JPS58165387A - Mirror supporting structure for laser oscillator - Google Patents
Mirror supporting structure for laser oscillatorInfo
- Publication number
- JPS58165387A JPS58165387A JP4743982A JP4743982A JPS58165387A JP S58165387 A JPS58165387 A JP S58165387A JP 4743982 A JP4743982 A JP 4743982A JP 4743982 A JP4743982 A JP 4743982A JP S58165387 A JPS58165387 A JP S58165387A
- Authority
- JP
- Japan
- Prior art keywords
- case
- mirror
- output
- gap
- laser
- 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
- H01S3/05—Construction or shape of optical resonators; Accommodation of active medium therein; Shape of active medium
- H01S3/08—Construction or shape of optical resonators or components thereof
- H01S3/08059—Constructional details of the reflector, e.g. shape
-
- 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
- H01S3/034—Optical devices within, or forming part of, the tube, e.g. windows, mirrors
Landscapes
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Lasers (AREA)
- Engineering & Computer Science (AREA)
- Plasma & Fusion (AREA)
- Optics & Photonics (AREA)
Abstract
Description
【発明の詳細な説明】
本発明は出カバ9−の大きな炭酸ガスレーザに好適なレ
ーザ発振器のミラー支持装置に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a mirror support device for a laser oscillator suitable for a carbon dioxide laser with a large output cover 9-.
一般に炭酸ガスレーザ発振器は、第1図、8に2図を用
いて説明すると、炭酸ガス、窒素ガス、ヘリウムガス等
の混合ガス6を放電管4内に充填し、放電管内に設けら
れた陰極と陽極とからなる電極3間でグロー放電を行う
と、混合ガスが励起されてレーず光音発生する。レーザ
光は放電管両端に設&Jられた鏡開で共振し、一方の鏡
である出力鏡12に介してレーず出力8として外11K
取出される。出力鏡12はゲルマニウム中セレン化亜鉛
などの結晶体で形bl[れている、民力鏡12はレーザ
光8が共振並びに透過することにより温度上昇するので
、ケース10内に冷却路を設けて、水などの冷却媒体9
を出力f/Ia12υ外周にまわすことにより1.11
1J&上昇を防止し、結晶体の熱破壊を防止している。In general, a carbon dioxide laser oscillator is explained using FIGS. 1, 8 and 2. A discharge tube 4 is filled with a mixed gas 6 of carbon dioxide, nitrogen gas, helium gas, etc., and a cathode and When glow discharge is performed between the electrode 3 and the anode, the mixed gas is excited and a laser beam sound is generated. The laser light resonates with mirror openings installed at both ends of the discharge tube, and is transmitted through one mirror, the output mirror 12, to the outside as a laser output of 8.
taken out. The output mirror 12 is made of a crystal material such as zinc selenide in germanium. Since the temperature of the Minriki mirror 12 increases due to resonance and transmission of the laser beam 8, a cooling path is provided in the case 10. Cooling medium 9 such as water
1.11 by rotating around the output f/Ia12υ
1J & rise and prevent thermal destruction of the crystal.
しρ為し、結晶体の結晶欠陥や出力鏡が冷却されている
ことにより、室温との温度差による結藤が生じ、結果と
して空気中の臘埃が付着し、また共ms内部の農機も皆
無でないことから、出力鏡表面に異物が付着し、レーザ
発振を行うことにより品分発熱を生じ、結晶体内の熱応
力による割れを生じてI!また。However, due to crystal defects in the crystal and the output mirror being cooled, dust formation occurs due to the temperature difference from room temperature, and as a result, dust in the air adheres to the agricultural machinery inside the ms. Since there is no foreign matter attached to the surface of the output mirror, laser oscillation causes part heat generation, which causes cracks due to thermal stress within the crystal, causing I! Also.
この結末、冷却媒体9が、発振器内sK侵入し内部汚損
を生じる欠点があった。この解決策として、出力−12
外j11t−直接冷却媒体9により冷却する方法でなく
、jllK3図に示す如く、間接的にミラーケース1O
−2を介して冷却する方法があるが、従来、レーザ出力
が数キロワット以上になると熱破壊する欠点があった。As a result, the cooling medium 9 enters the oscillator sK, causing internal contamination. As a solution, output −12
Outside j11t - Instead of cooling directly with the cooling medium 9, as shown in Figure jllK3, the mirror case 1O is indirectly cooled.
There is a method of cooling the laser via -2, but conventionally this method has had the drawback of thermal breakdown when the laser output exceeds several kilowatts.
特にミラーケース周辺の温度上昇もその一因であった。In particular, the rise in temperature around the mirror case was a contributing factor.
こnは、レーザ光軸が必ずしもミラーケースlOの中心
にあるとは限らず、周辺にぶつかることによる発熱と、
レーザ光自身の拡散によるケース照射発熱である。This is because the laser optical axis is not necessarily at the center of the mirror case IO, and heat generation due to collision with the periphery occurs.
This is heat generated by irradiation of the case due to the diffusion of the laser beam itself.
本発明の目的は、間接的な冷却方法にあってもミラーケ
ース周辺の温度上昇を防止するケース構造を提供するこ
とKある。SUMMARY OF THE INVENTION An object of the present invention is to provide a case structure that prevents temperature rise around the mirror case even when an indirect cooling method is used.
以下、本発明の実施例を図面に示す出力鏡部IKより説
明する。Hereinafter, embodiments of the present invention will be explained from the output mirror section IK shown in the drawings.
出力鏡12は支持ケース10−2と10−3に、:1”
・
より挾持されており、熱伝導を良くする為に熱伝111
1:
導材13を介して、冷却木本どの冷却媒体9が円周方向
にまわり出力鏡を間目的に冷却している。The output mirror 12 is attached to the support cases 10-2 and 10-3.
・It is more sandwiched and heat transfer 111 is used to improve heat conduction.
1: A cooling medium 9, such as a cooling wood, circulates in the circumferential direction via the conductor 13 to cool the output mirror.
、−”し1゜
熱伝導材13は、インジウムなどの硬度の低い材質で、
熱伝導率が大きいことが望ましく、バッキング11−1
で抑えつけておく。通常発振器内部は電圧であることか
ら、シールを兼ねて使うか、別途パツキンにより7−ル
する構造をとることもめる。レーザ出力8は内部で共振
し曳結果として、出力される。このと龜、出力鏡部1と
全反射鏡部2を調整し光軸合わせt行ない出力鏡12の
中心に、レーザ出力8の光中心が出来る様に調整するが
、巌酸ガスレーザは波長がほぼ10.611mの非可視
光領域で6L光軸が、出力鏡12並びにケース1Gの中
心に一致する様KI4整する迄に、レーザ光がケース1
Gの周辺に照射されて発熱することがあり、また、光軸
合せ完了後であっても、ミラー中支持金臭の熱変形によ
りレーザ光とフランジ中心は外れて≦る。又、レーザ光
自身も一定角の拡散がある。従って、レーザ出力8とオ
フ−ケース10−1間に長さXのギャップをとり、し、
′
一ザ出力が内縦#ア・直進した場合の2ラーケース10
−3とレーザー、カ間ギャップ(レーザ光11y。, -"1° The heat conductive material 13 is made of a material with low hardness such as indium,
It is desirable that the thermal conductivity is high, and the backing 11-1
Keep it in check. Since there is usually a voltage inside the oscillator, it may also be used as a seal, or it may be structured to be sealed with a separate seal. The laser output 8 resonates internally and is output as a result of the pulling. At this point, the output mirror section 1 and the total reflection mirror section 2 are adjusted to align the optical axis so that the optical center of the laser output 8 is placed at the center of the output mirror 12. By the time the KI4 is adjusted so that the 6L optical axis coincides with the center of the output mirror 12 and the case 1G in the non-visible light region of 10.611 m, the laser beam is transferred to the case 1.
The periphery of G may be irradiated and generate heat, and even after the optical axis alignment is completed, the laser beam and the center of the flange may deviate from each other due to thermal deformation of the support metal inside the mirror. Further, the laser light itself has a certain angle of diffusion. Therefore, a gap of length X is taken between the laser output 8 and the off-case 10-1, and
′2 case 10 when the output is inward vertical #A and straight forward
Gap between -3 and laser (laser beam 11y).
・1・、・ ケース1111t)Y+Xtとる様に構成する。・1・、・ Case 1111t) It is configured to take Y+Xt.
この様にミラーケース10−3とV−ザ出力間にギャッ
プをとり、かつ共振器側のギャップXよりも出力側ギャ
ップy+tが大きいので、レーザ出力86光軸中心がミ
ラーケース゛10−1の中心を外nた場合におっても、
ミラーケース10−3とレーザ出力8にはギャップtが
あるので、ケースにぶつかり発熱することはない。
−このように本発明によれば、出力鏡がミラーケース
の発熱による熱歪を生じることがなく、出力鏡の割れを
防止できる。In this way, there is a gap between the mirror case 10-3 and the V-laser output, and since the output side gap y+t is larger than the gap X on the resonator side, the optical axis center of the laser output 86 is the center of the mirror case 10-1. Even if you exclude
Since there is a gap t between the mirror case 10-3 and the laser output 8, the mirror case 10-3 will not collide with the case and generate heat.
- Thus, according to the present invention, the output mirror does not undergo thermal distortion due to heat generated by the mirror case, and cracking of the output mirror can be prevented.
図面の簡単な説明 ′第1図はレ
ーザ発振器の概略側断面、第2図は従来の出力鏡−概略
側断面図、゛第3図は本発明の出力碗部概略側断面図で
ある。BRIEF DESCRIPTION OF THE DRAWINGS Figure 1 is a schematic side sectional view of a laser oscillator, Figure 2 is a schematic side sectional view of a conventional output mirror, and Figure 3 is a schematic side sectional view of the output bowl of the present invention.
1・・・出力鏡部、2・・・全反射鏡部、3・・・電極
、4・・・放電管、8・・・レーザ出力、10・・・ミ
ラーケース、−18
第2図DESCRIPTION OF SYMBOLS 1... Output mirror part, 2... Total reflection mirror part, 3... Electrode, 4... Discharge tube, 8... Laser output, 10... Mirror case, -18 Fig. 2
Claims (1)
端に設けられた少くとも一対の鏡と、放電管本体内圧設
けられた陰極と陽極を有する電極と、該電極間で放電を
行い混合ガスをレーザ光に変換し、かつ両鏡間で共振し
てレーザ光として外部に取出す一方の鏡の支持物とから
成るものにおいて、上記支持物の内径穴部が、レーザ光
共振器側よりも、外部レーザ光取り出し側が大なること
を特徴とし九レーザ発振器の非判吻12−支持構造。1. A discharge tube body filled with a mixed gas, at least a pair of mirrors provided at both ends of the discharge tube body, an electrode having a cathode and an anode provided within the discharge tube body, and a discharge being generated between the electrodes. and a support for one of the mirrors that converts a mixed gas into laser light and emits the laser light to the outside through resonance between the two mirrors, with the inner diameter hole of the support being closer to the laser light resonator side. Also, the non-proboscis 12-support structure of the nine laser oscillators is characterized in that the external laser beam extraction side is large.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP4743982A JPS58165387A (en) | 1982-03-26 | 1982-03-26 | Mirror supporting structure for laser oscillator |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP4743982A JPS58165387A (en) | 1982-03-26 | 1982-03-26 | Mirror supporting structure for laser oscillator |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS58165387A true JPS58165387A (en) | 1983-09-30 |
Family
ID=12775178
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP4743982A Pending JPS58165387A (en) | 1982-03-26 | 1982-03-26 | Mirror supporting structure for laser oscillator |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS58165387A (en) |
-
1982
- 1982-03-26 JP JP4743982A patent/JPS58165387A/en active Pending
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