JPS6021583A - Gas laser oscillating device - Google Patents

Gas laser oscillating device

Info

Publication number
JPS6021583A
JPS6021583A JP12794483A JP12794483A JPS6021583A JP S6021583 A JPS6021583 A JP S6021583A JP 12794483 A JP12794483 A JP 12794483A JP 12794483 A JP12794483 A JP 12794483A JP S6021583 A JPS6021583 A JP S6021583A
Authority
JP
Japan
Prior art keywords
mirror
laser
housing
contracting
envelope
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
JP12794483A
Other languages
Japanese (ja)
Inventor
Akira Wada
和田 昭
Hiroyuki Sugawara
宏之 菅原
Koji Kuwabara
桑原 皓二
Sei Takemori
竹森 聖
Hiroharu Sasaki
弘治 佐々木
Makoto Yano
眞 矢野
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.)
Hitachi Ltd
Original Assignee
Hitachi 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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP12794483A priority Critical patent/JPS6021583A/en
Publication of JPS6021583A publication Critical patent/JPS6021583A/en
Pending 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
    • H01S3/05Construction or shape of optical resonators; Accommodation of active medium therein; Shape of active medium
    • H01S3/08Construction or shape of optical resonators or components thereof
    • H01S3/081Construction or shape of optical resonators or components thereof comprising three or more reflectors
    • H01S3/0818Unstable resonators

Landscapes

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

Abstract

PURPOSE:To facilitate the dust-proof and moisture-proof treatment of the surface of a contracting reflection mirror and to miniaturize the titled device by a method wherein this device is equipped with the contracting reflection concave mirror of the laser resonator inside the body of housing, and the contracting convex mirror inside the projection on the side of the housing. CONSTITUTION:The concave mirror 13 is placed in the cylindrical body 24 of the housing 2, and the convex mirror 15 that receives the reflected light of the mirror 13 in the swell-out projection 2B on the side of the package. The contraction of the flux of light is carried out inside the housing 2, and, in addition to the miniaturization of the whole device, the mirrors of the contraction system do not become cloudy; therefore the decrease of laser output is prevented. Since a contracted laser beam 6d passes through an output window 9, and the diameter of the window 9 can be reduced, the expensive material of a crystal plate 9 can be saved.

Description

【発明の詳細な説明】 〔発明の利用分野〕 この発明は高出力ガスレーザ発信装置の出力ビーム取り
出し部の改良に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Application of the Invention] The present invention relates to an improvement in the output beam extraction section of a high-power gas laser transmitter.

〔発明の背景〕[Background of the invention]

高効率で集束性の良いビーム金得るには不安定形共振器
の構成が一般に採用されている。
In order to obtain a beam with high efficiency and good focusing, an unstable resonator configuration is generally adopted.

ガスレーザ装置ではその出力を高めるために、レーザ媒
質部の容積を増大することによって、ピームロ径を大き
くしている。
In order to increase the output of a gas laser device, the volume of the laser medium section is increased to increase the diameter of the beam.

第1図は従来の高出力ガスレーザ装置の構造を説明する
ものである。
FIG. 1 illustrates the structure of a conventional high-power gas laser device.

図において1はレーザ媒質で、CO2、N2 。In the figure, 1 is the laser medium, which is CO2 and N2.

)1eなどが使用される。2は媒質全封入した外囲器で
ある。外囲器は細長い円筒状の本体部2Aと、本体部の
一部を側方に膨出せしめて形成した突出部2Bとから成
る。本体部2人の内部には、一端に凹面鏡3が、他端に
凸面鏡4が、レーザ光6を発生する反射鏡として、鏡軸
が一致するように配置しである。前記の2個の反射鏡の
中間には円環状の平面鏡5が鏡軸を45°下方に傾けた
姿勢で配置されている。この平面鏡5の中央の円形窓7
をレーザ光6が通過し、平面鏡5の円猿部8がレーザ光
6の一部を反射して平行光束のレーザ光6aとなす。レ
ーザ光6aは外囲器の突出部2Bに取付けである結晶板
9を透過して器外に放出されレーザ光6bとなる。レー
ザ光6bは凹面鏡10に入射し、反射して収れん光束の
レーザ光6Cとなり、凸面鏡11に入射し、その反射光
6dは所定の割合に縮小された平行光束のレーザ光とな
って加工用集光装置に照射され、集光されて切断加工や
溶接に使用される。
) 1e etc. are used. 2 is an envelope in which the medium is completely enclosed. The envelope consists of an elongated cylindrical main body 2A and a protrusion 2B formed by bulging a part of the main body laterally. Inside the two main bodies, a concave mirror 3 at one end and a convex mirror 4 at the other end are arranged as reflecting mirrors for generating laser light 6 so that their mirror axes coincide. An annular plane mirror 5 is arranged between the two reflecting mirrors with its mirror axis tilted downward by 45 degrees. A circular window 7 in the center of this plane mirror 5
The laser beam 6 passes through, and the circular portion 8 of the plane mirror 5 reflects a part of the laser beam 6 to form a parallel beam of laser beam 6a. The laser beam 6a is transmitted through a crystal plate 9 attached to the protruding portion 2B of the envelope, and is emitted outside the device to become a laser beam 6b. The laser beam 6b enters the concave mirror 10, is reflected, becomes a convergent beam of laser beam 6C, and enters the convex mirror 11, and the reflected beam 6d becomes a parallel beam of laser beam reduced to a predetermined ratio and is focused for processing. The light is irradiated by an optical device, focused, and used for cutting and welding.

上記の構成では、ビーム縮小用の凹面鏡10と凸面鏡1
1が外囲器2の外にあるため、レーザ装置の全体が大型
になり、かつ、縮小用の2面の反射鏡10と11の鏡面
の防塵、防湿が困難であることが欠点である。
In the above configuration, a concave mirror 10 and a convex mirror 1 for beam reduction are used.
1 is outside the envelope 2, the laser device as a whole becomes large-sized, and it is difficult to keep the mirror surfaces of the two mirrors 10 and 11 for reduction dust-proof and moisture-proof.

本発明は次に述べる構成によって上記の欠点を除いたも
のである。
The present invention eliminates the above-mentioned drawbacks by the following configuration.

〔発明の概要〕[Summary of the invention]

本発明の特徴は、第2図に示したように、円環状反射鏡
に形成された縮小用の凹面鏡12を外囲器2の円筒状本
体部2人内に設置し、凹面鏡12の反射光を受ける縮小
用の凸面鏡15を外囲器側方の膨出突出部2B内に設置
した点にある。
The feature of the present invention is that, as shown in FIG. A convex mirror 15 for receiving the reduction is installed inside the bulging protrusion 2B on the side of the envelope.

〔発明の実施例〕 凹面鏡12と凸面鏡15との相対的配置は第1図に示し
た従来の装置における凹面鏡1oと凸面鏡11の相対的
配置と同様である。
[Embodiment of the Invention] The relative arrangement of the concave mirror 12 and the convex mirror 15 is the same as the relative arrangement of the concave mirror 1o and the convex mirror 11 in the conventional device shown in FIG.

しかし、光束の縮小が第1図の従来の装置では外囲器2
の外で行われるのに対し、第2図の本発明装置では外囲
器2の内部で行われるから、レーザ光発振装置の全体が
小型となるほか、縮小系の反射鏡に曇りを生じないから
レーザ出力の低下が防止される効果がある。
However, in the conventional device shown in FIG.
In contrast, in the device of the present invention shown in FIG. 2, the laser beam oscillation is performed inside the envelope 2, which makes the entire laser beam oscillation device compact, and does not cause fogging on the reflecting mirror of the reduction system. This has the effect of preventing a decrease in laser output.

々お、従来の装置では縮小前のレーザ光6aが出力窓9
を透過したが、本発明装置では縮小されたレーザ光6d
が出力窓9を透過する。
In the conventional device, the laser beam 6a before reduction is output through the output window 9.
However, in the device of the present invention, the laser beam 6d was reduced.
is transmitted through the output window 9.

〔発明の効果〕〔Effect of the invention〕

出力窓9となる結晶板はZ nI Seなどの特殊の結
晶体全材料とする高価なものである。本発明によれば出
力窓9の直径が小さくなるので結晶板9の高価々材料を
節約できる効果もある。
The crystal plate serving as the output window 9 is an expensive one made entirely of a special crystal material such as Z nI Se. According to the present invention, since the diameter of the output window 9 is reduced, there is also the effect that the expensive material of the crystal plate 9 can be saved.

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

第1図は従来のガスレーザ発振装置の縦断面図。 第2図は本発明のガスレーザ発振装置の縦断面図である
。 2・・・外囲器、3.10・・・凹面鏡、4,11.1
5・・・凸面鏡。 代理人 弁理士 高橋明夫 A
FIG. 1 is a longitudinal sectional view of a conventional gas laser oscillation device. FIG. 2 is a longitudinal sectional view of the gas laser oscillation device of the present invention. 2... Envelope, 3.10... Concave mirror, 4, 11.1
5... Convex mirror. Agent Patent Attorney Akio Takahashi A

Claims (1)

【特許請求の範囲】[Claims] 1、 レーザ媒質を封入した外囲器内にレーザビームを
共振させる反射鏡を対置したレーザ共振器において、円
環状反射鏡に形成された縮小用の凹面鏡を外囲器の円筒
状本体部内に設置し、前記の凹面鏡の反射光が入射する
縮小用の凸面鏡を外囲器側方の膨出突出部内に設置した
ことを特徴とするガスレーザ発振装置。
1. In a laser resonator in which a reflecting mirror for resonating a laser beam is placed oppositely within an envelope enclosing a laser medium, a concave mirror for reduction formed in an annular reflecting mirror is installed inside the cylindrical main body of the envelope. A gas laser oscillation device characterized in that a reduction convex mirror into which the reflected light from the concave mirror is incident is installed in a bulging protrusion on the side of the envelope.
JP12794483A 1983-07-15 1983-07-15 Gas laser oscillating device Pending JPS6021583A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP12794483A JPS6021583A (en) 1983-07-15 1983-07-15 Gas laser oscillating device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP12794483A JPS6021583A (en) 1983-07-15 1983-07-15 Gas laser oscillating device

Publications (1)

Publication Number Publication Date
JPS6021583A true JPS6021583A (en) 1985-02-02

Family

ID=14972494

Family Applications (1)

Application Number Title Priority Date Filing Date
JP12794483A Pending JPS6021583A (en) 1983-07-15 1983-07-15 Gas laser oscillating device

Country Status (1)

Country Link
JP (1) JPS6021583A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2004099831A3 (en) * 2003-04-30 2005-02-03 Visi Image Inc Laser mirror housing

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2004099831A3 (en) * 2003-04-30 2005-02-03 Visi Image Inc Laser mirror housing

Similar Documents

Publication Publication Date Title
US5359622A (en) Radial polarization laser resonator
US5216687A (en) Solid state laser device with a bi-cylindrical covexo-convex lens having selected radii of curvature to preferably pump a region of a laser medium
JPS6021583A (en) Gas laser oscillating device
US4096447A (en) Unstable resonator laser system
EP0957546A2 (en) solid-state laser device and solid-state laser amplifier provided therewith
JPH0563263A (en) Semiconductor laser-pumped solid-state laser device
JP5135650B2 (en) Laser equipment
JPS6037628B2 (en) gas laser oscillator
JPS60239078A (en) Solid-state laser oscillator
JPS5843420A (en) External optical device for laser
CN220122323U (en) High-power high-purity tunable single-frequency vortex laser
US4683576A (en) Optical pumping laser system
US4577324A (en) High power output laser apparatus
JPS6028287A (en) Laser generator
JPS63254776A (en) Solid-state laser device
JPH06350168A (en) Solid-state laser oscillator
JPH07176811A (en) Laser resonator
JPS5855663Y2 (en) Laser oscillation device
JP3493373B2 (en) Laser oscillator
SU1597014A1 (en) Resonator of free-electron laser
JPH11177165A (en) Light excitation method for solid state laser
JPH03245582A (en) Semiconductor laser excitation solid-state laser
JPH03217064A (en) Excited light resonance type laser
JPS63141382A (en) Solid state laser oscillator
JPH0337247Y2 (en)