JP2765351B2 - Laser-pumped solid-state laser - Google Patents

Laser-pumped solid-state laser

Info

Publication number
JP2765351B2
JP2765351B2 JP7521692A JP7521692A JP2765351B2 JP 2765351 B2 JP2765351 B2 JP 2765351B2 JP 7521692 A JP7521692 A JP 7521692A JP 7521692 A JP7521692 A JP 7521692A JP 2765351 B2 JP2765351 B2 JP 2765351B2
Authority
JP
Japan
Prior art keywords
laser
solid
state laser
medium
state
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 - Fee Related
Application number
JP7521692A
Other languages
Japanese (ja)
Other versions
JPH05243646A (en
Inventor
浩之 久保村
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.)
NEC Corp
Original Assignee
Nippon Electric Co 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 Nippon Electric Co Ltd filed Critical Nippon Electric Co Ltd
Priority to JP7521692A priority Critical patent/JP2765351B2/en
Publication of JPH05243646A publication Critical patent/JPH05243646A/en
Application granted granted Critical
Publication of JP2765351B2 publication Critical patent/JP2765351B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

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、レーザ光励起固体レー
ザに関する。
The present invention relates to a laser-pumped solid-state laser.

【0002】[0002]

【従来の技術】レーザ光励起固体レーザとしては、従
来、例えば図2に示すものが知られている。図2におい
て、21は固体レーザ媒質であり、これは円柱状のもの
である。この固体レーザ媒質21の略半外周側面には、
半円筒状のリフレクタ22が接着され、残りの半外周側
面に励起光源たる半導体レーザからのレーザ光23を照
射する。そして、固体レーザ媒質21の長手方向の一端
側に全反射鏡24が他端側に出力鏡25がそれぞれ配置
され、全体としてレーザ共振器を構成する。
2. Description of the Related Art As a laser beam pumped solid-state laser, for example, the one shown in FIG. 2 is conventionally known. In FIG. 2, reference numeral 21 denotes a solid-state laser medium, which has a cylindrical shape. On a substantially semi-peripheral side surface of the solid-state laser medium 21,
A semi-cylindrical reflector 22 is adhered, and the remaining semi-peripheral side surface is irradiated with laser light 23 from a semiconductor laser as an excitation light source. Then, a total reflection mirror 24 is arranged on one end side of the solid-state laser medium 21 in the longitudinal direction, and an output mirror 25 is arranged on the other end side, respectively.

【0003】以上の構成において、固体レーザ媒質21
の内部に透過したレーザ光は当該媒質に吸収されこれを
励起する。1回の透過で吸収されなかったレーザ光は、
リフレクタ22で反射され再度固体レーザ媒質21内に
入り吸収される。そして、固体レーザ媒質21の内部に
おいて光励起された部分は固体レーザ光に対する利得媒
質となり、レーザ共振器の作用により増幅され、固体レ
ーザ光が出力鏡25から出力される。
In the above configuration, the solid-state laser medium 21
The laser light transmitted through the inside is absorbed by the medium and excites the medium. The laser light that was not absorbed in one transmission is
The light is reflected by the reflector 22, enters the solid-state laser medium 21 again, and is absorbed. The light-excited portion inside the solid-state laser medium 21 becomes a gain medium for the solid-state laser light, is amplified by the action of the laser resonator, and the solid-state laser light is output from the output mirror 25.

【0004】[0004]

【発明が解決しようとする課題】上述した従来のレーザ
光励起固体レーザでは、固体レーザ媒質が円柱状のもの
であるので、その側面はレーザ光に対して凸レンズとし
て作用する。従って、図2(b)に示したように、レー
ザ光は固体レーザ媒質の全体を均一に光励起できず、利
得媒質に不均一な励起分布が生じ、固体レーザ光光軸が
偏った位置に形成される。従って、発振横モードを単一
にすると、高効率・高出力動作を実現するレーザ共振器
の設計が非常に面倒になるという問題がある。
In the above-mentioned conventional laser-pumped solid-state laser, since the solid-state laser medium has a cylindrical shape, the side surface acts as a convex lens for the laser light. Therefore, as shown in FIG. 2B, the laser light cannot uniformly excite the entire solid laser medium, and an uneven excitation distribution occurs in the gain medium, and the laser light is formed at a position where the optical axis of the solid laser light is deviated. Is done. Therefore, there is a problem that the design of the laser resonator that achieves high efficiency and high output operation becomes very troublesome when the oscillation lateral mode is made single.

【0005】本発明の目的は、レーザ光による励起分布
の均一化の図れる構造の固体レーザ媒質を備えたレーザ
光励起固体レーザを提供することにある。
It is an object of the present invention to provide a laser beam pumped solid-state laser having a solid-state laser medium having a structure capable of attaining a uniform pumping distribution by a laser beam.

【0006】[0006]

【課題を解決するための手段】前記目的を達成するため
に、本発明のレーザ光励起固体レーザは次の如き構成を
有する。即ち、本発明のレーザ光励起固体レーザは、レ
ーザ光励起固体レーザにおいて; 固体レーザ媒質は、
4角柱状のものからなり; 当該固体レーザ媒質の2つ
の対向側面の一方の対向側面の両側面にレーザ光入射部
としての凹レンズを密着配置してあると共に; 他方の
対向側面の両側面に完全拡散面を形成してある;ことを
特徴とするものである。
In order to achieve the above object, a laser beam pumped solid-state laser of the present invention has the following configuration. That is, the laser-pumped solid-state laser of the present invention is a laser-pumped solid-state laser;
The solid-state laser medium has a concave lens as a laser beam incident portion on both side surfaces of one of the two opposite side surfaces of the solid-state laser medium; and a complete surface on both side surfaces of the other opposite side surface. A diffusion surface is formed;

【0007】[0007]

【作用】次に、前記の如く構成される本発明のレーザ光
励起固体レーザの作用を説明する。本発明では、固体レ
ーザ媒質を4角柱状のものとし、その一方の対向側面の
両側面に凹レンズを密着し、その他方の対向側面の両側
面に完全拡散面を形成し、凹レンズを介して入射したレ
ーザ光が媒質内で拡がり完全拡散面で拡散されるように
してある。従って、媒質内が均一に光励起されるので、
固体レーザ光光軸の偏りをなくすことができ、高効率・
高出力動作のためのレーザ共振器の設計が容易となる。
Next, the operation of the laser-pumped solid-state laser of the present invention having the above-described structure will be described. In the present invention, the solid-state laser medium has a quadrangular prism shape, and a concave lens is adhered to both sides of one of the opposite sides, and a perfect diffusion surface is formed on both sides of the other opposite side, and light is incident through the concave lens. The laser beam spreads in the medium and is diffused on the perfect diffusion surface. Therefore, since the inside of the medium is uniformly photoexcited,
It can eliminate the deviation of the optical axis of solid-state laser light,
The design of the laser resonator for high-power operation is facilitated.

【0008】[0008]

【実施例】以下、本発明の実施例を図面を参照して説明
する。図1は、本発明の一実施例に係るレーザ光励起固
体レーザを示す。図1において、固体レーザ媒質1は、
4角柱状のものからなり、この固体レーザ媒質1の2つ
の対向側面のうち、一方の対向側面の両側面にレーザ光
入射部としての凹レンズ2a、同2bをオプティカルコ
ンタクトで密着してあり、他方の対向側面の両側面に完
全拡散面3a、同3bを形成してある。
Embodiments of the present invention will be described below with reference to the drawings. FIG. 1 shows a laser-pumped solid-state laser according to one embodiment of the present invention. In FIG. 1, the solid-state laser medium 1 is
The solid-state laser medium 1 has a concave lens 2a and a concave lens 2b as laser light incident portions which are in close contact with both side surfaces of one of the two opposing side surfaces of the solid laser medium 1 by optical contact. The perfect diffusion surfaces 3a and 3b are formed on both side surfaces of the opposite side surface.

【0009】なお、完全拡散面3a、同3bは、砂ずり
面に研磨した媒質側面にBaSO4を主成分とする塗料
を塗布して形成したものである。
The complete diffusion surfaces 3a and 3b are formed by applying a paint containing BaSO 4 as a main component on the side surface of the polished sand medium.

【0010】以上の構成において、レーザ光4a(4
b)は、凹レンズ2a(2b)を介して固体レーザ媒質
1内に入力すると、凹レンズの作用により媒質内で拡が
るが、図1(b)に示すように、完全拡散面3a(3
b)の形成面に達しそこの完全拡散面で拡散され媒質内
の隅々まで浸透する。つまり、レーザ光4a(4b)は
固体レーザ媒質1の内部を均一に光励起する。その後は
図2の場合と同様である。
In the above configuration, the laser beam 4a (4
b), when input into the solid-state laser medium 1 through the concave lens 2a (2b), expands in the medium due to the action of the concave lens, but as shown in FIG.
It reaches the formation surface of b), is diffused by the perfect diffusion surface there, and penetrates all corners in the medium. That is, the laser light 4a (4b) uniformly optically pumps the inside of the solid-state laser medium 1. After that, it is the same as the case of FIG.

【0011】前記したように、媒質内の光励起された部
分が利得媒質となるが、本発明では媒質内が均一に励起
されるので、固体レーザ光光軸の偏りがなく、高効率・
高出力動作のためのレーザ共振器の設計が容易になる。
As described above, the light-excited portion in the medium becomes the gain medium. However, in the present invention, since the inside of the medium is uniformly excited, there is no deviation of the optical axis of the solid-state laser and high efficiency and high efficiency.
The design of the laser resonator for high-power operation is facilitated.

【0012】[0012]

【発明の効果】以上説明したように、本発明のレーザ光
励起固体レーザによれば、固体レーザ媒質を4角柱状の
ものとし、その一方の対向側面の両側面に凹レンズを密
着し、その他方の対向側面の両側面に完全拡散面を形成
し、凹レンズを介して入射したレーザ光が媒質内で拡が
り完全拡散面で拡散されるようにしてあるので、媒質内
が均一に光励起され、固体レーザ光光軸の偏りをなくす
ことができ、高効率・高出力動作のためのレーザ共振器
の設計が容易となる効果がある。
As described above, according to the laser-excited solid-state laser of the present invention, the solid-state laser medium is formed in a quadrangular prism shape, and concave lenses are adhered to both sides of one of the opposite sides, and A perfect diffusion surface is formed on both sides of the opposite side surface, and the laser light incident through the concave lens is spread in the medium and diffused on the perfect diffusion surface. There is an effect that the deviation of the optical axis can be eliminated and the design of the laser resonator for high efficiency and high output operation becomes easy.

【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レーザ光励起固体レー
ザの概念構成図であり、(a)は側面図、(b)は断面
図である。
FIGS. 1A and 1B are conceptual configuration diagrams of a laser-pumped solid-state laser according to one embodiment of the present invention, wherein FIG. 1A is a side view and FIG.

【図2】従来のレーザ光励起固体レーザの概念構成図で
あり、(a)は側面図、(b)は断面図である。
FIG. 2 is a conceptual configuration diagram of a conventional laser beam pumped solid-state laser, in which (a) is a side view and (b) is a cross-sectional view.

【符号の説明】[Explanation of symbols]

1 固体レーザ媒質 2a 凹レンズ 2b 凹レンズ 3a 完全拡散面 3b 完全拡散面 4a レーザ光 4b レーザ光 Reference Signs List 1 solid laser medium 2a concave lens 2b concave lens 3a perfect diffusion surface 3b perfect diffusion surface 4a laser beam 4b laser beam

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 レーザ光励起固体レーザにおいて; 固
体レーザ媒質は、4角柱状のものからなり; 当該固体
レーザ媒質の2つの対向側面の一方の対向側面の両側面
にレーザ光入射部としての凹レンズを密着配置してある
と共に; 他方の対向側面の両側面に完全拡散面を形成
してある; ことを特徴とするレーザ光励起固体レー
ザ。
A solid-state laser medium having a quadrangular prism shape; and a concave lens serving as a laser beam incident portion provided on both sides of one of two opposite sides of the solid-state laser medium. A laser light pumped solid-state laser, wherein the laser light pumped solid-state laser is in close contact with each other;
JP7521692A 1992-02-26 1992-02-26 Laser-pumped solid-state laser Expired - Fee Related JP2765351B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP7521692A JP2765351B2 (en) 1992-02-26 1992-02-26 Laser-pumped solid-state laser

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7521692A JP2765351B2 (en) 1992-02-26 1992-02-26 Laser-pumped solid-state laser

Publications (2)

Publication Number Publication Date
JPH05243646A JPH05243646A (en) 1993-09-21
JP2765351B2 true JP2765351B2 (en) 1998-06-11

Family

ID=13569802

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7521692A Expired - Fee Related JP2765351B2 (en) 1992-02-26 1992-02-26 Laser-pumped solid-state laser

Country Status (1)

Country Link
JP (1) JP2765351B2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP5085007B2 (en) * 2005-01-13 2012-11-28 浜松ホトニクス株式会社 Solid-state laser amplifier and solid-state laser oscillator
KR102388949B1 (en) * 2020-12-18 2022-04-22 한국과학기술원 Efficient and directional non-resonance laser using scattering cavity and manufacturing method thereof

Also Published As

Publication number Publication date
JPH05243646A (en) 1993-09-21

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