas, and generates a discharge by the alternating electric field of the microwave, and reflects the laser light in a predetermined direction between one end and the other end of the discharge tube. In the laser oscillation device, the laser oscillation device is equipped with an optical resonator for resonating and a communication means for circulating and supplying a laser medium gas to the discharge tube, in which a downstream side of the laser medium gas flow from an end of the cavity resonator is provided. A laser oscillation device characterized in that a discharge tube extension section is provided on the side thereof, the discharge tube extension section extending the length of the discharge tube by a predetermined length determined by the excitation life of the laser medium gas and the average gas flow velocity.
JP11647790A 1990-05-02 1990-05-02 Laser oscillating equipment Pending JPH0414272A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP11647790A JPH0414272A (en) 1990-05-02 1990-05-02 Laser oscillating equipment

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP11647790A JPH0414272A (en) 1990-05-02 1990-05-02 Laser oscillating equipment

Publications (1)

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JPH0414272A true JPH0414272A (en) 1992-01-20

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JP11647790A Pending JPH0414272A (en) 1990-05-02 1990-05-02 Laser oscillating equipment

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Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE19625603A1 (en) * 1995-06-27 1997-01-02 Matsushita Electric Ind Co Ltd Microwave pumped gas, e.g. carbon di:oxide, laser oscillator for industrial use

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE19625603A1 (en) * 1995-06-27 1997-01-02 Matsushita Electric Ind Co Ltd Microwave pumped gas, e.g. carbon di:oxide, laser oscillator for industrial use
US5706305A (en) * 1995-06-27 1998-01-06 Matsushita Electric Industrial Co., Ltd. Gas laser oscillating apparatus for discharging laser beam by exciting gas with microwave
DE19625603C2 (en) * 1995-06-27 2001-10-11 Matsushita Electric Ind Co Ltd Gas laser for emitting a laser beam due to the excitation of gas by means of microwaves

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