JPS60211990A - Laser oscillator - Google Patents
Laser oscillatorInfo
- Publication number
- JPS60211990A JPS60211990A JP6889084A JP6889084A JPS60211990A JP S60211990 A JPS60211990 A JP S60211990A JP 6889084 A JP6889084 A JP 6889084A JP 6889084 A JP6889084 A JP 6889084A JP S60211990 A JPS60211990 A JP S60211990A
- Authority
- JP
- Japan
- Prior art keywords
- laser light
- laser
- linearly polarized
- light
- metal
- 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
- H01S3/08004—Construction or shape of optical resonators or components thereof incorporating a dispersive element, e.g. a prism for wavelength selection
- H01S3/08009—Construction or shape of optical resonators or components thereof incorporating a dispersive element, e.g. a prism for wavelength selection using a diffraction grating
Landscapes
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Engineering & Computer Science (AREA)
- Plasma & Fusion (AREA)
- Optics & Photonics (AREA)
- Lasers (AREA)
Abstract
Description
【発明の詳細な説明】
〔発明の技術分野〕
この発明は、直線偏光のレーザ発振、および円偏光のレ
ーザ光を得る1こめのレーザ発振器の構成に関するもの
である−
〔従来技術〕
従来この種の発振器として第1図に示すものかあ−・r
ニー図において、(1)は真空容器、(2)はレーザ媒
質、(3)は全反射鏡、(4)は部分透過鏡、(5)は
レーザ光である。全反射鏡(3)と部分透過暁(4)は
レーザ光(5)の光軸上に対向して配置されている。次
に動作について説明す名、容器(1)内のレーザ媒質(
2)を放電やフラ・リシュランブなどで励起すると、全
反射鏡(3)と部分透過鏡(4)との間でレーザ発振が
起り、部分透過鏡(4)からレーザ光(5)を出力する
。[Detailed Description of the Invention] [Technical Field of the Invention] The present invention relates to the configuration of a single laser oscillator that produces linearly polarized laser oscillation and circularly polarized laser light. [Prior Art] Conventionally, this type of laser oscillator Is the oscillator shown in Figure 1 r
In the knee diagram, (1) is a vacuum vessel, (2) is a laser medium, (3) is a total reflection mirror, (4) is a partially transmission mirror, and (5) is a laser beam. The total reflection mirror (3) and the partial transmission mirror (4) are arranged facing each other on the optical axis of the laser beam (5). Next, we will explain the operation of the laser medium (
When 2) is excited by an electric discharge or a full-resistance mirror, laser oscillation occurs between the total reflection mirror (3) and the partially transmitting mirror (4), and a laser beam (5) is output from the partially transmitting mirror (4). .
従来のレーザ発振器は以上のように構成されているので
、レーザ光(5)の偏光方向を決定する1こめの手段が
なく、その偏光方向は不安定であつ1こ。Since the conventional laser oscillator is constructed as described above, there is no one-and-done means for determining the polarization direction of the laser beam (5), and the polarization direction is unstable.
このTこめレーザにより金属、特に鉄系金属を切断する
時は、切断方向により切断性能に差かでTこり、切断面
が斜めになる、ま1こ切断後に材料から切り出され1こ
加工物が自由落下しないなどの欠点があつ1ユ
〔発明の概要〕
この発明は上記のような従来のものの欠点を除去するT
コめになされ1こもので、全反射鏡と部分透過鏡間に金
属の細線から成る金属格子を設けることにより、直線偏
光のレーザ光が得られるレーザ発振器を提供するもので
ある、ま1こ、上記によって得られ1こ直線偏光のレー
ザ光をフェーズリターダで円偏光のレーザ光に変換する
ことで、均一で安定し1こレーザ切断特性を得ることを
目的としている、
〔発明の実施例〕
以下、この第1の発明の一実施例を第2囚および第3図
に−)いて祝明する、図において、(1)〜(4)は上
記従来の発振器と全く同じものである。、<6)は第8
図に示すように、レーザ光を通過させる1こめの穴(9
)を有し1こ基台(8)に金属の細線(7)を接着又は
溶接等により固定し1こ金属格子、(61に月は上記金
属格子(6)によ−て発生し1こ直線偏光のレーザ光で
ある、
レーザ切断では、均一な切断特性を持つ1こ刀ロエ物を
得るγこめには安定し1こ円偏光のレーザ光を出力する
ことが要求される、この1こめにはレーザ発振器は直線
偏光のレーザ光を発生することが望ましく、それにはレ
ーザ発振空胴内に適当な偏光素子を備えることが必要で
ある。以上のことから、レーザ光を反射する金属1例え
ば金の細線から成る金属格子(6) ’!−第2図に示
すまうに、部分透過鏡(4)側に設けることにより、こ
の金属格子(6)は格子と直角方向の偏光を持つレーザ
光が通過するときの減衰が最も少ないという特徴を持っ
ている1こめレーザ発振は、金属格子(6)と直角方向
の偏光を持つことになり、血縁偏光のレーザ光(5a)
を発生することができる、理論的には上記金属格子(6
)に使用される金の細線(7)の直径はレーザ光の波長
に近い程良いが、約0.1u以下でもレーザ発振器内へ
挿入しても損失を増加させることが少ない。ま1こ細線
(7)の間隔もレーザ光の波長に近い程効果が太きい、
シTコがって細線(7)の本数は上記条件を満足する限
りなるべく多く設けるのが理想である、なお、上記実施
例では金属格子(6)を部分透過鏡(4)側へ設け1こ
か、全反射鏡(3)と部分透過鏡(4)の間ならは、い
づれの位置に設けても所期の目的を達成し得ることはい
うまでもない、ま1こ、金属の細線(7)は金としTこ
が、レーザ光を反射する金IM、例えばi、 銅、タン
クステン、モリフテン、又はアルミニウム等であっても
同様の効果は期待できる2ところで、上記実施例では細
線(7)の間隔をレーザ光の波長に近い程良いとしてい
るが、広くしても効果はある、まTこ細線(7)の本数
についても多い方が理想的ではあるか、第3図のように
1〜数本でも直線偏光のレーザ光(5a)を出力するこ
とができる、さらに、金属格子(6)の方向を変えるこ
とをこより、レーザ発振し1こ状態においても任意の方
向の血縁偏光を得ることかできる。When cutting metals, especially ferrous metals, with this T-cut laser, the cutting performance differs depending on the cutting direction, so the cutting surface becomes slanted, and the workpiece is cut out of the material after the first cut. [Summary of the Invention] This invention eliminates the drawbacks of the conventional products as described above.
This invention provides a laser oscillator that can obtain linearly polarized laser light by providing a metal grating made of thin metal wires between a total reflection mirror and a partially transmission mirror. The purpose is to obtain uniform and stable single-polarity laser cutting characteristics by converting the linearly polarized laser beam obtained above into a circularly polarized laser beam using a phase retarder. [Embodiments of the invention] The following , an embodiment of the first invention is illustrated in FIGS. 2 and 3. In the figures, (1) to (4) are exactly the same as the conventional oscillator described above. , <6) is the 8th
As shown in the figure, there is one hole (9 holes) through which the laser beam passes.
), and a thin metal wire (7) is fixed to the base (8) by gluing or welding, and a metal grid is formed. In laser cutting, which uses a linearly polarized laser beam, it is necessary to output a stable single-circularly polarized laser beam in order to obtain a one-stroke loe material with uniform cutting characteristics. It is desirable for the laser oscillator to generate a linearly polarized laser beam, and for this it is necessary to provide an appropriate polarizing element in the laser oscillation cavity.From the above, it is clear that the metal 1 that reflects the laser beam, e.g. A metal grating (6) made of thin gold wires is provided on the side of the partially transmitting mirror (4) as shown in Figure 2, so that this metal grating (6) can absorb laser light with polarization perpendicular to the grating. The first laser oscillation, which has the characteristic of having the least attenuation when it passes through, has polarization perpendicular to the metal grating (6), and the related polarized laser light (5a)
The above metal lattice (6
) The diameter of the thin gold wire (7) used in the wire (7) should be closer to the wavelength of the laser beam, but if it is less than about 0.1 μ, it will not increase the loss even if it is inserted into the laser oscillator. The closer the distance between the thin lines (7) to the wavelength of the laser light, the thicker the effect.
Therefore, it is ideal to provide as many thin wires (7) as possible as long as the above conditions are satisfied.In addition, in the above embodiment, the metal grid (6) is provided on the partially transmitting mirror (4) side. It goes without saying that between the total reflection mirror (3) and the partial transmission mirror (4), the desired purpose can be achieved no matter where it is placed. (7) is made of gold, and the same effect can be expected even if the material is gold IM that reflects laser light, such as copper, tanksten, molyftene, or aluminum. It is said that the closer the spacing of 7) is to the wavelength of the laser beam, the better, but it is effective even if it is widened.Wouldn't it be ideal to have as many thin lines (7) as shown in Figure 3? It is possible to output even one to several linearly polarized laser beams (5a), and by changing the direction of the metal grating (6), laser oscillation can produce blood-related polarized light in any direction even in this state. Can you get it?
次に、第2の発明の一実施例を第4図、第5図について
祝明する。図において、(1)〜(4)、(5B)。Next, an embodiment of the second invention will be explained with reference to FIGS. 4 and 5. In the figure, (1) to (4), (5B).
(6)〜(9)は上記第1の発明の装置と全く同じもの
である、Tこだし、金属格子(6)はレーせ光の伝搬路
に配設され1こフェーズリターダ(1(Iの傾きに対し
て、第5図に示すように格子の角度が45°となるよう
に設けられている。なお、この第2の発明は、レーザ光
の伝搬路にフェーズリターダαOを配設し、金属格子(
6)を45°となるように設け1こことを除けば上記第
1の発明と全く同様である。(6) to (9) are exactly the same as the device of the first invention. The T-column and metal grating (6) are disposed in the propagation path of the laser light, and the one-phase retarder (1(I) The grating is provided so that the angle of the grating is 45° with respect to the inclination of the laser beam, as shown in FIG. , metal grid (
6) is provided at an angle of 45°, and except for 1, it is completely the same as the first invention.
上述しγこように、全反射鏡(3)と部分透過鏡(4)
間Ef&けられ1こ金属格子(6)により、レーザ発振
され1こレーザ光は直線偏光のレーザ光(5a)となっ
て部分透過鏡(4)から出力される、この直線偏光のレ
ーザ光(5a)は、レーザ光の伝搬路に配設され1こフ
ェーズリターダαOの傾きに対して、第5図に示すよう
に金属格子(6)の角度を45°にすることで、上記フ
ェーズリターダ叫に反射されて円偏光のレーザ光α刀と
なる、この場合金属格子(6)の角度は45゜に近い程
、最適な円偏光に近いレーザ光か得られることはいうま
でもない。As mentioned above, the total reflection mirror (3) and the partial transmission mirror (4)
The laser beam is oscillated by the metal grating (6) between Ef and keratin, and becomes a linearly polarized laser beam (5a), which is output from the partially transmitting mirror (4). 5a) is arranged in the propagation path of the laser beam, and by setting the angle of the metal grating (6) to 45° with respect to the inclination of the phase retarder αO as shown in FIG. It goes without saying that the closer the angle of the metal grating (6) is to 45°, the closer to optimal circularly polarized laser light can be obtained.
以上のように、この発明にまれはレーザ発振空胴内に直
線偏光を発生させる1こめの素子、つまり全反射鏡と部
分透過鏡間のいづれかの位置に金属の細線で構成され1
こ金属格子を設け1こことにより、安定し1コ直線偏光
のレーザ光が得られる効果がある、まTこ、レーザ光の
伝搬路にフェーズリターダを配設し、このフェーズリタ
ーダの傾きに対して上記金属格子の角度を45°にし1
こことでフェーズリターダに反射さt′1Tこレーザ光
は円偏光のレーザ光に変換される。この円偏光のレーザ
光での切断においては、特に鉄系の金属の場合、切れ味
に差が生じることなく、均一で安定し1こ切断特性が得
られるすぐれ1こ効果がある。As mentioned above, the present invention rarely requires a single element that generates linearly polarized light within the laser oscillation cavity, that is, a thin metal wire located somewhere between the total reflection mirror and the partial transmission mirror.
By providing this metal grating, it is possible to obtain a stable and linearly polarized laser beam.In addition, a phase retarder is placed in the propagation path of the laser beam, and the inclination of this phase retarder is and set the angle of the above metal grid to 45°1
At this point, the laser beam reflected by the phase retarder t'1T is converted into a circularly polarized laser beam. In cutting with this circularly polarized laser beam, especially in the case of iron-based metals, there is no difference in sharpness, and there is an excellent effect in that uniform and stable cutting characteristics can be obtained.
第1図は従来のレーザ発振器を示す概略構成図、82図
はこの第1の発明の一実施例を示す構成図、第8図は同
金属格子の正面図、第4図はこの第2の発明の一実施例
を示す構成図、第5図は同金属格子の正面図である、
図において、(3)は全反射鏡、(4)は部分透過鏡、
(5a)は面線偏光のレーザ光、(6)は金属格子、(
7)は金属細線、αOはフェーズリターダ、(ロ)は円
偏光のレーザ光である。
なお、図中同一符号は同一、又は相当部分を示す。
代理人 大岩増雄
第1図
第2図
第3図
乙
第4図
第5図FIG. 1 is a schematic configuration diagram showing a conventional laser oscillator, FIG. 82 is a configuration diagram showing an embodiment of this first invention, FIG. 8 is a front view of the same metal grid, and FIG. A configuration diagram showing an embodiment of the invention, and FIG. 5 is a front view of the same metal grating. In the figure, (3) is a total reflection mirror, (4) is a partial transmission mirror,
(5a) is a plane-polarized laser beam, (6) is a metal grating, (
7) is a thin metal wire, αO is a phase retarder, and (b) is a circularly polarized laser beam. Note that the same reference numerals in the figures indicate the same or equivalent parts. Agent Masuo Oiwa Figure 1 Figure 2 Figure 3 Figure Otsu Figure 4 Figure 5
Claims (4)
射鏡と部分透過鏡とを有するレーザ発振器において、上
記全反射鏡と部分透過鏡の間に金属の細線から成る金属
格子を設け1こことを特徴とするレーザ発振器、(1) In a laser oscillator having a total reflection mirror and a partial transmission mirror, which are provided oppositely on the optical axis of the laser beam, a metal grating made of thin metal wires is installed between the total reflection mirror and the partial transmission mirror. A laser oscillator characterized by:
徴とする特許請求の範囲第1JJI記載のレーザ発振器
、(2) A laser oscillator according to claim 1 JJI, characterized in that the thin metal wire has a diameter of about 0.1 mm or less;
射鏡と部分透過鏡とを有するレーザ発振器において、上
記全反射鏡と部分透過鏡の間に直線偏光のレーぜ光を発
生させる1こめに金属の細線から成る金属格子を設け、
この発生し1コ直線偏光のレーザ光を円偏光のレーザ光
に変換するTこめのフェースリタータを上記レーザ光の
伝搬路に配設しTこことを特徴とするレーザ発振器。(3) In a laser oscillator that has a total reflection mirror and a partial transmission mirror that are arranged opposite to each other on the optical axis of the laser beam, a linearly polarized laser beam is generated between the total reflection mirror and the partial transmission mirror. A metal grid made of thin metal wires is installed in each corner,
A laser oscillator characterized in that a T-face retarder for converting the generated linearly polarized laser light into circularly polarized laser light is disposed in the propagation path of the laser light.
徴とする特許請求の範囲第8項記載のレーザ発振器、(4) A laser oscillator according to claim 8, wherein the thin metal wire has a diameter of about 0.1 mm or less;
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP6889084A JPS60211990A (en) | 1984-04-06 | 1984-04-06 | Laser oscillator |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP6889084A JPS60211990A (en) | 1984-04-06 | 1984-04-06 | Laser oscillator |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS60211990A true JPS60211990A (en) | 1985-10-24 |
Family
ID=13386697
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP6889084A Pending JPS60211990A (en) | 1984-04-06 | 1984-04-06 | Laser oscillator |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS60211990A (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4757514A (en) * | 1985-08-13 | 1988-07-12 | Laser Corporation Of America | Wire array light polarizer for gas laser |
| US4977574A (en) * | 1988-01-08 | 1990-12-11 | Fanuc Ltd. | Laser oscillator |
-
1984
- 1984-04-06 JP JP6889084A patent/JPS60211990A/en active Pending
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4757514A (en) * | 1985-08-13 | 1988-07-12 | Laser Corporation Of America | Wire array light polarizer for gas laser |
| US4977574A (en) * | 1988-01-08 | 1990-12-11 | Fanuc Ltd. | Laser oscillator |
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