JPS59101885A - Laser device - Google Patents
Laser deviceInfo
- Publication number
- JPS59101885A JPS59101885A JP21171982A JP21171982A JPS59101885A JP S59101885 A JPS59101885 A JP S59101885A JP 21171982 A JP21171982 A JP 21171982A JP 21171982 A JP21171982 A JP 21171982A JP S59101885 A JPS59101885 A JP S59101885A
- Authority
- JP
- Japan
- Prior art keywords
- laser
- case
- mirror
- laser device
- blower
- 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
- H01S3/02—Constructional details
Abstract
Description
【発明の詳細な説明】
産業上の利用分野
本発明は、基準ベンチを有するレーザ装置に関するもの
でちる。DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a laser device having a reference bench.
従来例の構成とその問題点
レーザ装置として安定している為には、光軸に対してミ
ラー角度(全反射鏡、半透過鏡の角度)を一定に保つ必
要があり、また光軸の基準を決定するベースが安定して
いることは当然のこととなる。従来、安定したベースを
得る為に、光軸に対し非対称(光軸とベース中心が異る
)となる欠点を有するも、ベースの中心に光軸がある対
称形のパイプベース(第1図)と同じ強度を小形にて得
ることの出来る、第2図に示すような基準ベンチ形のレ
ーザ装置が用いられることが多い。なお第1図及び第2
図において、囚はパイプ、(B)は支持板、(C)はレ
ーザ管、の)はミラー、(E)は基準ベンチである。Conventional configuration and its problems In order to be stable as a laser device, it is necessary to keep the mirror angle (angle of total reflection mirror, semi-transmission mirror) constant with respect to the optical axis. It is a matter of course that the base for determining is stable. Conventionally, in order to obtain a stable base, a symmetrical pipe base with the optical axis at the center of the base (Figure 1) has the disadvantage of being asymmetrical with respect to the optical axis (the optical axis and the center of the base are different). A reference bench-type laser device as shown in FIG. 2 is often used, which can obtain the same intensity as in a small size. In addition, Figures 1 and 2
In the figure, (B) is a pipe, (B) is a support plate, (C) is a laser tube, (A) is a mirror, and (E) is a reference bench.
しかしながらこのような従来の基準ベンチ形のレーザ装
置は、レーザ発振による発熱及び外部雰囲気温度の変化
により、各構成部品が伸縮を行なった時に、光軸に対し
ミラー角度を変化させてしまい、しいてはレーデ出力を
変化させてし捷い、レーデ装置としての安定性に欠ける
という欠点があった。すなわち従来の基準ベンチ形の7
−ザ装置は、%3図のように、基準ベンチ(1)上に支
持板(4)によシレーザ管(3)と全反射鏡(2a)及
び半透過鏡(2b)とが取付けられ、これがケース(5
)内に設置されている。レーザ発振が安定した状態にお
いて外部雰囲気温度を上昇させた場合を例に説明を行う
と、外部雰囲気温度が上昇するとケース(5)を通じて
、内部温度が上昇する。その際長手方向にすべての構成
部品が平行に伸縮すれば出力変動は問題のない範囲であ
るが、現実には各部で温度勾配が生じ、光軸(6ンと異
った方向に変化し、ミラー角度を光軸(6)に対し変え
てしまうこととなる。この時の出力変動は第5図に実線
(イ)で示すようになる。However, in such a conventional reference bench type laser device, when each component expands and contracts due to heat generation due to laser oscillation and changes in external ambient temperature, the mirror angle with respect to the optical axis changes. The disadvantage was that it was unstable as a radar device because it had to change the radar output. In other words, the conventional standard bench type 7
- As shown in Figure 3, the laser device includes a laser tube (3), a total reflection mirror (2a), and a semi-transmission mirror (2b) attached to a support plate (4) on a reference bench (1), This is the case (5
) is installed within. Taking as an example a case where the external atmosphere temperature is increased in a state where laser oscillation is stable, when the external atmosphere temperature increases, the internal temperature increases through the case (5). At that time, if all the components expand and contract in parallel in the longitudinal direction, the output fluctuation will be within a range where there is no problem, but in reality, temperature gradients occur in each part, and the optical axis (6 degrees) changes in different directions. The mirror angle will be changed with respect to the optical axis (6).The output fluctuation at this time will be as shown by the solid line (A) in FIG.
発明の目的
本発明は上記従来の欠点を解消するもので、出力の安定
したレーデ装置を得ること全目的とする。OBJECTS OF THE INVENTION The present invention is intended to eliminate the above-mentioned drawbacks of the prior art, and its entire purpose is to obtain a radar device with stable output.
発明の構成
上記目的を達するため、本発明のレーザ装置は、ケース
の内部に、レーザ装置の光軸を決めるための基準ベンチ
と、この基準ベンチ上に配置されたレーザ管と全反射鏡
と半透過鏡とからなるレーザ共振器と、このレーザ共振
器の各部分の温度を均一化する送風機とを設けた構成で
ある。Structure of the Invention In order to achieve the above object, the laser device of the present invention includes, inside a case, a reference bench for determining the optical axis of the laser device, a laser tube, a total reflection mirror, and a half-reflector disposed on the reference bench. This configuration includes a laser resonator made up of a transmitting mirror and a blower that equalizes the temperature of each part of the laser resonator.
実施例の説明
以下、本発明の一実施例について、図面に基づいて説明
する。第4図は本発明の一実施例におけるレーザ装置の
概略構成図光あり、第3図に示す構成要素と同一の構成
要素には同一の符号を付してその説明を省略する。第4
図において、(7)は送風機であり、この送風機(7)
により、ケース(5)の内部温度を均一化し、各部の温
度勾配を少なくする働きを生じさせているため、ミラー
角度変化は微少となり、第5図に実線(ロ)で示すよう
に出方変動は極めて小さくなる。DESCRIPTION OF EMBODIMENTS An embodiment of the present invention will be described below with reference to the drawings. FIG. 4 is a schematic configuration diagram of a laser device according to an embodiment of the present invention, and the same components as those shown in FIG. 3 are given the same reference numerals and their explanations are omitted. Fourth
In the figure, (7) is a blower;
As a result, the internal temperature of the case (5) is made uniform and the temperature gradient in each part is reduced, so the change in the mirror angle is slight, and the change in the angle of the mirror is small, as shown by the solid line (b) in Figure 5. becomes extremely small.
発明の効果
以上、説明したように本発明によれば、レーデ出力を安
定にすることが可能となシ、レーデ装置として安定なも
のを得ることができ、その工業的利用価値は極めて大で
ある。Effects of the Invention As explained above, according to the present invention, it is possible to stabilize the radar output, and a stable radar device can be obtained, and its industrial utility value is extremely large. .
第1図(イ)は従来の対称形のレーデ装置の概略縦断側
面図、同図(ロ)は同レーデ装置の概略縦断正面図、第
2図(インは従来の基準ベンチ形のレーデ装置の概略縦
断側面図、同図(ロ)は同レーデ装置の概略縦断正面図
、第3図は従来の基準ベンチ形のレーザ装置の概略全体
構成図、第4図は本発明の一実施例におけるレーデ装置
の概略全体構成図、第5図は第3図及び第4図に示すレ
ーザ装置の出力特性の説明図である。
(1)・・・基準ベンチ、(2a)・・・全反射鏡、(
2b)・・・半透過鏡、(3)・・・レーザ管、(4)
・・−支持板、(5)・・・ケース、(7)・・・送風
機
代理人 森 木 義 弘
第1図
(わ (口2第3図
第4図
第5図
口
温度変札Figure 1 (a) is a schematic longitudinal side view of a conventional symmetrical radar device, Figure 1 (b) is a schematic longitudinal sectional front view of the same radar device, and Figure 2 (in) is a schematic longitudinal sectional side view of a conventional symmetrical radar device. FIG. 3 is a schematic overall configuration diagram of a conventional reference bench-type laser device, and FIG. 4 is a schematic longitudinal sectional side view of the radar device, FIG. A schematic overall configuration diagram of the device, and FIG. 5 is an explanatory diagram of the output characteristics of the laser device shown in FIGS. 3 and 4. (1)... Reference bench, (2a)... Total reflection mirror, (
2b)...Semi-transparent mirror, (3)...Laser tube, (4)
...-Support plate, (5)...Case, (7)...Blower agent Yoshihiro Moriki Figure 1 (Wa) Figure 2 Figure 3 Figure 4 Figure 5 Temperature change plate
Claims (1)
基準ベンチと、この基準ベンチ上に配置されたレーザ管
と全反射鏡と半透過鏡とからなるレーザ共振器と、この
レーデ共振器の各部の温度を均一化する送風機とを設け
たレーデ装置。1. A reference bench for determining the optical axis of the laser device inside the case, a laser resonator consisting of a laser tube, a total reflection mirror, and a semi-transmission mirror placed on this reference bench, and a laser resonator for this laser resonator. A radar device equipped with a blower that equalizes the temperature of each part.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP21171982A JPS59101885A (en) | 1982-12-01 | 1982-12-01 | Laser device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP21171982A JPS59101885A (en) | 1982-12-01 | 1982-12-01 | Laser device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS59101885A true JPS59101885A (en) | 1984-06-12 |
Family
ID=16610462
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP21171982A Pending JPS59101885A (en) | 1982-12-01 | 1982-12-01 | Laser device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS59101885A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5181215A (en) * | 1991-11-22 | 1993-01-19 | Sam Richard C | Heated solid state laser |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5243980U (en) * | 1975-09-18 | 1977-03-29 |
-
1982
- 1982-12-01 JP JP21171982A patent/JPS59101885A/en active Pending
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5243980U (en) * | 1975-09-18 | 1977-03-29 |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5181215A (en) * | 1991-11-22 | 1993-01-19 | Sam Richard C | Heated solid state laser |
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