JPH0789591B2 - Carbon dioxide laser device - Google Patents
Carbon dioxide laser deviceInfo
- Publication number
- JPH0789591B2 JPH0789591B2 JP59131692A JP13169284A JPH0789591B2 JP H0789591 B2 JPH0789591 B2 JP H0789591B2 JP 59131692 A JP59131692 A JP 59131692A JP 13169284 A JP13169284 A JP 13169284A JP H0789591 B2 JPH0789591 B2 JP H0789591B2
- Authority
- JP
- Japan
- Prior art keywords
- mirror
- carbon dioxide
- resonator
- laser device
- degrees
- 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
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
- H01S3/005—Optical devices external to the laser cavity, specially adapted for lasers, e.g. for homogenisation of the beam or for manipulating laser pulses, e.g. pulse shaping
Landscapes
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Engineering & Computer Science (AREA)
- Plasma & Fusion (AREA)
- Optics & Photonics (AREA)
- Lasers (AREA)
Description
【発明の詳細な説明】 〔発明の技術分野〕 この発明は大出力の炭酸ガスレーザ装置に係り、特にそ
の出力レーザ光の偏光特性の改善に関する。Description: TECHNICAL FIELD OF THE INVENTION The present invention relates to a high-power carbon dioxide laser device, and more particularly to improvement of polarization characteristics of its output laser light.
従来、大出力の炭酸ガスレーザ装置は、第3図及び第4
図に示すようにエンドミラー1と出力ミラー2から共振
器3が構成されている。第3図では、(b)に示すよう
なランダム偏光レーザ光4が得られ、第4図では共振器
3内にブリユスターウインドウ5を設けて(b)に示す
ような直線偏光レーザ光6を得ている。この直線偏光レ
ーザ光6を円偏光に変換する方法が、第5図に示してあ
る。Conventionally, a high-power carbon dioxide laser device is shown in FIGS.
As shown in the figure, the end mirror 1 and the output mirror 2 constitute a resonator 3. In FIG. 3, a randomly polarized laser light 4 as shown in FIG. 3B is obtained, and in FIG. 4 a linearly polarized laser light 6 as shown in FIG. Is getting A method of converting the linearly polarized laser light 6 into circularly polarized light is shown in FIG.
従来の炭酸ガスレーザ装置においては、第4図に示した
ように、ブリユスターウインドウ5を設け、そのブリユ
スターウインドウ5の光の偏光面の違いによる透過率の
違いにより、レーザ共振光の偏光面を決定していた。し
かしながら、レーザ出力が高くなり、又、炭酸ガスレー
ザのように波長が10.6μmと長くなると、一般のガラス
材が用いられず、特殊な材料(ZnSe等)を用いる必要が
ある。共振エネルギーが高くなると、このブリユスター
ウインドウ5を通過するエネルギーを多くなり、従つて
ブリユスターウインドウ5が吸収するエネルギーが増大
する。そのため、このブリユスターウインドウ材が光学
的熱歪を受け、共振器3の構成を狂わせ、レーザ出力の
低下、発振横モードの変化をもたらすことがあつた。In a conventional carbon dioxide gas laser device, as shown in FIG. 4, a Brüster window 5 is provided, and the polarization of the laser resonance light is changed by the difference in the transmittance due to the difference in the polarization plane of the light of the Brüster window 5. I had decided on the plane. However, when the laser output becomes high and the wavelength becomes long at 10.6 μm like a carbon dioxide gas laser, a general glass material is not used and it is necessary to use a special material (ZnSe or the like). When the resonance energy becomes high, the energy passing through the Brewster window 5 increases, and the energy absorbed by the Brewster window 5 increases accordingly. For this reason, this Brüster window material may be subjected to optical thermal strain, causing the configuration of the resonator 3 to be disturbed, resulting in a reduction in laser output and a change in oscillation transverse mode.
又、第5図に示したように、直線偏光のレーザ光6の円
偏光のレーザ光8への変換においても、1/4波長板7を
用いて行なつていたが、この場合も上記ブリユスターウ
インドウ5と同じような不具合を生じると共に、その熱
負荷のため、破壊されてしまう場合もあつた。Further, as shown in FIG. 5, the conversion of the linearly polarized laser light 6 into the circularly polarized laser light 8 was also performed using the 1/4 wavelength plate 7. In addition to causing the same problems as the Uster window 5, it may be destroyed due to the heat load.
この発明の目的は、上記従来の問題点を解消し、きれい
な円偏光の大出力炭酸ガスレーザ光が得られる炭酸ガス
レーザ装置を提供することである。It is an object of the present invention to provide a carbon dioxide gas laser device which solves the above-mentioned conventional problems and is capable of obtaining a high-power carbon dioxide gas laser beam of clean circularly polarized light.
この発明は、管軸がL字状の管の両端部にそれぞれエン
ドミラーおよび出力ミラーを備え、前記管の内部であっ
て、前記出力ミラー近くに入射角および反射角が30度〜
60度となるように光軸を折り曲げる折曲げ反射ミラーが
配置された一体構成の炭酸ガスレーザ共振器と、この共
振器の出力ミラー近くの光路上に入射角が45度となるよ
うに配置された1/4波長変換ミラーとからなる炭酸ガス
レーザ装置である。According to the present invention, an end mirror and an output mirror are provided at both ends of a tube having an L-shaped tube axis, and inside the tube, an incident angle and a reflection angle are 30 degrees to near the output mirror.
An integrated carbon dioxide gas laser resonator with a bending reflection mirror that bends the optical axis to 60 degrees, and an incident angle of 45 degrees on the optical path near the output mirror of this resonator. A carbon dioxide laser device consisting of a 1/4 wavelength conversion mirror.
この発明の炭酸ガスレーザ装置は第1図に示すようにな
り、従来例と同一箇所は同一符号を付すと、共振器3は
管軸がL字状の管の両端部にそれぞれエンドミラー1と
出力ミラー2により構成されている。そして、この共振
器3の内部の角部、すなわち上記出力ミラー2の近くに
は、折曲げ反射ミラー9がその入射角及び反射角が30゜
〜60゜、例えば45゜になるように配設されている。更
に、共振器3の外部、即ち上記出力ミラー2の近くの光
路上には、45゜の入射角に設定された1/4波長変換ミラ
ー10が設けられている。The carbon dioxide gas laser device of the present invention is as shown in FIG. 1. When the same parts as those in the conventional example are designated by the same reference numerals, the resonator 3 outputs the end mirror 1 and the output to the both ends of the tube having the L-shaped tube axis. It is composed of a mirror 2. A bending reflection mirror 9 is disposed near the output mirror 2 at a corner inside the resonator 3 so that the incident angle and the reflection angle are 30 ° to 60 °, for example 45 °. Has been done. Further, a 1/4 wavelength conversion mirror 10 set at an incident angle of 45 ° is provided outside the resonator 3, that is, on the optical path near the output mirror 2.
動作時には、折曲げ反射ミラー9により共振におけるレ
ーザ光の偏光面が決定される。これは、P偏光、S偏光
により反射率が違うことと、炭酸ガスレーザでは発振の
ゲインが高いことにより、決定させるものである。その
P偏光、S偏光における反射の特性曲線を第2図に示し
た。次に、1/4波長変換ミラー10により、共振器3から
射出された直線偏光のレーザ光6は、1/4波長変換ミラ
ー10により偏光面の回転作用を受け、円偏光のレーザ光
8に変換される。During operation, the folding reflection mirror 9 determines the plane of polarization of the laser light at resonance. This is determined because the reflectance differs depending on the P-polarized light and the S-polarized light and the oscillation gain is high in the carbon dioxide laser. The characteristic curves of reflection in the P-polarized light and the S-polarized light are shown in FIG. Next, the 1/4 wavelength conversion mirror 10 causes the linearly polarized laser beam 6 emitted from the resonator 3 to undergo a rotation action of the plane of polarization by the 1/4 wavelength conversion mirror 10, and becomes a circularly polarized laser beam 8. To be converted.
この発明によれば、従来のように光学部品、特にブリユ
スターウインドウ5及び1/4波長板7に対して大きな熱
負荷を与えることなく、折曲げ反射ミラー9を共振器内
部に1枚、1/4波長変換ミラー10をレーザ出射直後に1
枚、それぞれ設けることにより、簡単に円偏光の炭酸ガ
スレーザ光を得ることができ、そのレーザ光の加工等へ
の応用の効果は大である。According to the present invention, one bending reflection mirror 9 is provided inside the resonator without giving a large heat load to the optical components, particularly the Brüster window 5 and the quarter-wave plate 7, as in the conventional case. 1/4 wavelength conversion mirror 10 immediately after laser emission
Circularly polarized carbon dioxide laser light can be easily obtained by providing each one, and the effect of applying the laser light to processing or the like is great.
又、この発明では、上記機能を出力ミラー2付近に集結
したため、全機能のユニツト化が可能となつた。更に一
体構造としたため、直線偏光面と1/4波長変換ミラー10
との位置関係を機械的精度で設定することができた。こ
の一体構造のため、出力ミラーユニツト部での回転に関
しても、その円偏光(直線偏光から円偏光への変換機
能)には影響がない。Further, in the present invention, since the above-mentioned functions are concentrated near the output mirror 2, all the functions can be unitized. Furthermore, because of the integrated structure, the linear polarization plane and the quarter-wave conversion mirror 10
The positional relationship with and could be set with mechanical accuracy. Due to this integrated structure, the circularly polarized light (the function of converting linearly polarized light into circularly polarized light) is not affected by the rotation at the output mirror unit.
更にこの発明によれば、レーザの共振器の基本の光軸と
円偏光化された後の光軸とを平行にすることができるう
え、更に同軸上に合わせる場合にも、あと2枚の折曲げ
反射ミラー9の使用でよい。この場合には、1/4波長変
換ミラー10を1/8波長変換ミラー2枚としてもよい。Further, according to the present invention, the basic optical axis of the laser resonator can be made parallel to the optical axis after being circularly polarized, and when the coaxial optical axis is further aligned, two more folds are required. It is possible to use the bending reflection mirror 9. In this case, the 1/4 wavelength conversion mirror 10 may be two 1/8 wavelength conversion mirrors.
尚、この発明は、単軸の共振器に適用できるのみなら
ず、多重折返し型の共振器にも適用できるのは勿論であ
る。The present invention can be applied not only to a single-axis resonator but also to a multi-folded resonator.
第1図はこの発明の一実施例に係る炭酸ガスレーザ装置
を示す概略構成図、第2図はP偏光、S偏光における反
射特性を示す特性曲線図、第3図及び第4図は従来の炭
酸ガスレーザ装置の2例を示す概略構成図、第5図は直
線偏光のレーザ光を1/4波長板により円偏光のレーザ光
に変換する方法を示す説明図である。 1……エンドミラー、2……出力ミラー、9……折曲げ
反射ミラー、10……1/4波長変換ミラー。FIG. 1 is a schematic configuration diagram showing a carbon dioxide gas laser device according to an embodiment of the present invention, FIG. 2 is a characteristic curve diagram showing reflection characteristics in P-polarized light and S-polarized light, and FIGS. FIG. 5 is a schematic configuration diagram showing two examples of the gas laser device, and FIG. 5 is an explanatory diagram showing a method of converting linearly polarized laser light into circularly polarized laser light by a 1/4 wavelength plate. 1 …… End mirror, 2 …… Output mirror, 9 …… Bending reflection mirror, 10 …… 1/4 wavelength conversion mirror.
Claims (1)
ドミラーおよび出力ミラーを備え、前記管の内部であっ
て、前記出力ミラー近くに入射角および反射角が30度〜
60度となるように光軸を折り曲げる折曲げ反射ミラーが
配置された一体構成の炭酸ガスレーザ共振器と、この共
振器の出力ミラー近くの光路上に入射角が45度となるよ
うに配置された1/4波長変換ミラーとからなる炭酸ガス
レーザ装置。1. An end mirror and an output mirror are respectively provided at both ends of a tube having an L-shaped tube axis, and inside the tube, near the output mirror, an incident angle and a reflection angle are 30 degrees to 30 degrees.
An integrated carbon dioxide gas laser resonator with a bending reflection mirror that bends the optical axis to 60 degrees, and an incident angle of 45 degrees on the optical path near the output mirror of this resonator. Carbon dioxide laser device consisting of 1/4 wavelength conversion mirror.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59131692A JPH0789591B2 (en) | 1984-06-26 | 1984-06-26 | Carbon dioxide laser device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59131692A JPH0789591B2 (en) | 1984-06-26 | 1984-06-26 | Carbon dioxide laser device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6110291A JPS6110291A (en) | 1986-01-17 |
| JPH0789591B2 true JPH0789591B2 (en) | 1995-09-27 |
Family
ID=15063975
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP59131692A Expired - Lifetime JPH0789591B2 (en) | 1984-06-26 | 1984-06-26 | Carbon dioxide laser device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0789591B2 (en) |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS63292432A (en) * | 1987-05-25 | 1988-11-29 | Sony Corp | Optical pickup device |
| JPH0710542B2 (en) * | 1989-12-22 | 1995-02-08 | 株式会社松田製作所 | Mold moving device in injection molding machine |
| JPH0856028A (en) * | 1994-08-10 | 1996-02-27 | Fanuc Ltd | Laser oscillator |
| US5878067A (en) * | 1994-08-10 | 1999-03-02 | Fanuc Ltd. | Laser oscillator |
Family Cites Families (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5613389A (en) * | 1979-06-29 | 1981-02-09 | Ajinomoto Kk | Valve for powder |
| JPS56133889A (en) * | 1980-03-24 | 1981-10-20 | Hitachi Ltd | Laser generating apparatus |
| JPS59129485A (en) * | 1983-01-13 | 1984-07-25 | Matsushita Electric Ind Co Ltd | Laser oscillation device |
-
1984
- 1984-06-26 JP JP59131692A patent/JPH0789591B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6110291A (en) | 1986-01-17 |
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