JPS59145585A - Laser oscillator - Google Patents
Laser oscillatorInfo
- Publication number
- JPS59145585A JPS59145585A JP2021383A JP2021383A JPS59145585A JP S59145585 A JPS59145585 A JP S59145585A JP 2021383 A JP2021383 A JP 2021383A JP 2021383 A JP2021383 A JP 2021383A JP S59145585 A JPS59145585 A JP S59145585A
- Authority
- JP
- Japan
- Prior art keywords
- output coupling
- coupling mirror
- total reflection
- laser
- resonator
- 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
- H01S3/08063—Graded reflectivity, e.g. variable reflectivity mirror
-
- 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
- H01S2301/00—Functional characteristics
- H01S2301/20—Lasers with a special output beam profile or cross-section, e.g. non-Gaussian
- H01S2301/203—Lasers with a special output beam profile or cross-section, e.g. non-Gaussian with at least one hole in the intensity distribution, e.g. annular or doughnut mode
Abstract
Description
【発明の詳細な説明】 産業上の利用分野 本発明はレーザ発振器に関するものである。[Detailed description of the invention] Industrial applications The present invention relates to a laser oscillator.
従来例の構成とその問題点
第1図は従来の安定型共振器の例を示し、1は全反射鏡
、2は出力結合鏡、3は共振器本体、4は出力光線、4
0は出力光線4の断面、401は出力の強度分布で、基
本モードの例である。この例では出力結合鏡2の中心部
分にエネルギーが集中すること、又外周は保持具で冷却
されるが中心部は冷却されにくいだめ表面膜の破壊や母
材の変形を起し易く出力やモードが不安定になる。Configuration of conventional example and its problems Figure 1 shows an example of a conventional stable resonator, where 1 is a total reflection mirror, 2 is an output coupling mirror, 3 is the resonator body, 4 is an output beam, 4
0 is the cross section of the output light beam 4, and 401 is the output intensity distribution, which is an example of the fundamental mode. In this example, the energy is concentrated at the center of the output coupling mirror 2, and although the outer periphery is cooled by the holder, the center is difficult to cool, which can easily cause the surface film to break or the base material to deform. becomes unstable.
第2図は第1図に示しだ従来の安定型共振器の出力結合
鏡2の拡大断面図である。図において、200は母材、
2o3はパーセント反射膜、204は反射防止膜である
。出力結合鏡のパーセント反射膜203は2%Se 、
!: PbF、、などの異種物質を交互に多層蒸着して
得られるだめ、レーザ光面」力や母材200との密着強
度が弱く、特に中心部はエネルギー密度が高く、冷却効
果も悪いだめこの部分から破袋が始まることが多かった
。FIG. 2 is an enlarged sectional view of the output coupling mirror 2 of the conventional stable resonator shown in FIG. In the figure, 200 is the base material;
2o3 is a percent reflective film, and 204 is an antireflective film. The percent reflection film 203 of the output coupling mirror is 2%Se,
! : It is obtained by alternately depositing multiple layers of different materials such as PbF, etc., the laser beam surface strength and adhesion strength with the base material 200 are weak, the energy density is particularly high in the center, and the cooling effect is also poor. In many cases, the bag started to break from that part.
第3図は従来の不安定型共振器の模式原理図である。1
及び20は全反射鏡、21は透過窓である。41は出力
光線の断面でリング状である。この構成では全反射鏡2
0の光学調整が共振器内で複雑になるため実用上は第4
図に示す様にドーナツ状の全反射鏡201を内蔵させ、
本体と直角方向に断面ドーナツ状の出力光線41を得て
いる。FIG. 3 is a schematic principle diagram of a conventional unstable resonator. 1
20 is a total reflection mirror, and 21 is a transmission window. Reference numeral 41 denotes a ring-shaped cross section of the output light beam. In this configuration, total reflection mirror 2
Since the optical adjustment of 0 becomes complicated within the resonator, it is practically
As shown in the figure, a donut-shaped total reflection mirror 201 is built in,
An output beam 41 having a doughnut-shaped cross section is obtained in a direction perpendicular to the main body.
不安定共振器の特徴は共振器の有効内径を大きく取るこ
とにより、放電励起に大電力が投入でき、大出力レーザ
光線が得られることにあるが、第4図の例の様に全反射
鏡20. ドーナツ鏡(全反射鏡)201.透過窓2
1の3枚の光学部品が出力取出側に必要である。The feature of an unstable resonator is that by increasing the effective inner diameter of the resonator, a large amount of power can be input for discharge excitation and a high output laser beam can be obtained. 20. Donut mirror (total reflection mirror) 201. Transparent window 2
Three optical components (No. 1) are required on the output extraction side.
このように従来方式では出力結合鏡の劣化や使用光学部
品点数が多いなどの欠点があり、出力やモード不安定の
要因となっていた。As described above, the conventional method has drawbacks such as deterioration of the output coupling mirror and the large number of optical components used, which causes output and mode instability.
発明の目的
本発明は上記従来の欠点を解消するもので、光学系が簡
単で、出力結合鏡の劣化、変形がない、耐久性、信頼性
に優れたレーザ発振器を提供することを目日勺とする。OBJECTS OF THE INVENTION The present invention solves the above-mentioned conventional drawbacks, and aims to provide a laser oscillator with a simple optical system, no deterioration or deformation of the output coupling mirror, and excellent durability and reliability. shall be.
発明の構成
本発明は上記目的を達成するもので、レーザ発振器の光
学共振器を構成する出力結合鏡の内側の而の中心部分に
、当該レーザ光線を反射する全反射面を形成し、レーザ
光強度分布の断面がリング状のレーザ光線を取り出すよ
うにしたレーザ発振器を提供するものである。Structure of the Invention The present invention achieves the above object by forming a total reflection surface that reflects the laser beam at the center of the output coupling mirror constituting the optical resonator of the laser oscillator. The present invention provides a laser oscillator that outputs a laser beam whose intensity distribution has a ring-shaped cross section.
実施例の説明
第5図は本発明の光学共振器の一実施例であり、(a)
は安定型共振器、(b)は不安定型共振器を示す。DESCRIPTION OF EMBODIMENTS FIG. 5 shows an embodiment of the optical resonator of the present invention, (a)
shows a stable resonator, and (b) shows an unstable resonator.
第1図と同じ部位には同じ番号を付してその説明を省略
するが、本発明の特徴は出力結合鏡2の内面の中央部に
例えば金蒸着などで得られた全反射面202が形成され
ている点であり、出力光線41の断面は中心部分が抜け
だドーナツ状である。The same parts as in FIG. 1 are given the same numbers and their explanations are omitted, but the feature of the present invention is that a total reflection surface 202 obtained by, for example, gold vapor deposition is formed in the center of the inner surface of the output coupling mirror 2. The cross section of the output light beam 41 is donut-shaped with the center section missing.
第6図は第6図(a)に示しだ安定型共振器の出力結合
鏡2の拡大断面図である。図において200はZxSe
やKclなどの母材、204がPbF、、とThF4な
どの反射防止膜、202は金蒸着等で得られた全反射面
である。FIG. 6 is an enlarged sectional view of the output coupling mirror 2 of the stable resonator shown in FIG. 6(a). In the figure, 200 is ZxSe
204 is PbF, 204 is an antireflection film such as ThF4, and 202 is a total reflection surface obtained by gold vapor deposition.
本実施例の出力結合鏡2は中心部分に金などの物質を一
層蒸着するだけの簡単な構成であり、まだ全反射鏡であ
るからこの中心部はレーザ光線が通過することなく、発
熱や変形、破・廐が大巾に減少できる。The output coupling mirror 2 of this embodiment has a simple structure, with just a layer of material such as gold deposited on the center part, and since it is still a total reflection mirror, the laser beam does not pass through this center part, causing heat generation and deformation. , the damage and damage can be greatly reduced.
発明の効果
以上のように本発明はレーザ発振器の光学共J尿器を構
成する出力結合鏡の共振器の内側の面の中心部分に、全
反射面を設けてリング状のレーザ光線を取り出すよう、
にしたもので、レーザ発振器の信頼性を著しく低下させ
ていた出力結合鏡の内面の劣化や変形を低減することが
でき耐久性、信頼性の向上が図れるとともに、不安定共
振器においては光学系を簡単にできる利点を有する。Effects of the Invention As described above, the present invention provides a total reflection surface at the center of the inner surface of the resonator of the output coupling mirror constituting the optical system of the laser oscillator to extract a ring-shaped laser beam. ,
This makes it possible to reduce the deterioration and deformation of the inner surface of the output coupling mirror, which significantly reduces the reliability of the laser oscillator, thereby improving durability and reliability. It has the advantage of being easy to use.
第1図は従来の安定型共振器の概略構成図、第2図は第
1図に示しだ安定型共振器の出力結合鏡の断面図、第3
図、第4図は従来の不安定型共振器の模式原理図、第6
図は本発明のレーザ発振器の構成図で(a)は安定型共
振器、(b)は不安定型共振器の例を示す、第6図は第
6図(8L)に示した安定型共振器の出力結合鏡の断面
図である。
1・・・・・・全反射鏡、2・・・・・出力結合鏡、3
・・・・・・共振器本体、40,41・・・・・・出力
光線、20・・・・・・全反射鏡、21・・・・・・透
過窓、200・・・・・・母材、201・・・・・・ド
ーナツ型全反射鏡、202・・・・・・全反射面。
代理人の氏名 弁理士 中 尾 敏 男 ほか1名第1
図
第2図
\ 沈
第3図
第4図 201
第5図
20?
第6図
397−Figure 1 is a schematic diagram of a conventional stable resonator; Figure 2 is a sectional view of the output coupling mirror of the stable resonator shown in Figure 1;
Figure 4 is a schematic principle diagram of a conventional unstable resonator, Figure 6
The figures are block diagrams of the laser oscillator of the present invention, in which (a) shows a stable resonator, (b) shows an example of an unstable resonator, and Fig. 6 shows the stable resonator shown in Fig. 6 (8L). FIG. 3 is a cross-sectional view of the output coupling mirror of FIG. 1... Total reflection mirror, 2... Output coupling mirror, 3
...Resonator main body, 40, 41 ... Output beam, 20 ... Total reflection mirror, 21 ... Transmission window, 200 ... Base material, 201...Doughnut-shaped total reflection mirror, 202...Total reflection surface. Name of agent: Patent attorney Toshio Nakao and 1 other person No. 1
Figure 2 \ Shen Figure 3 Figure 4 201 Figure 5 20? Figure 6 397-
Claims (1)
中心部分に、当該レーザ光線を反射する全反射面を形成
し、レーザ光強度分布の断面がリング状のレーザ光線を
取り出すことを特徴とするレーザ発振器。A total reflection surface that reflects the laser beam is formed at the center of the output coupling mirror inside the resonator constituting the optical resonator, and a laser beam with a ring-shaped cross section of the laser beam intensity distribution is extracted. Characteristic laser oscillator.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2021383A JPS59145585A (en) | 1983-02-08 | 1983-02-08 | Laser oscillator |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2021383A JPS59145585A (en) | 1983-02-08 | 1983-02-08 | Laser oscillator |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS59145585A true JPS59145585A (en) | 1984-08-21 |
Family
ID=12020880
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP2021383A Pending JPS59145585A (en) | 1983-02-08 | 1983-02-08 | Laser oscillator |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS59145585A (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS61199686A (en) * | 1985-03-01 | 1986-09-04 | Mitsubishi Electric Corp | Unstable laser resonator |
JPH01207983A (en) * | 1988-02-16 | 1989-08-21 | Mitsubishi Electric Corp | Solid laser equipment |
JPH01270372A (en) * | 1988-04-22 | 1989-10-27 | Mitsubishi Electric Corp | Laser device |
-
1983
- 1983-02-08 JP JP2021383A patent/JPS59145585A/en active Pending
Cited By (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS61199686A (en) * | 1985-03-01 | 1986-09-04 | Mitsubishi Electric Corp | Unstable laser resonator |
JPH0334239B2 (en) * | 1985-03-01 | 1991-05-21 | Mitsubishi Electric Corp | |
JPH01207983A (en) * | 1988-02-16 | 1989-08-21 | Mitsubishi Electric Corp | Solid laser equipment |
JP2673301B2 (en) * | 1988-02-16 | 1997-11-05 | 三菱電機株式会社 | Solid-state laser device |
JPH01270372A (en) * | 1988-04-22 | 1989-10-27 | Mitsubishi Electric Corp | Laser device |
JP2673304B2 (en) * | 1988-04-22 | 1997-11-05 | 三菱電機株式会社 | Laser device |
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