JPH05160477A - Solid-state laser device - Google Patents

Solid-state laser device

Info

Publication number
JPH05160477A
JPH05160477A JP31813491A JP31813491A JPH05160477A JP H05160477 A JPH05160477 A JP H05160477A JP 31813491 A JP31813491 A JP 31813491A JP 31813491 A JP31813491 A JP 31813491A JP H05160477 A JPH05160477 A JP H05160477A
Authority
JP
Japan
Prior art keywords
solid
central axis
state laser
laser
rod
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
Application number
JP31813491A
Other languages
Japanese (ja)
Inventor
Hirotaka Koyama
博隆 小山
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.)
Toshiba Corp
Original Assignee
Toshiba Corp
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 Toshiba Corp filed Critical Toshiba Corp
Priority to JP31813491A priority Critical patent/JPH05160477A/en
Publication of JPH05160477A publication Critical patent/JPH05160477A/en
Pending legal-status Critical Current

Links

Landscapes

  • Lasers (AREA)

Abstract

PURPOSE:To provide a solid-state laser device to obtain a laser oscillator in which the intensity distribution and flaring angle of laser output light are uniform in radial directions. CONSTITUTION:A solid-state laser device is provided with a pumping light condensing mechanism 13, in which a laser rod 5 and a rod-shaped pumping lamp 6 are arranged in a cylindrical, elliptical reflection mirror 4 fitted into a rectangular paralleled member 8, and a holding mechanism 7 to hold the pumping light condensing mechanism, and further the rectangular paralleled member is constituted in such a way that the plane sectional shape perpendicular to its central axis may be a regular polyhedron or circle having a center on the central axis and the central axis coincide with the central axis of the laser rod.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】この発明は、レ−ザ発振器に使用
して好適な固体レ−ザ装置に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a solid-state laser device suitable for use in a laser oscillator.

【0002】[0002]

【従来の技術】一般にレ−ザ発振器は、レ−ザ電源から
固体レ−ザ装置の励起ランプに電力が供給されて、励起
ランプが点灯する。その光が集光器にて固体レ−ザ媒質
へ入射すると、固体レ−ザ媒質が励起されてレ−ザ発振
が起り、出力ミラ−からレ−ザ光が出射される。
2. Description of the Related Art Generally, in a laser oscillator, electric power is supplied from a laser power source to an excitation lamp of a solid-state laser device so that the excitation lamp is turned on. When the light is incident on the solid-state laser medium by the condenser, the solid-state laser medium is excited to cause laser oscillation, and laser light is emitted from the output mirror.

【0003】さて、従来の固体レ−ザ装置は図9および
図10に示すように構成され、図9は分解斜視図、図1
0は断面図である。そして、図中の符号1は蓋、2は励
起光集光機構で直方体部材3,筒状楕円反射鏡4,棒状
固体レ−ザ媒質5,棒状励起ランプ6からなっている。
又、7は直方体部材8に設けられた凹部9と透孔10,
11を有する保持機構であり、この保持機構7の凹部9
に励起光集光機構2が嵌合され、蓋1で覆われている。
尚、符号12は、直方体部材3の中心軸であると同時に
励起光集光機構2の中心軸でもある。
A conventional solid-state laser device is constructed as shown in FIGS. 9 and 10, and FIG. 9 is an exploded perspective view, FIG.
0 is a sectional view. In the figure, reference numeral 1 is a lid, 2 is an excitation light condensing mechanism, and is composed of a rectangular parallelepiped member 3, a cylindrical elliptical reflecting mirror 4, a rod-shaped solid laser medium 5, and a rod-shaped excitation lamp 6.
Reference numeral 7 denotes a recess 9 and a through hole 10 provided in the rectangular parallelepiped member 8.
And a recess 9 of the holding mechanism 7.
The excitation light condensing mechanism 2 is fitted to and is covered with the lid 1.
The reference numeral 12 is the central axis of the rectangular parallelepiped member 3 and at the same time the central axis of the excitation light focusing mechanism 2.

【0004】ところで、筒状楕円反射鏡4の2つの焦点
軸に一致するようにそれぞれ固体レ−ザ媒質5,励起ラ
ンプ6を配置した固体レ−ザ装置を用いてレ−ザ発振器
を構成し、レ−ザ発振を行なう場合、筒状楕円反射鏡4
の楕円断面の長軸方向に励起光が集光し易く、励起分布
が偏ることになる。これによってレ−ザ発振器より出力
されるレ−ザ光の断面形状が楕円となり、長軸方向と短
軸方向とで拡がり角が異なっている。
By the way, a laser oscillator is constructed by using a solid-state laser device in which a solid-state laser medium 5 and an excitation lamp 6 are arranged so as to coincide with the two focal axes of the cylindrical elliptical reflecting mirror 4. , When performing laser oscillation, the cylindrical elliptical reflecting mirror 4
The excitation light is likely to be condensed in the major axis direction of the elliptical cross section, and the excitation distribution is biased. As a result, the cross-sectional shape of the laser light output from the laser oscillator becomes elliptical, and the divergence angle differs between the major axis direction and the minor axis direction.

【0005】[0005]

【発明が解決しようとする課題】上記のような従来の固
体レ−ザ装置では、レ−ザ光を利用する場合の不具合と
なることが多い。そこで、複数の固体レ−ザ装置を用い
た多段形レ−ザ発振器において、個々の固体レ−ザ装置
全体を例えば90度づつ傾けて固定し、レ−ザ発振器全
体としては一様な励起を行ない、レ−ザ光の品質を向上
させる方法が行なわれている。しかし、この方法では固
体レ−ザ装置を保持する構造が複雑且つ大形となり、意
図した効果を安定して得難い、調整が煩雑となる、等の
不具合があった。この発明は、レ−ザ出力光の強度分布
および拡がり角が動径方向に対し一様なレ−ザ発振器を
得ることが出来る固体レ−ザ装置を提供することを目的
とする。
The conventional solid-state laser device as described above often causes a problem when utilizing laser light. Therefore, in a multistage laser oscillator using a plurality of solid-state laser devices, the individual solid-state laser devices as a whole are tilted and fixed, for example, by 90 degrees, so that the laser oscillator as a whole produces uniform excitation. A method for improving the quality of laser light has been implemented. However, with this method, the structure for holding the solid-state laser device becomes complicated and large, and it is difficult to obtain the intended effect in a stable manner, and the adjustment becomes complicated. It is an object of the present invention to provide a solid-state laser device capable of obtaining a laser oscillator in which the intensity distribution and spread angle of laser output light are uniform in the radial direction.

【0006】[0006]

【課題を解決するための手段】この発明は、直方体部材
に穿設形成された筒状楕円反射鏡内に棒状固体レ−ザ媒
質と棒状励起ランプが配置されてなる励起光集光機構
と、この励起光集光機構を保持する保持機構とを具備
し、更に上記の直方体部材はその中心軸に対し垂直な平
面での断面形状が上記中心軸上に中心を持つ正多角形又
は円形であり、且つ上記中心軸と上記固体レ−ザ媒質の
中心軸が一致するように構成されてなる固体レ−ザ装置
である。
SUMMARY OF THE INVENTION The present invention provides a pumping light condensing mechanism in which a rod-shaped solid laser medium and a rod-shaped pumping lamp are arranged in a cylindrical elliptical reflecting mirror formed in a rectangular parallelepiped member. The rectangular parallelepiped member has a cross-sectional shape in a plane perpendicular to the central axis, which is a regular polygon or a circle centered on the central axis. The solid-state laser device is configured so that the central axis and the central axis of the solid-state laser medium coincide with each other.

【0007】[0007]

【作用】この発明によれば、装置の構成部品を全く変更
することなく、励起光集光機構のみを光軸に対して回転
することによって励起分布の方向を回転させ、多段形レ
−ザ発振器全体の励起分布を一様とすることが出来る。
この結果、レ−ザ出力光の強度分布および拡がり角が動
径方向に対し一様なレ−ザ発振器を得ることが出来る。
According to the present invention, the direction of the excitation distribution is rotated by rotating only the excitation light converging mechanism with respect to the optical axis without changing the components of the apparatus, and the multistage laser oscillator is rotated. The entire excitation distribution can be made uniform.
As a result, it is possible to obtain a laser oscillator in which the intensity distribution and spread angle of the laser output light are uniform in the radial direction.

【0008】[0008]

【実施例】以下、図面を参照して、この発明の一実施例
を詳細に説明する。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the present invention will be described in detail below with reference to the drawings.

【0009】この発明による固体レ−ザ装置は、図1お
よび図2に示すように構成されているが、この発明では
励起光集光機構13を改良したもので、先ずこの励起光
集光機構13から述べることにする。
The solid-state laser device according to the present invention is constructed as shown in FIGS. 1 and 2. In the present invention, the pumping light collecting mechanism 13 is improved. Let's start from 13.

【0010】従来例(図9)と同一箇所には同一符号を
付すことにすると、励起光集光機構13は直方体部材1
4,筒状楕円反射鏡4,棒状固体レ−ザ媒質5,棒状励
起ランプ6からなっている。即ち、直方体部材14に
は、偏心して筒状楕円柱が穿設され、その内面に筒状楕
円反射鏡4が形成されている。この筒状楕円反射鏡4の
内側には、光増幅効果をもたらす1本の棒状固体レ−ザ
媒質5と、この固体レ−ザ媒質5を励起する1本の棒状
励起ランプ6とが所定間隔で配置されている。
If the same parts as those in the conventional example (FIG. 9) are designated by the same reference numerals, the excitation light focusing mechanism 13 has a rectangular parallelepiped member 1.
4, a cylindrical elliptical reflecting mirror 4, a rod-shaped solid-state laser medium 5, and a rod-shaped excitation lamp 6. That is, the rectangular parallelepiped member 14 is eccentrically provided with a cylindrical elliptic cylinder, and the cylindrical elliptical reflecting mirror 4 is formed on the inner surface thereof. Inside the cylindrical elliptical reflecting mirror 4, one rod-shaped solid-state laser medium 5 that produces an optical amplification effect and one rod-shaped excitation lamp 6 that excites this solid-state laser medium 5 are arranged at predetermined intervals. It is located at.

【0011】この場合、直方体部材14は図示のように
その中心軸15に対し垂直な平面での断面形状が、中心
軸15上に中心を持つ正多角形例えば正方形に形成され
ている。そして、この直方体部材14の中心軸15に対
し、筒状楕円反射鏡4,棒状固体レ−ザ媒質5,棒状励
起ランプ6の各中心軸はそれぞれ平行になっている。更
に、この発明では、直方体部材14の中心軸15と固体
レ−ザ媒質5の中心軸とが一致するように構成されてい
る。而も、固体レ−ザ媒質5,励起ランプ6はそれぞれ
筒状楕円反射鏡4の2つの焦点軸に一致するように、配
置されている。一方、上記の励起光集光機構13が収容
保持される保持機構7は、直方体部材8に凹部9と透孔
10,11が設けられてなり、この保持機構7の凹部9
に上記の励起光集光機構13が嵌合され、蓋1が覆われ
ている。
In this case, the rectangular parallelepiped member 14 is formed in a regular polygonal shape having a center on the central axis 15, for example, a square, as shown in the drawing, in a plane perpendicular to the central axis 15. The central axes 15 of the rectangular parallelepiped member 14 are parallel to the central axes of the cylindrical elliptical reflecting mirror 4, the rod-shaped solid laser medium 5, and the rod-shaped excitation lamp 6. Further, according to the present invention, the central axis 15 of the rectangular parallelepiped member 14 and the central axis of the solid laser medium 5 are aligned with each other. Moreover, the solid-state laser medium 5 and the excitation lamp 6 are arranged so as to coincide with the two focal axes of the cylindrical elliptical reflecting mirror 4. On the other hand, the holding mechanism 7 in which the above-mentioned excitation light condensing mechanism 13 is housed and held comprises a rectangular parallelepiped member 8 having a recess 9 and through holes 10 and 11, and the recess 9 of the holding mechanism 7
The excitation light condensing mechanism 13 described above is fitted to and the lid 1 is covered.

【0012】さて、上記のように直方体部材14の中心
軸15つまり励起光集光機構13の中心軸が、固体レ−
ザ媒質5の中心軸(光軸)と一致する構造になってお
り、且つ励起光集光機構13をその中心軸に垂直な平面
での断面がその中心軸上に中心を持つ正方形に構成する
と、励起光集光機構13のみをその中心軸について90
度づつ回転させることが可能となり、筒状楕円反射鏡4
の長軸方向を固体レ−ザ媒質5の中心軸に対し90度づ
つ回転することが出来る。
Now, as described above, the central axis 15 of the rectangular parallelepiped member 14, that is, the central axis of the excitation light converging mechanism 13 is the solid-state laser.
If the excitation light converging mechanism 13 has a structure that coincides with the central axis (optical axis) of the medium 5 and that the section of the excitation light condensing mechanism 13 in a plane perpendicular to the central axis is a square centered on the central axis. , 90 about the central axis of the pumping light focusing mechanism 13 only
It becomes possible to rotate by degrees, and the cylindrical elliptical reflecting mirror 4
The major axis direction of the solid laser medium 5 can be rotated by 90 degrees with respect to the central axis of the solid laser medium 5.

【0013】つまり、励起分布の偏りを、光軸に対し9
0度づつ回転させることが可能となる。これにより、保
持機構7および励起光集光機構13が1種類の部品で
も、励起分布の偏りの方向を変更することが可能とな
る。又、筒状楕円反射鏡4の楕円断面の長軸方向を、励
起光集光機構13の側面又は底面とのなす角は、任意の
角度でも良いが、これを45度となるようにすると、励
起光集光機構13を小形化することが出来る。
That is, the bias of the excitation distribution is 9 with respect to the optical axis.
It is possible to rotate by 0 degrees. This makes it possible to change the bias direction of the excitation distribution even if the holding mechanism 7 and the excitation light focusing mechanism 13 are one type of component. Further, the major axis direction of the elliptical cross section of the tubular elliptical reflecting mirror 4 may be an arbitrary angle with the side surface or the bottom surface of the excitation light converging mechanism 13, but if this is set to 45 degrees, The excitation light focusing mechanism 13 can be miniaturized.

【0014】上記のようなこの発明の固体レ−ザ装置を
採用すれば、部品の種類の増加、保守作業の不具合、調
整箇所の増加を招くことなく、安価で簡単な構造にて励
起分布を一様にした多段形レ−ザ発振器を得ることが出
来る。
If the solid-state laser device of the present invention as described above is adopted, the excitation distribution can be obtained with an inexpensive and simple structure without increasing the kinds of parts, the trouble of maintenance work, and the increase of adjustment points. It is possible to obtain a uniform multistage laser oscillator.

【0015】図2に、この発明の固体レ−ザ装置を採用
した場合の4段形レ−ザ発振器を示すが、図中の符号1
5,16はミラ−、17は楕円断面の長軸方向、18は
レ−ザ出力光パタ−ンである。 (他の実施例)図4〜図8はこの発明の他の実施例を示
したもので、上記実施例と同様効果が得られる。
FIG. 2 shows a four-stage laser oscillator in which the solid-state laser device of the present invention is adopted.
Reference numerals 5 and 16 are mirrors, 17 is a major axis direction of the elliptical cross section, and 18 is a laser output light pattern. (Other Embodiment) FIGS. 4 to 8 show another embodiment of the present invention, in which the same effect as the above embodiment can be obtained.

【0016】即ち、上記実施例では励起光集光機構13
の外観形状つまり直方体部材14はその中心軸に対し垂
直な平面での断面形状が、中心軸上に中心を持つ正方形
に形成されていたが、正方形に限定されることなく、正
多角形例えば図4に示すような正3角形の直方体部材1
9からなる励起光集光機構20、図5に示すような正6
角形の直方体部材21からなる励起光集光機構22を使
用することも出来る。これに伴ない、図4の保持機構2
3の凹部24は断面が正3角形であり、図5の保持機構
25の凹部26は断面が正6角形に対応し、蓋27も対
応している。
That is, in the above embodiment, the excitation light condensing mechanism 13 is used.
The outer shape of the rectangular parallelepiped member 14, that is, the cross-sectional shape on a plane perpendicular to the central axis of the rectangular parallelepiped member 14 is formed in a square shape having a center on the central axis, but the shape is not limited to the square shape, and may be a regular polygonal shape, for example. A regular rectangular parallelepiped member 1 as shown in FIG.
Excitation light condensing mechanism 20 consisting of 9, positive 6 as shown in FIG.
It is also possible to use the excitation light condensing mechanism 22 composed of a rectangular parallelepiped member 21. Along with this, the holding mechanism 2 of FIG.
The concave portion 24 of No. 3 has a regular triangular cross section, and the concave portion 26 of the holding mechanism 25 in FIG. 5 corresponds to a regular hexagonal sectional shape, and the lid 27 also corresponds.

【0017】一般に、直方体部材つまり励起光集光機構
の断面形状をn多角形とした場合、励起分布の偏りを
(360÷n)度づつ回転させることが可能である。
又、楕円断面の長軸方向と励起光集光機構の側面とのな
す角を90×(n−2)/n度とすると、最も小形化出
来る。
Generally, when the sectional shape of the rectangular parallelepiped member, that is, the excitation light condensing mechanism is an n-polygon, it is possible to rotate the bias of the excitation distribution by (360 ÷ n) degrees.
Further, if the angle between the major axis direction of the elliptical cross section and the side surface of the excitation light condensing mechanism is 90 × (n−2) / n degrees, the size can be minimized.

【0018】又、図6に示すような断面円形の直方体部
材28からなる励起光集光機構29を使用しても良く、
これに伴ない、保持機構30の凹部31は断面が円形に
対応し、蓋32も対応している。この場合は、励起分布
の偏りを任意の角度で回転させることが可能である。
Further, an excitation light condensing mechanism 29 composed of a rectangular parallelepiped member 28 having a circular cross section as shown in FIG. 6 may be used.
Accordingly, the recess 31 of the holding mechanism 30 has a circular cross section, and the lid 32 also has a corresponding cross section. In this case, the bias of the excitation distribution can be rotated at an arbitrary angle.

【0019】尚、各直方体部材19,21,28のそれ
ぞれ中心軸が、固体レ−ザ媒質5の中心軸に一致してい
る。又、各図では便宜上、励起ランプ6の図示は省略し
ている。
The central axes of the rectangular parallelepiped members 19, 21 and 28 coincide with the central axis of the solid laser medium 5. Further, in each drawing, the illustration of the excitation lamp 6 is omitted for convenience.

【0020】更に、図7および図8は、断面が正方形の
直方体部材14に連続的に形成された2つの筒状楕円反
射鏡33,34および35,36を使用した場合であ
り、2つの筒状楕円反射鏡33,34および35,36
に共通する焦点に固体レ−ザ媒質5が配置され、各筒状
楕円反射鏡33,34および35,36の焦点に励起ラ
ンプ6a,6bが配置されている。勿論、2つ以上の筒
状楕円反射鏡を用いることも可能である。
Further, FIGS. 7 and 8 show the case where two cylindrical elliptical reflecting mirrors 33, 34 and 35, 36 continuously formed on the rectangular parallelepiped member 14 having a square cross section are used. Elliptical reflectors 33, 34 and 35, 36
The solid-state laser medium 5 is arranged at the focal point common to the two, and the excitation lamps 6a and 6b are arranged at the focal points of the cylindrical elliptical reflecting mirrors 33, 34 and 35, 36, respectively. Of course, it is also possible to use two or more tubular elliptical reflecting mirrors.

【0021】[0021]

【発明の効果】この発明によれば、光軸に対する断面形
状が光軸上に中心を持つ正多角形又は円形である励起光
集光機構を用いているので、装置の構成部品を全く変更
することなく、励起光集光機構のみを光軸に対して回転
することによって励起分布の方向を回転させ、多段形レ
−ザ発振器全体の励起分布を一様とすることが出来る。
この結果、レ−ザ出力光の強度分布および拡がり角が動
径方向に対し一様なレ−ザ発振器を得ることが出来る。
According to the present invention, since the excitation light condensing mechanism whose cross-sectional shape with respect to the optical axis is a regular polygon or a circle centered on the optical axis is used, the components of the apparatus are completely changed. Without rotating the pumping light converging mechanism alone with respect to the optical axis, the direction of the pumping distribution can be rotated to make the pumping distribution of the entire multistage laser oscillator uniform.
As a result, it is possible to obtain a laser oscillator in which the intensity distribution and spread angle of the laser output light are uniform in the radial direction.

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

【図1】この発明の一実施例に係る固体レ−ザ装置を示
す分解斜視図。
FIG. 1 is an exploded perspective view showing a solid-state laser device according to an embodiment of the present invention.

【図2】この発明の固体レ−ザ装置を示す断面図。FIG. 2 is a sectional view showing a solid-state laser device of the present invention.

【図3】この発明の固体レ−ザ装置を用いたレ−ザ発振
器を示す斜視図。
FIG. 3 is a perspective view showing a laser oscillator using the solid-state laser device of the present invention.

【図4】この発明の他の実施例を示す分解斜視図。FIG. 4 is an exploded perspective view showing another embodiment of the present invention.

【図5】この発明の他の実施例を示す分解斜視図。FIG. 5 is an exploded perspective view showing another embodiment of the present invention.

【図6】この発明の他の実施例を示す分解斜視図。FIG. 6 is an exploded perspective view showing another embodiment of the present invention.

【図7】この発明の他の実施例を示す斜視図。FIG. 7 is a perspective view showing another embodiment of the present invention.

【図8】この発明の他の実施例を示す斜視図。FIG. 8 is a perspective view showing another embodiment of the present invention.

【図9】従来の固体レ−ザ装置を示す分解斜視図。FIG. 9 is an exploded perspective view showing a conventional solid-state laser device.

【図10】従来の固体レ−ザ装置を示す断面図。FIG. 10 is a sectional view showing a conventional solid-state laser device.

【符号の説明】[Explanation of symbols]

1…蓋、4…筒状楕円反射鏡,5…固体レ−ザ媒質,6
…励起ランプ、7…保持機構、8…直方体部材、9…凹
部、10,11…透孔、13…励起光集光機構、14…
直方体部材、15…中心軸。
1 ... Lid, 4 ... Cylindrical ellipsoidal mirror, 5 ... Solid-state laser medium, 6
... Excitation lamp, 7 ... Holding mechanism, 8 ... Rectangular member, 9 ... Recess, 10, 11 ... Through hole, 13 ... Excitation light condensing mechanism, 14 ...
Rectangular member, 15 ... Central axis.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 直方体部材に穿設形成された筒状楕円反
射鏡内に棒状固体レ−ザ媒質と棒状励起ランプが配置さ
れてなる励起光集光機構と、この励起光集光機構を保持
する保持機構とを具備する固体レ−ザ装置において、 上記直方体部材はその中心軸に対し垂直な平面での断面
形状が上記中心軸上に中心を持つ正多角形又は円形であ
り、且つ上記中心軸と上記固体レ−ザ媒質の中心軸が一
致するように構成されてなることを特徴とする固体レ−
ザ装置。
1. An excitation light condensing mechanism in which a rod-shaped solid-state laser medium and a rod-shaped excitation lamp are arranged in a cylindrical elliptical reflecting mirror formed in a rectangular parallelepiped member, and the excitation light condensing mechanism is held. In the solid-state laser device having a holding mechanism for holding, the rectangular parallelepiped member has a cross-sectional shape in a plane perpendicular to the central axis thereof, which is a regular polygon or a circle centered on the central axis, and A solid-state laser characterized in that the axis and the central axis of the solid-state laser medium coincide with each other.
The device.
JP31813491A 1991-12-02 1991-12-02 Solid-state laser device Pending JPH05160477A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP31813491A JPH05160477A (en) 1991-12-02 1991-12-02 Solid-state laser device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP31813491A JPH05160477A (en) 1991-12-02 1991-12-02 Solid-state laser device

Publications (1)

Publication Number Publication Date
JPH05160477A true JPH05160477A (en) 1993-06-25

Family

ID=18095885

Family Applications (1)

Application Number Title Priority Date Filing Date
JP31813491A Pending JPH05160477A (en) 1991-12-02 1991-12-02 Solid-state laser device

Country Status (1)

Country Link
JP (1) JPH05160477A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5828690A (en) * 1995-12-18 1998-10-27 General Electric Company Unitary body laser head
JP2002541670A (en) * 1999-03-30 2002-12-03 コミツサリア タ レネルジー アトミーク Laser Optical Pumping Module Including a Cylindrical Reflector with Polygonal Bottom

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5828690A (en) * 1995-12-18 1998-10-27 General Electric Company Unitary body laser head
JP2002541670A (en) * 1999-03-30 2002-12-03 コミツサリア タ レネルジー アトミーク Laser Optical Pumping Module Including a Cylindrical Reflector with Polygonal Bottom

Similar Documents

Publication Publication Date Title
US5946337A (en) Hybrid laser resonator with special line narrowing
US5432811A (en) Laser rod with polyhedron shaped ends
RU99105608A (en) LASER DEVICE
JPH05160477A (en) Solid-state laser device
US4096447A (en) Unstable resonator laser system
JP3285957B2 (en) Optical device
JPH02122581A (en) Laser oscillator
JP4047989B2 (en) Laser oscillator
JPH033377A (en) Semiconductor laser pumping solid-state laser device
JPH05259539A (en) Solid-state laser
JPH10107344A (en) Laser device
JPH033379A (en) Solid-state laser device
JPH02122586A (en) Solid state laser oscillator
KR0168880B1 (en) Laser oscillation apparatus
JPH11284256A (en) Solid laser device
JPH0637368A (en) Laser and beam expander
RU1817171C (en) Laser
JPH11177165A (en) Light excitation method for solid state laser
JP2580703B2 (en) Laser device
JPH0330482A (en) Laser device
JPS582062Y2 (en) solid state laser device
RU96115602A (en) INSTALLATION FOR LASER PROCESSING
JPH0738471B2 (en) Solid-state laser oscillator
JPH0751805Y2 (en) Broadband dye laser
JPH06334245A (en) Laser diode pumping solid state laser