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JP2930482B2 - Conical Raman laser device - Google Patents
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JP2930482B2 - Conical Raman laser device - Google Patents

Conical Raman laser device

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Publication number
JP2930482B2
JP2930482B2 JP23917292A JP23917292A JP2930482B2 JP 2930482 B2 JP2930482 B2 JP 2930482B2 JP 23917292 A JP23917292 A JP 23917292A JP 23917292 A JP23917292 A JP 23917292A JP 2930482 B2 JP2930482 B2 JP 2930482B2
Authority
JP
Japan
Prior art keywords
laser
main body
raman
shape
conical
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
Application number
JP23917292A
Other languages
Japanese (ja)
Other versions
JPH0690066A (en
Inventor
敬二 吉村
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Mitsubishi Heavy Industries Ltd
Original Assignee
Mitsubishi Heavy Industries Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Mitsubishi Heavy Industries Ltd filed Critical Mitsubishi Heavy Industries Ltd
Priority to JP23917292A priority Critical patent/JP2930482B2/en
Publication of JPH0690066A publication Critical patent/JPH0690066A/en
Application granted granted Critical
Publication of JP2930482B2 publication Critical patent/JP2930482B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【産業上の利用分野】本発明は、ラマンレーザ装置に関
し、特にラマン変換効率を向上させるように改良したも
のである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a Raman laser device and, more particularly, to a Raman laser device improved so as to improve Raman conversion efficiency.

【0002】[0002]

【従来の技術】ラマンレーザは、レーザ光を一対の鏡の
間で多重反射して、ガス分子の回転散乱遷移でレーザ光
を長波長側へ波長変換するものであり(石川島播磨技報
第24巻5号,昭和59年9月)、そのような従来のラ
マンレーザ装置の一例を図3に示す。
2. Description of the Related Art A Raman laser reflects a laser beam multiple times between a pair of mirrors, and converts the wavelength of the laser beam to a longer wavelength side by rotational scattering transition of gas molecules (Ishikawajima Harima Technical Report Vol. 24) No. 5, September 1984), an example of such a conventional Raman laser device is shown in FIG.

【0003】同図に示すように、レーザ媒質ガスを保有
する円筒3の両端フランジ3A,3Bに端板22,23
が取り付けられると共にそれぞれの端板22,23の内
側に短筒20,21が固定され、更に、短筒20,21
には凹面鏡1,2が挿入されている。端板22、凹面鏡
2には、外部からレーザ光を入射させるために窓4、入
射用孔2Aがそれぞれ設けられ、また、端板23、凹面
鏡1には、レーザ光を出射させる為に出射用孔1A、窓
5がそれぞれ設けられている。
As shown in FIG. 1, end plates 22, 23 are provided on both end flanges 3A, 3B of a cylinder 3 holding a laser medium gas.
Are attached and the short cylinders 20 and 21 are fixed inside the respective end plates 22 and 23.
Have concave mirrors 1 and 2 inserted therein. The end plate 22 and the concave mirror 2 are provided with a window 4 and an incident hole 2A, respectively, for allowing a laser beam to enter from the outside. The end plate 23 and the concave mirror 1 have an emission port for emitting a laser beam. A hole 1A and a window 5 are provided.

【0004】従って、図4に示すように、レーザ光30
が、端板22の窓4、凹面鏡2の入射用孔2Aを通っ
て、凹面鏡1,2の間に入り、これら凹面鏡1,2の間
の多重反射部分24で多重反射する。そして、多重反射
によりラマンレーザとなったレーザ光31は、凹面鏡1
の出射用孔1A、端板23の窓5を通って、外部へ出射
することとなる。
Accordingly, as shown in FIG.
Passes through the window 4 of the end plate 22 and the entrance hole 2A of the concave mirror 2 and enters between the concave mirrors 1 and 2, and is multiple reflected by the multiple reflection portion 24 between the concave mirrors 1 and 2. Then, the laser beam 31 that has become a Raman laser due to the multiple reflection is reflected by the concave mirror 1.
Through the exit hole 1A and the window 5 of the end plate 23.

【0005】[0005]

【発明が解決しようとする課題】上述した従来のラマン
レーザ装置では、レーザ光30が凹面鏡1,2の間で多
重反射すると、特に、円筒3の中央部に集中するため、
レーザ光のエネルギにより、レーザ媒質ガスの温度が上
昇し、ラマン変換効率が低下する虞がある。そこで、ラ
マン変換効率を改善し、ラマンレーザ出力を高めるため
には、レーザ媒質ガスの冷却を如何に行うかが課題とな
る。
In the above-mentioned conventional Raman laser device, when the laser beam 30 is multiply reflected between the concave mirrors 1 and 2, it concentrates particularly on the central portion of the cylinder 3.
Due to the energy of the laser light, the temperature of the laser medium gas may increase, and the Raman conversion efficiency may decrease. Therefore, in order to improve the Raman conversion efficiency and increase the output of the Raman laser, it is an issue how to cool the laser medium gas.

【0006】特に、入射レーザ出力が増大し、又は、パ
ルス状の入射レーザ光の単位時間当りのパルス数が大き
くなればなるほど、一層大きな課題となる。本発明は、
上記従来技術に鑑みて成されたものであり、レーザ媒質
ガスの温度を低く保ち、ラマン変換効率を向上させるこ
とのできるラマンレーザ装置を提供することを目的とす
る。
In particular, the greater the incident laser output or the greater the number of pulses per unit time of the pulsed incident laser light, the greater the problem. The present invention
An object of the present invention is to provide a Raman laser device capable of keeping the temperature of a laser medium gas low and improving Raman conversion efficiency.

【0007】[0007]

【課題を解決するための手段】斯かる目的を達成する本
発明の構成はレーザ媒質ガスを保有しておく本体容器を
レーザ光の多重反射の形状に合わせて、中央を小径、両
端を大径としたつづみ形としたことを特徴とする。
According to the structure of the present invention for achieving the above object, a main container for holding a laser medium gas is adjusted to the shape of multiple reflection of a laser beam so that the center has a small diameter and both ends have a large diameter. It is characterized in that it has a continuous shape.

【0008】[0008]

【作用】本発明では本体容器がレーザ光の多重反射の形
状に合わせて、中央を小径、両端を大径としたつづみ形
となっている為、レーザ光多重反射部の最外殻部と本体
との距離を、特に中央部で著しく小さくすることができ
る。この為、レーザ媒質ガスの熱が本体容器へ効率良く
伝達することとなる。従って、本体外部からレーザ媒質
ガスを効率的に冷却することができ、レーザ媒質ガスの
温度を低く保つことができる。
According to the present invention, since the main body container has a conical shape with a small diameter at the center and a large diameter at both ends in accordance with the shape of the multiple reflection of the laser beam, the outermost shell of the multiple reflection portion of the laser beam is formed. The distance from the body can be significantly reduced, especially at the center. Therefore, the heat of the laser medium gas is efficiently transmitted to the main body container. Therefore, the laser medium gas can be efficiently cooled from outside the main body, and the temperature of the laser medium gas can be kept low.

【0009】[0009]

【実施例】以下、本発明について、図面に示す実施例を
参照して詳細に説明する。図1に本発明の一実施例を示
す。同図に示すように、レーザ媒質ガスを保有する本体
容器35の両端フランジ3A,3Bに端板22,23が
取り付けられると共にそれぞれ端板22,23の内側に
短筒20,21が固定され、更に、短筒20,21には
凹面鏡1,2が挿入されている。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS Hereinafter, the present invention will be described in detail with reference to embodiments shown in the drawings. FIG. 1 shows an embodiment of the present invention. As shown in the figure, end plates 22 and 23 are attached to both end flanges 3A and 3B of a main body container 35 holding a laser medium gas, and short cylinders 20 and 21 are fixed inside the end plates 22 and 23, respectively. Further, concave mirrors 1 and 2 are inserted into the short cylinders 20 and 21, respectively.

【0010】端板22、凹面鏡2には、外部からレーザ
光を入射させるために窓4、入射用孔2Aがそれぞれ設
けられ、また、端板23、凹面鏡1には、レーザ光を出
射させる為に出射用孔1A、窓5がそれぞれ設けられて
いる。ここで、本体容器35の形状は、レーザ光多重反
射の形状に合わせて、中央が小径で、両端を大径とした
つづみ形となっている。言い換えると、本体容器35の
形状は、頂点を向かい合わせて二つの円錐形を結合した
ものに似た形状となっている。
The end plate 22 and the concave mirror 2 are provided with a window 4 and an incident hole 2A, respectively, for allowing a laser beam to enter from the outside, and the end plate 23 and the concave mirror 1 are provided for emitting the laser beam. Are provided with an emission hole 1A and a window 5, respectively. Here, the shape of the main body container 35 is a continuous shape having a small diameter at the center and large diameters at both ends in accordance with the shape of the laser beam multiple reflection. In other words, the shape of the main body container 35 is similar to a shape obtained by connecting two cones with the vertexes facing each other.

【0011】このように、本実施例では、本体容器35
の形状が中央部ほど小径となっているので、レーザ光多
重反射部24との間隔が狭くなり、本体容器35内のレ
ーザ媒質の熱が本体容器35に効率的に伝達されること
になる。この為、本体容器35の外部からレーザ媒質を
冷却すれば、レーザ媒質の温度上昇を抑えて、ラマン変
換の効率を維持することが可能となる。但し、冷却は、
自然冷却によっても良いが、本体容器35の外部に機械
的冷却、電子的冷却等による冷却装置を設けることも考
えられる。
As described above, in the present embodiment, the main container 35 is used.
Is smaller in the center, so that the distance from the laser light multiple reflection portion 24 is reduced, and the heat of the laser medium in the main body container 35 is efficiently transmitted to the main body container 35. For this reason, if the laser medium is cooled from the outside of the main body container 35, it is possible to suppress the temperature rise of the laser medium and maintain the efficiency of the Raman conversion. However, cooling is
Natural cooling may be used, but it is also conceivable to provide a cooling device outside the main body container 35 by mechanical cooling, electronic cooling, or the like.

【0012】ここで、冷却効率の向上という観点から
は、レーザ光多重反射部24と本体容器25との間隔が
できるだけ狭く、且つ、一定していることが望ましいと
考えられる。また、本体容器35の材質について、冷却
効率を考慮して決定することも考えられる。更に、レー
ザ光多重反射部24の形状は、凹面鏡1,2の曲率半径
に専ら依存するので、本体容器35の形状は、凹面鏡
1,2の形状に応じて適宜設計変更することが可能であ
る。
Here, from the viewpoint of improving the cooling efficiency, it is considered desirable that the distance between the laser beam multiple reflection section 24 and the main body container 25 be as narrow and constant as possible. Further, the material of the main body container 35 may be determined in consideration of the cooling efficiency. Furthermore, since the shape of the laser beam multiple reflection portion 24 depends exclusively on the radius of curvature of the concave mirrors 1 and 2, the shape of the main body container 35 can be appropriately changed in design according to the shape of the concave mirrors 1 and 2. .

【0013】次に、本発明の他の実施例を図2に示す。
本実施例は、図2に示すように、製造上の制約を緩和す
るため、本体容器36の中央部を円筒部3Xとしたもの
である。本実施例は、本体容器36の中央部を円筒部2
Xとしているが、レーザ光多重反射部との間隔を充分に
狭くすれば、上述した実施例と同様な作用、効果を奏す
る。尚、その他の構成は、前述した実施例と同様であ
り、同様の効果を奏する。
Next, another embodiment of the present invention is shown in FIG.
In this embodiment, as shown in FIG. 2, the central portion of the main body container 36 is formed as a cylindrical portion 3X in order to ease the restrictions on manufacturing. In this embodiment, the central portion of the main body
Although it is set to X, the same operation and effect as those of the above-described embodiment can be obtained if the distance between the laser light and the multiple reflection unit is sufficiently reduced. The other configurations are the same as those of the above-described embodiment, and have the same effects.

【0014】[0014]

【発明の効果】以上、実施例に基づいて具体的に説明し
たように、本発明は、レーザ光多重反射の形状に合わせ
て、本体容器の形状を中央が小径で両端を大径としたの
で、レーザ媒質ガスの温度を低く維持できる。この為、
入射レーザのエネルギが高くなった場合或いはパルス状
の入射レーザ光の単位時間のパルス数が増加した場合で
も、効率良くラマンレーザに変換できるものである。
As described above in detail with reference to the embodiments, according to the present invention, the shape of the main body container is made smaller at the center and larger at both ends in accordance with the shape of the laser beam multiple reflection. In addition, the temperature of the laser medium gas can be kept low. Because of this,
Even when the energy of the incident laser is increased or the number of pulses of the pulsed incident laser light per unit time is increased, the laser can be efficiently converted into a Raman laser.

【図面の簡単な説明】[Brief description of the drawings]

【図1】本発明の一実施例に係る円錐形ラマンレーザ装
置の断面図である。
FIG. 1 is a sectional view of a conical Raman laser device according to one embodiment of the present invention.

【図2】本発明の他の実施例に係る円錐形ラマンレーザ
装置の要部断面図である。
FIG. 2 is a sectional view of a main part of a conical Raman laser device according to another embodiment of the present invention.

【図3】従来のラマンレーザ装置の断面図である。FIG. 3 is a cross-sectional view of a conventional Raman laser device.

【図4】レーザ光の多重反射の説明図である。FIG. 4 is an explanatory diagram of multiple reflection of laser light.

【符号の説明】[Explanation of symbols]

1,2 凹面鏡 1A 入射用孔 2A 出射用孔 3 円筒 3A,3B 両端フランジ部 4,5 窓 20,21 短筒 22,23 端板 24 多重反射部分 30 レーザ光 31 ラマンレーザ光 35,36 本体容器 3X 円筒部 1, 2 concave mirror 1A entrance hole 2A exit hole 3 cylinder 3A, 3B both ends flange 4,5 window 20,21 short cylinder 22,23 end plate 24 multiple reflection part 30 laser light 31 Raman laser light 35,36 main body container 3X Cylindrical part

フロントページの続き (58)調査した分野(Int.Cl.6,DB名) H01S 3/30 Continuation of the front page (58) Field surveyed (Int.Cl. 6 , DB name) H01S 3/30

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 レーザ媒質ガスを保有しておく本体容器
をレーザ光の多重反射の形状に合わせて、中央を小径、
両端を大径としたつづみ形としたことを特徴とする円錐
形ラマンレーザ装置。
A main container for holding a laser medium gas has a small diameter at the center according to the shape of multiple reflection of laser light.
A conical Raman laser device having a conical shape with both ends having large diameters.
JP23917292A 1992-09-08 1992-09-08 Conical Raman laser device Expired - Lifetime JP2930482B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP23917292A JP2930482B2 (en) 1992-09-08 1992-09-08 Conical Raman laser device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP23917292A JP2930482B2 (en) 1992-09-08 1992-09-08 Conical Raman laser device

Publications (2)

Publication Number Publication Date
JPH0690066A JPH0690066A (en) 1994-03-29
JP2930482B2 true JP2930482B2 (en) 1999-08-03

Family

ID=17040799

Family Applications (1)

Application Number Title Priority Date Filing Date
JP23917292A Expired - Lifetime JP2930482B2 (en) 1992-09-08 1992-09-08 Conical Raman laser device

Country Status (1)

Country Link
JP (1) JP2930482B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP1059708B1 (en) 1998-11-10 2006-01-25 Kabushiki Kaisha IDX Technologies Apparatus for photoreaction

Also Published As

Publication number Publication date
JPH0690066A (en) 1994-03-29

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