JPH088477A - Solid state laser device - Google Patents
Solid state laser deviceInfo
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- JPH088477A JPH088477A JP8460895A JP8460895A JPH088477A JP H088477 A JPH088477 A JP H088477A JP 8460895 A JP8460895 A JP 8460895A JP 8460895 A JP8460895 A JP 8460895A JP H088477 A JPH088477 A JP H088477A
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- Prior art keywords
- solid
- state laser
- laser medium
- laser device
- excitation
- 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.)
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Abstract
Description
【０００１】[0001]
【産業上の利用分野】本発明は、高輝度・高出力の固体
レーザ装置に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a high-brightness, high-output solid-state laser device.
【０００２】[0002]
【従来の技術】従来、高出力の固体レーザ装置の構成の
一つとして、固体レーザ媒質をロッド型とし、光軸をロ
ッドの中心軸方向に取る構成が知られている。この構成
では、ロッドの周囲に冷却水を流してロッドを冷却する
構成をとるので、製造、保守が容易で実用性の高い装置
を安価に提供できる利点がある。しかしながら、ロッド
中心と周辺部との温度差に基づく複屈折効果等によりビ
ーム品質が劣化するという問題がある。この熱歪を低減
する一つの方法として、ロッドの中心をくり抜いて冷却
媒質をロッドの中心軸にも流して冷却効率を高める装置
構成が、特開昭６２−２６２４８０号公報にスタンリー
リーム等により報告されている。2. Description of the Related Art Conventionally, as one of the configurations of a high-power solid-state laser device, a configuration is known in which the solid-state laser medium is a rod type and the optical axis is in the central axis direction of the rod. In this configuration, since the rod is cooled by flowing cooling water around the rod, there is an advantage that a device that is easy to manufacture and maintain and has high practicality can be provided at low cost. However, there is a problem that the beam quality is deteriorated due to a birefringence effect or the like based on a temperature difference between the rod center and the peripheral portion. As one method of reducing this thermal strain, an apparatus configuration for cutting the center of the rod and flowing the cooling medium also to the central axis of the rod to enhance the cooling efficiency is reported by Stanley Ream in JP-A-62-262480. Has been done.
【０００３】また、前記したようなロッド型レーザ媒質
を用いる場合に生じる問題を改善するものとして、板上
の固体レーザ媒質中でじぐざぐに折り返す光路を光軸と
することにより、熱歪による複屈折を補償するスラブ型
固体レーザ装置が知られている。この方式により高輝度
のレーザ装置を得る構成として、特開平２−１１９１９
２号公報に八木等により、スラブ型レーザに一軸方向の
不安定共振器構成を適用した例が報告されている。一般
にスラブ型では、薄く平たいスラブほど熱歪を低くでき
る点で有効であるが、大出力化のためには、励起体積を
大きく得るために横幅の長いスラブ構成のレーザ媒質を
用いる必要があり、これにより横幅方向のビーム品質劣
化を生じるので、上記発明では、その方向のビーム品質
劣化を抑えるために不安定共振器を適用している。In order to improve the problems that occur when the rod-type laser medium is used, the optical path that is zigzag-folded in the solid-state laser medium on the plate is used as the optical axis, so that a compound due to thermal strain is generated. A slab type solid-state laser device that compensates refraction is known. As a structure for obtaining a high-brightness laser device by this method, Japanese Patent Application Laid-Open No. 2-119919
No. 2, Yagi et al. Report an example in which a uniaxial unstable resonator configuration is applied to a slab laser. Generally, in the slab type, a thin and flat slab is effective in that the thermal strain can be lowered, but in order to increase the output, it is necessary to use a laser medium having a long slab configuration in order to obtain a large excitation volume. This causes deterioration of the beam quality in the width direction, and therefore, in the above invention, the unstable resonator is applied to suppress the deterioration of the beam quality in that direction.
【０００４】[0004]
【発明が解決しようとする課題】従来のロッド型固体レ
ーザ装置を用いる方式では、ロッド中心と周辺の温度差
に伴う熱歪を介して生じる複屈折や熱レンズ効果によ
り、高輝度かつ大出力な固体レーザ装置を得ることは困
難である。また中抜きロッドを用いる方式では、出射ビ
ームが中抜けとなり、レンズによる集光性が劣るほか、
ビーム形状が伝搬距離とともに変化するなど実用上使い
にくいという問題がある。In the conventional system using a rod-type solid-state laser device, high brightness and large output are obtained due to birefringence and thermal lens effect generated through thermal strain caused by a temperature difference between the center and the periphery of the rod. It is difficult to obtain a solid-state laser device. Also, in the method using the hollow rod, the emitted beam becomes hollow, and the condensing property of the lens is inferior.
There is a problem that it is practically difficult to use, for example, the beam shape changes with the propagation distance.
【０００５】一方、スラブ型レーザでは、レーザ出射面
のビームがスラブ面に対して縦方向と横方向で品質及び
ビーム幅が異なり、出射ビームの集光性の異方性を生
じ、ビームの取り扱いが複雑となる問題がある。また、
スラブの全反射面が冷却面を兼ねるために、長期間の運
転により冷却面の汚れ等により出力が低下する等、経時
劣化が生じ易いという問題がある。On the other hand, in a slab type laser, the quality and beam width of the beam on the laser emission surface differ in the vertical and horizontal directions with respect to the slab surface. Is complicated. Also,
Since the total reflection surface of the slab also serves as the cooling surface, there is a problem that deterioration over time easily occurs, such as a decrease in output due to dirt on the cooling surface during long-term operation.
【０００６】また、上記のいずれの方式においても、励
起入力の変化に対して、ロッドもしくはスラブ媒質の熱
レンズ効果の大きさが変化し、そのために共振器の動作
点が最適点から外れるために、出射ビームのビーム品質
及び、入力に対する出力の線形性が励起入力の変化に伴
い低下するという問題がある。Further, in any of the above-mentioned methods, the magnitude of the thermal lens effect of the rod or slab medium changes with the change of the excitation input, which causes the operating point of the resonator to deviate from the optimum point. However, there is a problem that the beam quality of the output beam and the linearity of the output with respect to the input deteriorate with the change of the excitation input.
【０００７】[0007]
【発明の目的】本発明の目的は、このような問題を解消
し、高効率で高出力、かつ高品質なレーザビームを得る
ことが可能な固体レーザ装置を提供することにある。SUMMARY OF THE INVENTION An object of the present invention is to provide a solid-state laser device which can solve such a problem and can obtain a high-efficiency, high-output, high-quality laser beam.
【０００８】[0008]
【課題を解決するための手段】本発明の固体レーザ装置
は、レーザ発振波長に対して高反射面と高透過面を持つ
固体レーザ媒質と、前記固体レーザ媒質を励起する励起
光源と、励起光を前記固体レーザ媒質に導く光学系と、
レーザ共振器を構成する出力鏡からなる固体レーザ装置
において、前記固体レーザ媒質の高反射面側にヒートシ
ンクを接合し、固体レーザ媒質を光軸に垂直な面内で一
様に励起する照明光学系を設けたことを特徴とする。A solid-state laser device according to the present invention comprises a solid-state laser medium having a high reflection surface and a high transmission surface with respect to a laser oscillation wavelength, an excitation light source for exciting the solid-state laser medium, and an excitation light. An optical system for guiding the solid-state laser medium,
In a solid-state laser device including an output mirror forming a laser resonator, a heat sink is joined to the high-reflecting surface side of the solid-state laser medium to uniformly excite the solid-state laser medium in a plane perpendicular to the optical axis. Is provided.
【０００９】また、本発明の固体レーザ装置は、固体レ
ーザ媒質とヒートシンクとの間に、固体レーザ媒質との
接触面積を半径方向に変化させる空隙部を多数もつ熱伝
達体を備えることを特徴とする。この場合、励起強度分
布が、所定半径の範囲内で一様な強度分布となる励起光
学系を用い、熱伝達体は前記所定半径と同じ外径で、固
体レーザ媒質との接触面に格子状の溝を有することが好
ましい。或いは、励起強度分布が、中心部で強く半径方
向に弱くなる強度分布をもつ励起光学系を用い、熱伝達
体は固体レーザ媒質との接触面に半径方向の接触面積率
の分布が励起光強度分布と等しくなる同心円状の溝を有
することが好ましい。Further, the solid-state laser device of the present invention is characterized by including a heat transfer body having a large number of voids between the solid-state laser medium and the heat sink for changing the contact area with the solid-state laser medium in the radial direction. To do. In this case, an excitation optical system is used in which the excitation intensity distribution has a uniform intensity distribution within a predetermined radius, and the heat transfer body has the same outer diameter as the predetermined radius, and has a grid-like shape on the contact surface with the solid-state laser medium. It is preferable to have the groove of. Alternatively, an excitation optical system having an intensity distribution in which the excitation intensity distribution is strong at the center and weakened in the radial direction is used, and the distribution of the contact area ratio in the radial direction at the contact surface with the solid-state laser medium is the excitation light intensity. It is preferable to have concentric grooves that are equal in distribution.
【００１０】[0010]
【作用】本発明では、固体レーザ媒質の光軸と熱流の向
きを同一方向に合わせることにより、固体レーザ媒質に
生じる温度勾配を光軸と同じ方向とすることで、レーザ
発振光の波面歪の発生を根本的に無くすことができると
の新しい知見による。実際的なレーザ媒質の形として、
例えば、円盤状の固体レーザ媒質を用いた場合、円盤の
一面を高反射面として、この高反射面をヒートシンクに
接合させ、かつ、円盤の反対側の面から励起光を均一に
照射することで、固体レーザ媒質の光軸に垂直な平面内
での温度分布の発生を抑えることができる。According to the present invention, the optical axis of the solid-state laser medium and the direction of the heat flow are aligned in the same direction so that the temperature gradient generated in the solid-state laser medium is in the same direction as the optical axis. According to a new finding that the occurrence can be completely eliminated. As a practical form of laser medium,
For example, when a disk-shaped solid laser medium is used, one surface of the disk is a high reflection surface, this high reflection surface is bonded to a heat sink, and the excitation light is uniformly irradiated from the opposite surface of the disk. In addition, the occurrence of temperature distribution in a plane perpendicular to the optical axis of the solid-state laser medium can be suppressed.
【００１１】また、本発明では、熱伝達体の接触面に形
成した格子状の溝により形成されるヒダ状の非接触部
（空隙）により生じる熱伝達体の弾性変形によって、接
触部の応力発生を吸収することで、固体レーザ媒質の歪
発生を防止することが可能となる。さらに、中心軸対称
の励起光の強度分布に応じて熱伝達体の接触面に形成し
た溝が同心円状であるため、熱伝達体の接触面積率（面
積当たりの、接触部と非接触部の面積の比）が半径方向
に変化され、これにより中心軸対称の励起光の強度分布
に対応してレーザ発振光軸に垂直な面内で半径方向に熱
伝達率が変化され、固体レーザ媒質の接触部の歪発生が
防止される。Further, in the present invention, stress generation at the contact portion is caused by elastic deformation of the heat transfer member caused by a fold-like non-contact portion (gap) formed by a lattice-like groove formed on the contact surface of the heat transfer member. By absorbing this, it is possible to prevent distortion from occurring in the solid-state laser medium. Furthermore, since the grooves formed on the contact surface of the heat transfer member are concentric according to the intensity distribution of the excitation light symmetrical about the central axis, the contact area ratio of the heat transfer member (the ratio of the contact portion and the non-contact portion per area, Area ratio) is changed in the radial direction, whereby the heat transfer coefficient is changed in the radial direction in a plane perpendicular to the laser oscillation optical axis in accordance with the intensity distribution of the excitation light symmetrical about the central axis. The occurrence of distortion at the contact portion is prevented.
【００１２】[0012]
【実施例】本発明を図面を参照して説明する。図１は、
本発明の一実施例の固体レーザ装置の構成を示す図であ
る。同図において、円盤状のＮｄ：ＹＡＧ結晶（直径３
ｃｍ、厚み１ｃｍ）からなる固体レーザ媒質４は、円盤
面の片面に金蒸着を施した高反射ミラー２を介して冷却
水を流す銅ブロックからなるヒートシンク３に直接接合
され、また円盤面の他の一面は発振レーザ光及び、励起
光に対してＡＲコートが施されている。レーザ共振器
は、固体レーザ媒質４と、レーザ共振器を構成する出力
鏡９の間に、ビーム拡大器８、及び励起光を反射し発振
光を透過するダイクロイックミラー７を挟んで構成す
る。BRIEF DESCRIPTION OF THE DRAWINGS FIG. Figure 1
FIG. 1 is a diagram illustrating a configuration of a solid-state laser device according to an embodiment of the present invention. In the figure, a disk-shaped Nd: YAG crystal (diameter 3
cm, thickness 1 cm), the solid-state laser medium 4 is directly bonded to a heat sink 3 made of a copper block for flowing cooling water through a high-reflecting mirror 2 on one side of which a gold surface is vapor-deposited. AR coating is applied to the oscillated laser light and the excitation light on one surface. The laser resonator is configured by sandwiching a beam expander 8 and a dichroic mirror 7 that reflects pumping light and transmits oscillating light between a solid-state laser medium 4 and an output mirror 9 that constitutes the laser resonator.
【００１３】平均出力５００Ｗ（１００μｓパルス幅、
繰り返し１ＫＨｚ）のパルス動作の半導体レーザ光源８
個からなる合計出力４００Ｗの励起光源５の出射光は、
蠅の目レンズ光学系からなる、照明光学系６により均一
な照度分布の光束に変換され、ダイクロイックミラー７
を介して、固体レーザ媒質４に円盤面の高透過面側から
入射し、固体レーザ媒質４の円盤面内を均一に励起する
構成を取っている。ビーム拡大器８は、大口径のレーザ
媒質を用いる場合に、短い共振器長で高次横モードの発
振を抑えるために設ける。ビーム拡大器８の拡大倍率は
７倍、レーザ共振器長５０ｃｍ、出力鏡９の曲率３ｍ、
反射率９０％として、レーザ出力特性を調べた。Average output 500 W (100 μs pulse width,
Repetitive 1 KHz) pulsed semiconductor laser light source 8
The light emitted from the excitation light source 5 having a total output of 400 W is
The light is converted into a light flux having a uniform illuminance distribution by an illumination optical system 6 composed of a fly-eye lens optical system, and the dichroic mirror 7
, The laser beam enters the solid-state laser medium 4 from the high transmission surface side of the disk surface, and uniformly excites the disk surface of the solid-state laser medium 4. When a large-diameter laser medium is used, the beam expander 8 is provided in order to suppress oscillation of a high-order transverse mode with a short resonator length. The magnification of the beam expander 8 is 7 times, the laser cavity length is 50 cm, the curvature of the output mirror 9 is 3 m,
Laser output characteristics were examined with a reflectivity of 90%.
【００１４】その結果、励起入力４００Ｗにおいて、レ
ーザ出力２５０Ｗの基本横モードの発振を実現できた。
従来方式と比べると、励起効率が６３％と高いことは、
熱歪に起因する回折損失に伴う共振器損失を大幅に低減
できたためである。また、従来方式のロッド型やスラブ
型レーザでは、程度の差はあるものの励起入力の変化に
伴う熱レンズ効果により、共振器の最適動作条件が変化
するために、広い出力範囲で高いビーム品質及び入出力
の線形性を維持することは極めて困難であったが、本発
明による装置では、熱レンズ効果の発生がないために、
低出力から最大出力まで、入出力の線形性を保ちなが
ら、基本横モードの高品質なビーム品質を実現すること
ができた。その時、出射ビームの広がり角も励起の大き
さによらず一定値を保つ優れた特性が得られた。なお高
反射ミラー２に、通常のレーザミラーに用いられる誘電
体多層膜を用いても、多層膜の厚みが数μｍ程度と薄い
ことから、金属反射体を用いる場合と比べて固体レーザ
媒質４とヒートシンク３の間の温度差にほとんど差はな
いので使うことができる。As a result, a fundamental transverse mode oscillation with a laser output of 250 W was realized at an excitation input of 400 W.
The excitation efficiency is 63%, which is higher than that of the conventional method.
This is because the resonator loss due to the diffraction loss caused by the thermal strain can be significantly reduced. In the conventional rod-type and slab-type lasers, although the degree varies, the optimum operating condition of the resonator changes due to the thermal lens effect accompanying the change in the pumping input. Although it was extremely difficult to maintain the linearity of the input and output, in the device according to the present invention, since the thermal lens effect does not occur,
From low power to maximum power, high beam quality in the basic transverse mode was realized while maintaining input / output linearity. At that time, an excellent characteristic was obtained in which the divergence angle of the output beam was kept constant regardless of the magnitude of the excitation. Even if a dielectric multilayer film used for a normal laser mirror is used for the high-reflecting mirror 2, since the thickness of the multilayer film is as thin as several μm, the solid laser medium 4 and the solid laser medium 4 are different from those when a metal reflector is used. Since there is almost no difference in temperature between the heat sinks 3, it can be used.
【００１５】上記の実施例において、固体レーザ媒質４
は、平行平面の場合について述べたが、複合共振器効果
を避けるために１度程度の僅かなテーパをつけてもかま
わない。テーパをつけることにより、テーパ方向の光路
長差及び温度差により波面歪を生じるが、従来のロッド
型発振器における歪に比べると一桁以上小さく、本発明
の効果を十分生かすことができる。In the above embodiment, the solid-state laser medium 4
In the above, the case of parallel planes was described, but a slight taper of about 1 degree may be added to avoid the compound resonator effect. The taper causes a wavefront distortion due to a difference in optical path length and a difference in temperature in the taper direction. However, the distortion is smaller than that of the conventional rod-type oscillator by one digit or more, so that the effects of the present invention can be fully utilized.
【００１６】次に本発明の第２の実施例の構成図を図２
に示す。図１と異なる点は、ヒートシンク３にヒートパ
イプ方式を適用したこと、レーザ共振器の構成に不安定
共振器構成を適用した点、励起光をレーザ発振モードの
外側から斜め方向から固体レーザ媒質４に励起光を導く
構成を用いた点である。ヒートシンク３は冷却媒質を水
とし、内部に水の還流用の毛細メッシュ網１０を配置
し、固体レーザ媒質４の高反射面はヒートシンク３の内
壁の一部となっている。フィン１１は発熱を空気中に放
出するために用いる。出力鏡９は高反射部の直径が１５
ｍｍ、最大反射率９５％のスーパガウシャンミラーを用
いた。固体レーザ媒質４のサイズは第１の実施例と同じ
で、固体レーザ媒質４の側面に設けた反射板１２は固体
レーザ媒質４から洩れでた励起光成分を再度固体レーザ
媒質４に吸収させる機能を持つ。FIG. 2 is a block diagram of a second embodiment of the present invention.
Shown in The difference from FIG. 1 is that a heat pipe method is applied to the heat sink 3, an unstable resonator configuration is applied to the configuration of the laser resonator, and the solid-state laser medium 4 is excited from outside the laser oscillation mode. This is the point that a configuration for guiding the excitation light to the light source is used. The heat sink 3 uses water as a cooling medium, and a capillary mesh 10 for circulating water is disposed inside. The high reflection surface of the solid laser medium 4 is a part of the inner wall of the heat sink 3. The fins 11 are used to release heat to the air. The output mirror 9 has a high-reflectance diameter of 15
A super Gaussian mirror having a maximum reflectance of 95 mm and a maximum reflectance of 95% was used. The size of the solid-state laser medium 4 is the same as that of the first embodiment, and the reflection plate 12 provided on the side surface of the solid-state laser medium 4 has the function of absorbing the pumping light component leaking from the solid-state laser medium 4 into the solid-state laser medium 4 again. have.
【００１７】この実施例では、ヒートパイプ式の冷却を
行うことで、高反射ミラー２の面内の温度差の発生を
０．１℃程度に低減できることと、冷却面に金属ブロッ
ク等が直接接していないために、固体レーザ媒質４に冷
却面での応力歪の発生を著しく小さく抑えられることか
ら、レーザ発振における波面歪を第１の実施例の場合に
比べ一層低減できる。In this embodiment, by performing the heat pipe type cooling, the occurrence of the temperature difference in the surface of the high reflection mirror 2 can be reduced to about 0.1 ° C., and the metal block or the like directly contacts the cooling surface. Since the occurrence of stress distortion on the cooling surface of the solid-state laser medium 4 can be suppressed to a remarkably small level, the wavefront distortion in laser oscillation can be further reduced as compared with the case of the first embodiment.
【００１８】また、共振器長を５０ｃｍとし、励起光源
として平均出力５０Ｗ（１００μｓパルス幅、繰り返し
１ＫＨｚ）のパルス動作半導体レーザ４個、計２００Ｗ
の出力で励起した場合に基本横モードで最大レーザ平均
出力１４０Ｗが得られ、変換効率７０％の高効率かつ高
品質な固体レーザ装置を実現できた。第１の実施例の場
合と同様に、励起入力に対するビーム品質の低下は無
く、かつ入出力の線形性にも優れる特性が得られた。Further, the resonator length is set to 50 cm, and four pulse-operating semiconductor lasers having an average output of 50 W (100 μs pulse width, repetition rate of 1 KHz) as excitation light sources, total 200 W.
A maximum laser average output of 140 W was obtained in the fundamental transverse mode when pumped with the output of, and a high-efficiency and high-quality solid-state laser device with a conversion efficiency of 70% was realized. As in the case of the first embodiment, the characteristics of the beam quality with respect to the pumping input were not deteriorated and the input / output linearity was excellent.
【００１９】以上述べた本発明の第１及び第２の実施例
では、共振器構成として、それぞれビーム拡大器を用い
る安定共振器及び、スーパガウシャンミラーを用いる不
安定共振器を適用した場合について述べた。従来のロッ
ド型やスラブ型のレーザでこれらの共振器構成が適用さ
れていたが、従来は熱歪による波面歪の影響を最小限に
抑え、大出力時のビーム品質の劣化を抑えるものが主眼
であった。本発明においては固体レーザ装置による波面
歪が大出力時にも本質的に低減できているために、上記
の安定型や不安定共振器構成を本来の高次横モード発振
の抑止の目的のみに用いることができ、その結果、副次
的な共振器損失を最小限に抑えた上で低次横モード発振
を実現でき、ビーム品質の劣化を抑えるだけでなく、励
起光からレーザ出力への変換効率を大幅に向上できた。In the above-described first and second embodiments of the present invention, the case where a stable resonator using a beam expander and an unstable resonator using a super Gaussian mirror are applied as resonator configurations, respectively. Stated. These resonator configurations have been applied to conventional rod-type and slab-type lasers, but the main focus here is to minimize the effect of wavefront distortion due to thermal distortion and to prevent deterioration of beam quality at high output. Met. In the present invention, since the wavefront distortion due to the solid-state laser device can be essentially reduced even at the time of large output, the above-mentioned stable type or unstable resonator configuration is used only for the purpose of suppressing the original higher-order transverse mode oscillation. As a result, it is possible to realize low-order transverse mode oscillation while minimizing the secondary cavity loss, and not only suppress the deterioration of beam quality, but also convert the pump light to the laser output efficiency. Was greatly improved.
【００２０】以上述べた本発明の実施例においては、励
起光源に半導体レーザを用いた場合について述べたが、
励起光源に、フラッシュランプや、アークランプなどの
ランプ光源を適用できることは言うまでもない。In the embodiment of the present invention described above, the case where the semiconductor laser is used as the excitation light source has been described.
It goes without saying that a lamp light source such as a flash lamp or an arc lamp can be applied to the excitation light source.
【００２１】図３に本発明の第３実施例を示しており、
ここでは３ｃｍ角、１ｃｍ厚のＮｄ：ＹＡＧ結晶からな
る薄い直方体の固体レーザ媒質４の側面に励起光源を配
置している。図において、フラッシュランプからなる励
起光源５は円筒状の拡散反射面を持つ照明光学計６で反
射されて、固体レーザ媒質４に導かれる。固体レーザ媒
質４のレーザ光に対する高反射面、及び高透過面は、フ
ラッシュランプからの励起光を反射する特性を持たせる
ことにより、固体レーザ媒質４を均一性よく励起するこ
とができる。図２に示す実施例と同じ共振器構成を用い
て発振特性を調べた。なお、フラッシュランプの冷却は
円筒状の照明光学系内を流れる水流で行うが、図には記
述していない。この構成において、フラッシュランプへ
の入力３ＫＷ（１００Ｈｚ，３０Ｊ）において、レーザ
出力６００Ｗが得られ、その時のビーム品質を示すＭ2
値は２と、回折限界の２倍程度の優れたビーム品質が得
られた。FIG. 3 shows a third embodiment of the present invention.
Here, an excitation light source is arranged on the side surface of a thin rectangular solid laser medium 4 made of a 3 cm square, 1 cm thick Nd: YAG crystal. In the figure, an excitation light source 5 composed of a flash lamp is reflected by an illumination optics 6 having a cylindrical diffuse reflection surface and guided to a solid-state laser medium 4. The solid-state laser medium 4 has a high-reflection surface and a high-transmission surface with respect to laser light, and has a property of reflecting excitation light from a flash lamp, so that the solid-state laser medium 4 can be excited with high uniformity. The oscillation characteristics were examined using the same resonator configuration as the embodiment shown in FIG. The cooling of the flash lamp is performed by a water stream flowing through the cylindrical illumination optical system, but is not shown in the figure. In this configuration, when the input to the flash lamp is 3 KW (100 Hz, 30 J), a laser output of 600 W is obtained, and M 2 indicating the beam quality at that time is obtained.
The value was 2, which is an excellent beam quality of about twice the diffraction limit.
【００２２】また、固体レーザ媒質４の形状として、円
盤状の場合について述べたが、直方体や円筒状等、他の
形状でも、熱流の方向と光軸が一致する方向にする構成
を取れば本発明を適用できることは言うまでもない。Although the shape of the solid-state laser medium 4 has been described as a disk shape, other shapes such as a rectangular parallelepiped or a cylinder may be used if a configuration is adopted in which the direction of the heat flow coincides with the optical axis. It goes without saying that the invention can be applied.
【００２３】さらに、上記の実施例では、円盤状固体レ
ーザ媒質４に均一な照射分布を設ける例を示したが、固
体レーザ媒質の光軸の中心部が強くなる緩やかな励起強
度分布を持たせながら一様な励起を行えば、熱歪の発生
を従来方式に比べて低く抑制しながら基本横モードの発
振強度分布に合致する励起分布を実現することが可能で
あり、その場合、さらに高効率な発振を実現できる。こ
のとき中心部から外れた励起の弱い部分の発熱を補償す
るために、固体レーザ媒質４の側面にヒータを配置し、
温度分布を均一化して発振特性に影響する熱歪の発生を
大幅に低減することができる。Further, in the above embodiment, an example is shown in which the disk-shaped solid laser medium 4 is provided with a uniform irradiation distribution. However, it is provided with a gentle excitation intensity distribution in which the central portion of the optical axis of the solid laser medium becomes strong. However, if uniform excitation is performed, it is possible to realize an excitation distribution that matches the oscillation intensity distribution of the fundamental transverse mode while suppressing the generation of thermal strain to a lower level than in the conventional method. Oscillation can be realized. At this time, in order to compensate for heat generation in the weakly excited portion deviated from the central portion, a heater is arranged on the side surface of the solid-state laser medium 4,
By making the temperature distribution uniform, it is possible to greatly reduce the occurrence of thermal strain affecting the oscillation characteristics.
【００２４】上記の本発明の実施例においては、出力偏
光が無偏光の場合を記述したが、偏光性の固体レーザ媒
質を用いたり、共振器内に別の偏光素子を備えて、偏光
発振させてもよい。本発明の特徴の無歪性から、熱歪に
よる複屈折による付加的な共振器損失の発生はなく、無
偏光時と同様な励起入力−出力特性が得られるという利
点がある。固体レーザ媒質４には、Ｎｄ：ＹＡＧ以外の
Ｔｉ：Ａｌ2 Ｏ3 や、Ｎｄ：ＹＬＦ、Ｃｒ：ＬＩＳＡＦ
等、他の固体レーザ媒質を適用できる。その励起体積を
大きく取るために、板状の結晶を側面で融着して、大口
径の固体レーザ媒体として用いることも可能である。そ
の時、偏光発振させる場合などには、発振偏光面が、融
着面と平行になるようにすれば、融着による波面歪の影
響を最小に抑えることができる。In the above embodiment of the present invention, the case where the output polarized light is non-polarized light has been described. However, a polarized solid-state laser medium is used, or another polarization element is provided in the resonator to oscillate the polarized light. You may. Due to the distortionless characteristic of the present invention, there is an advantage that no additional resonator loss occurs due to birefringence due to thermal strain, and the same pump input-output characteristics as in the non-polarized state can be obtained. The solid-state laser medium 4 includes Ti: Al 2 O 3 other than Nd: YAG, Nd: YLF, and Cr: LISAF.
Etc., other solid-state laser media can be applied. In order to increase the excitation volume, a plate-like crystal can be fused on the side surface and used as a large-diameter solid-state laser medium. At this time, in the case of polarization oscillation, the influence of wavefront distortion due to fusion can be minimized by making the oscillation polarization plane parallel to the fusion plane.
【００２５】図４は本発明の第４実施例の固体レーザ装
置の構成を示す図である。円盤状のＮｄ：ＹＡＧ結晶
（直径１．５ｃｍ、厚み０．５ｃｍ）からなる固体レー
ザ媒質４は、片面に誘電体多層膜からなる高反射面２を
持ち、格子状の溝を形成した銅板からなる熱伝達体１３
を介して冷却水を流す銅ブロックからなるシートシンク
３に接合されている。固体レーザ媒質４の他方の面は発
振レーザ光、及び励起光に対してＡＲコートが施されて
いる。レーザ共振器は固体レーザ媒質４と出力鏡９との
間に励起光を透過し、発振光を反射するダイクロイック
ミラー７をおいて構成する。また、半導体レーザから励
起光を出力するファイバ励起源１５のファイバ出射端で
の出射径は２ｍｍ、励起光最大出力は２００Ｗである。
ファイバ励起光源１５からの出射光はレンズ１４、ダイ
クロイックミラー７を通り、固体レーザ媒質４の表面に
直径１．０ｃｍの均一な照射強度分布となるようレンズ
１４によりイメージ転写される。FIG. 4 is a diagram showing the structure of a solid-state laser device according to the fourth embodiment of the present invention. The solid-state laser medium 4 made of a disc-shaped Nd: YAG crystal (1.5 cm in diameter and 0.5 cm in thickness) is made of a copper plate having a highly reflective surface 2 made of a dielectric multilayer film on one side and having lattice-shaped grooves formed thereon. Heat transfer body 13
And a sheet sink 3 made of a copper block through which cooling water flows. The other surface of the solid-state laser medium 4 is provided with an AR coating for the oscillation laser light and the excitation light. The laser resonator comprises a dichroic mirror 7 which transmits excitation light and reflects oscillated light between the solid laser medium 4 and the output mirror 9. The fiber pumping source 15 that outputs pumping light from the semiconductor laser has a diameter of 2 mm at the fiber exit end and a maximum pumping light output of 200 W.
The light emitted from the fiber pumping light source 15 passes through the lens 14 and the dichroic mirror 7, and is image-transferred by the lens 14 onto the surface of the solid-state laser medium 4 so as to have a uniform irradiation intensity distribution with a diameter of 1.0 cm.
【００２６】図６（ａ）に前記熱伝達体１３の片面を示
すように、この熱伝達体１３の直径は励起ビームサイズ
と同じ１ｃｍであり、熱伝達体１３の固体レーザ媒質側
には幅０．１ｍｍ、深さ１．５ｍｍの溝１３ａが格子状
に掘られている。格子のピッチは両方向共１ｍｍであ
る。この構成の熱電熱体１３を用い、レーザ共振器長を
１ｍ、出力鏡９の曲率を凹３ｍ、出力鏡９の透過率を９
０％として、レーザ発振特性を調べた。As shown in FIG. 6A, one side of the heat transfer body 13 has a diameter of 1 cm, which is the same as the excitation beam size, and has a width on the solid laser medium side of the heat transfer body 13. A groove 13a having a depth of 0.1 mm and a depth of 1.5 mm is dug in a lattice shape. The grating pitch is 1 mm in both directions. Using the thermoelectric heating body 13 having this configuration, the laser resonator length is 1 m, the curvature of the output mirror 9 is concave, and the transmittance of the output mirror 9 is 9 m.
The laser oscillation characteristic was examined with 0%.
【００２７】この結果、レーザ出力は最大励起入力時に
基本横モード出力１００Ｗが得られ、長期的な動作試験
でもレーザ発振特性に変化は起こらず実用上十分な耐久
性があることが判った。一方、溝を掘った熱伝達体を省
略し、直接ヒートシンク３と固体レーザ媒質４を接合し
た場合、出力８０Ｗ付近より高次横モードの発振が基本
横モードに加わり、出力９０Ｗで固体レーザ媒質４がヒ
ートシンク３から剥がれる現象が見られた。As a result, the laser output showed a fundamental transverse mode output of 100 W at the maximum excitation input, and it was found that the laser oscillation characteristics did not change even in a long-term operation test, and that the laser had sufficient durability for practical use. On the other hand, when the heat transfer body in which the groove is dug is omitted and the heat sink 3 and the solid-state laser medium 4 are directly joined, the oscillation in the higher-order transverse mode is added to the fundamental transverse mode from about 80 W output, and the solid-state laser medium 4 is output at 90 W output. Was peeled off from the heat sink 3.
【００２８】因に、このように熱伝達体１３に溝１３ａ
が形成されていないと、ヒートシンク３と固体レーザ媒
質４の使用材質の熱膨張率の違いと、接合強度の面内の
不均一性等の理由により局所的な応力の集中が起こり、
特に高励起時に固体レーザ媒質４が破壊されたり撓みを
生じ、ヒートシンク３との接合が部分的に離れるという
問題が生じる。また、固体レーザ媒質４の破壊に至る前
段階では、接合部の応力が固体レーザ媒質内の歪をもた
らし、そのために出射ビームの品質が劣化されることも
ある。Incidentally, the groove 13a is formed in the heat transfer body 13 as described above.
Is not formed, local stress concentration occurs due to the difference in the coefficient of thermal expansion between the materials used for the heat sink 3 and the solid-state laser medium 4 and the in-plane nonuniformity of the bonding strength.
In particular, at the time of high excitation, the solid-state laser medium 4 is broken or bent, and a problem that the bonding with the heat sink 3 is partially separated occurs. Further, at a stage before the solid laser medium 4 is destroyed, the stress at the joint causes distortion in the solid laser medium, which may deteriorate the quality of the emitted beam.
【００２９】この場合、軟らかいインジウム箔等をヒー
トシンクと固体レーザ媒質の間に挟み込むことで応力の
緩和を図ることも考えられるが、この対策では励起と非
励起時の熱膨張差の繰り返しにより徐々に箔が変形され
るため、長期間の動作により冷却性能が劣化したり局所
的な非接触部が生じるなど、実用的なレーザ発振器とし
ての適用は困難となる。また、水銀等の液体金属をヒー
トシンクと固体レーザ媒質との間に閉じ込めることも考
えられるが、液体金属の封じ込めの困難さや材料の毒性
などの問題が生じる。In this case, it is conceivable to relax the stress by sandwiching a soft indium foil or the like between the heat sink and the solid-state laser medium. However, in this measure, the thermal expansion difference between the excitation and the non-excitation is gradually reduced. Since the foil is deformed, it becomes difficult to apply it as a practical laser oscillator, for example, the cooling performance is deteriorated due to long-term operation, or a local non-contact portion is generated. It is also possible to confine liquid metal such as mercury between the heat sink and the solid laser medium, but problems such as difficulty in confining the liquid metal and toxicity of the material occur.
【００３０】また、前記第１ないし第３実施例において
は、固体レーザ媒質４の片面の全面をヒートシンク３に
接合しているが、固体レーザ媒質４の中心軸付近では、
主に熱流は固体レーザ媒質の中心軸に沿ってヒートシン
ク３に熱が流れるのに対し、励起ビームの端部では温度
の低い固体レーザ媒質周辺の非励起部への熱伝導を介し
てのヒートシンク３への熱流束が相対的に大きくなり、
レーザ発振光軸に垂直な面内で温度差が生じ、発振ビー
ムの品質が多少劣化される懸念がある。しかしながら、
この第４実施例では、格子状の溝１３ａにより形成され
るヒダ状の非接触部（空隙）による熱伝達体１３の弾性
変形によって接触部の応力発生を吸収することで、固体
レーザ媒質４の歪発生を防止することが可能となる。In the first to third embodiments, one surface of the solid-state laser medium 4 is entirely bonded to the heat sink 3. However, in the vicinity of the central axis of the solid-state laser medium 4,
The heat flow mainly flows to the heat sink 3 along the central axis of the solid-state laser medium, while the heat-sink 3 at the end of the excitation beam through heat conduction to the non-excitation part around the low-temperature solid-state laser medium. The relative heat flux to
There is a concern that a temperature difference occurs in a plane perpendicular to the laser oscillation optical axis, and the quality of the oscillation beam is somewhat deteriorated. However,
In the fourth embodiment, the stress generation at the contact portion is absorbed by the elastic deformation of the heat transfer body 13 due to the fold-shaped non-contact portion (void) formed by the lattice-shaped grooves 13a, so that the solid-state laser medium 4 of the solid laser medium 4 is absorbed. It is possible to prevent distortion.
【００３１】図５は本発明の第５実施例の構成図であ
る。同図において、基本的な構成は第４実施例と同じで
あるが、ファイバ励起源１５からの励起ビームを固定レ
ーザ媒質４の表面で中心部で強く、周辺になるに従い弱
くなるような励起強度分布を持たせた点、及び、図６
（ｂ）に示すように、熱伝達体１３の溝１３ｂの構造を
同心円状として接触面積率が周辺に行くに従い小さくな
るように、周辺になるに従い溝の幅を大きくしている点
が相違している。FIG. 5 is a block diagram of a fifth embodiment of the present invention. In the figure, the basic configuration is the same as that of the fourth embodiment, except that the excitation beam from the fiber excitation source 15 is strong at the center of the surface of the fixed laser medium 4 and becomes weaker toward the periphery. Point with distribution and FIG. 6
As shown in (b), the structure of the groove 13b of the heat transfer body 13 is concentric and the width of the groove is increased toward the periphery so that the contact area ratio decreases toward the periphery. ing.
【００３２】この構造では、励起ビームの形状と、レー
ザ発振モードのマッチングがよいため、基本横モードの
発振がより容易となり、一層発振効率を高めることがで
きる。この構成において、第１の実施例と同じ共振器構
成を用いて発振特性を調べたところ、最大励起入力２０
０Ｗ時に、基本横モード出力１２０Ｗが得られた。この
ことは、励起分布を励起中心部に集中させる構成を用
い、レーザ発振光軸に対して垂直な面内での温度差の発
生を抑制するよう熱伝達体の熱伝導率を半径方向に周辺
になるに従い小さくなるように変化させた結果、得られ
たと考えられる。経時的な発振特性の変化もないことか
ら、第４実施例と同様に熱伝達体１３と固体レーザ媒質
４の界面の歪も熱伝達体１３の溝１３ｂの弾性変形によ
り吸収されているものと推測される。In this structure, since the shape of the excitation beam and the laser oscillation mode are well matched, the oscillation in the fundamental transverse mode becomes easier and the oscillation efficiency can be further increased. In this structure, when the oscillation characteristics were examined using the same resonator structure as that of the first embodiment, the maximum pumping input 20
At 0 W, a basic transverse mode output of 120 W was obtained. This is achieved by using a configuration in which the excitation distribution is concentrated in the center of the excitation, and the thermal conductivity of the heat transfer body is reduced in the radial direction so as to suppress the occurrence of a temperature difference in a plane perpendicular to the laser oscillation optical axis. It is considered that the result was obtained as a result of being changed so as to become smaller as becomes smaller. Since there is no change in the oscillation characteristics with time, it is assumed that the strain at the interface between the heat transfer body 13 and the solid-state laser medium 4 is also absorbed by the elastic deformation of the groove 13b of the heat transfer body 13 as in the fourth embodiment. Guessed.
【００３３】この第５実施例では、中心軸対称の励起光
の強度分布に応じて溝１３ｂが同心円状に形成されてい
るため、固体レーザ媒質４における熱伝達体１３の接触
面積率（面積当たりの、接触部と非接触部の面積の比）
が半径方向に変化され、これにより中心軸対称の励起光
の強度分布に対応してレーザ発振光軸に垂直な面内で半
径方向に熱伝達率が変化され、固体レーザ媒質４の接触
部の歪発生が防止され。前記した効果が更に助長され
る。In the fifth embodiment, since the grooves 13b are formed concentrically in accordance with the intensity distribution of the excitation light symmetrical about the central axis, the contact area ratio of the heat transfer body 13 in the solid-state laser medium 4 (per area) Of the contact area and the non-contact area)
Is changed in the radial direction, whereby the heat transfer coefficient is changed in the radial direction in a plane perpendicular to the laser oscillation optical axis corresponding to the intensity distribution of the pumping light symmetrical about the central axis, and the contact portion of the solid laser medium 4 is changed. Distortion is prevented. The effects described above are further promoted.
【００３４】この点で、前記第１ないし第３実施例のよ
うに、固体レーザ媒質４にヒートシンク３が全面で接触
していると、励起ビームの強度分布が中心部で強く、半
径の大きな周辺に行くに従い弱くなるような分布をもつ
場合、励起ビームの強度分布を反映してレーザ発振光軸
に垂直な面内で温度差が発生してビーム品質が劣化され
る懸念があるものに比較して優れていると言える。In this respect, when the heat sink 3 is in full contact with the solid-state laser medium 4 as in the first to third embodiments, the intensity distribution of the excitation beam is strong in the central portion and the periphery of the radius is large. If the distribution has a distribution that becomes weaker as it goes to, there is a risk that the beam quality will deteriorate due to a temperature difference in the plane perpendicular to the laser oscillation optical axis that reflects the intensity distribution of the excitation beam. Can be said to be excellent.
【００３５】ここで、熱伝達体の材質に銅の代わりに、
固体レーザ媒質に熱膨張率が近いチタンや、ニッケル鉄
合金等を用いれば、ヒダの深さを一層浅くしても応力の
発生を抑制することができ、製造が容易になり、装置を
安価にできる利点がある。Here, instead of copper for the material of the heat transfer body,
If a solid laser medium is made of titanium, nickel-iron alloy, or the like, which has a close coefficient of thermal expansion, stress generation can be suppressed even if the depth of the fold is made shallower, making it easier to manufacture and lowering the cost of the device. There are advantages that can be done.
【００３６】また、熱伝達体のヒダ構造として溝状の形
状を記述したが、接触面積率が励起強度分布に応じて変
化させるならば、溝の代わりに円形もしくは多角形状の
突起を熱伝達体表面に設けても本発明が有効となること
は言うまでもない。Although the groove shape is described as the fold structure of the heat transfer body, if the contact area ratio is changed in accordance with the excitation intensity distribution, a circular or polygonal projection is used instead of the groove. It goes without saying that the present invention is effective even if it is provided on the surface.
【００３７】[0037]
【発明の効果】本発明によれば、固体レーザ媒質一面を
高反射面として、この高反射面をヒートシンクに接合さ
せ、かつ、固体レーザ媒質の反対側の面から励起光を均
一に照射することで、固体レーザ媒質の光軸に垂直な平
面内での温度分布の発生を抑えることができ、高効率
で、高出力かつ高品質なレーザビームを、低出力から高
出力まで、入出力特性の線形性を保ちながら、ビーム品
質及び、ビーム広がり角の変動のない実用性に優れる固
体レーザ装置を提供することができる。According to the present invention, one surface of the solid-state laser medium is used as a high-reflecting surface, this high-reflecting surface is joined to the heat sink, and the excitation light is uniformly irradiated from the surface opposite to the solid-state laser medium. In this way, it is possible to suppress the occurrence of temperature distribution in a plane perpendicular to the optical axis of the solid-state laser medium, and to output a highly efficient, high-output and high-quality laser beam with low input and output characteristics. It is possible to provide a solid-state laser device that is excellent in practicality without changing the beam quality and the beam divergence angle while maintaining the linearity.
【００３８】また、固体レーザ媒質とヒートシンクとの
間に設けた熱伝達体の接触面に形成した格子状の溝によ
り可能とされる熱伝達体の弾性変形によって、接触部の
応力発生を吸収することで、固体レーザ媒質の歪発生を
防止することが可能となる。さらに、中心軸対称の励起
光の強度分布に応じて熱伝達体の接触面に同心円状の溝
を形成することで、熱伝達体の接触面積率が半径方向に
変化され、レーザ発振光軸に垂直な面内で半径方向に熱
伝達率が変化され、固体レーザ媒質の接触部の歪発生を
防止することができる。The stress generation at the contact portion is absorbed by the elastic deformation of the heat transfer member made possible by the lattice-shaped grooves formed on the contact surface of the heat transfer member provided between the solid-state laser medium and the heat sink. This makes it possible to prevent distortion of the solid-state laser medium. Furthermore, by forming concentric grooves on the contact surface of the heat transfer body according to the intensity distribution of the excitation light symmetrical about the central axis, the contact area ratio of the heat transfer body is changed in the radial direction, and the laser oscillation optical axis is changed. The heat transfer coefficient is changed in the radial direction in the vertical plane, and it is possible to prevent the occurrence of distortion at the contact portion of the solid-state laser medium.
【図１】本発明の第１実施例の正面図である。FIG. 1 is a front view of a first embodiment of the present invention.
【図２】本発明の第２実施例の平面図である。FIG. 2 is a plan view of a second embodiment of the present invention.
【図３】本発明の第３実施例の斜視図である。FIG. 3 is a perspective view of a third embodiment of the present invention.
【図４】本発明の第４実施例の正面図である。FIG. 4 is a front view of a fourth embodiment of the present invention.
【図５】本発明の第５実施例の正面図である。FIG. 5 is a front view of a fifth embodiment of the present invention.
【図６】本発明の第４実施例、第５実施例の各熱伝達体
に形成した溝の形状を示す図である。FIG. 6 is a view showing the shapes of grooves formed in each heat transfer body according to the fourth and fifth embodiments of the present invention.
１ 冷却水パイプ ２ 高反射ミラー ３ ヒートシンク ４ 固体レーザ媒質 ５ 励起光源 ６ 照明光学系 ７ ダイクロイックミラー ８ ビーム拡大器 ９ 出力鏡 １０ 毛細メッシュ網 １１ フィン １２ 反射板 １３ 熱伝達体 １３ａ 格子溝 １３ｂ 同心円溝 １４ レンズ １５ ファイバ励起源 1 Cooling Water Pipe 2 High Reflection Mirror 3 Heat Sink 4 Solid Laser Medium 5 Excitation Light Source 6 Illumination Optical System 7 Dichroic Mirror 8 Beam Expander 9 Output Mirror 10 Capillary Mesh Net 11 Fin 12 Reflector 13 Heat Transfer Element 13a Lattice Groove 13b Concentric Circular Groove 14 lens 15 fiber excitation source
Claims (8)
過面を持つ固体レーザ媒質と、前記固体レーザ媒質を励
起する励起光源と、励起光を前記固体レーザ媒質に導く
光学系と、レーザ共振器を構成する出力鏡からなる固体
レーザ装置において、前記固体レーザ媒質の高反射面側
にヒートシンクを接合し、固体レーザ媒質を光軸に垂直
な面内で一様に励起する照明光学系を設けたことを特徴
とする固体レーザ装置。1. A solid-state laser medium having a high reflection surface and a high transmission surface with respect to a laser oscillation wavelength, an excitation light source for exciting the solid-state laser medium, an optical system for guiding excitation light to the solid-state laser medium, and a laser. In a solid-state laser device comprising an output mirror constituting a resonator, a heat sink is joined to the high-reflection surface side of the solid-state laser medium, and an illumination optical system for uniformly exciting the solid-state laser medium in a plane perpendicular to the optical axis is provided. A solid-state laser device characterized by being provided.
発振モード面積が大きくなるビーム拡大器を備える請求
項１の固体レーザ装置。2. The solid-state laser device according to claim 1, further comprising a beam expander in which the oscillation mode area increases on the solid-state laser medium side in the laser resonator.
項１の固体レーザ装置。3. The solid-state laser device according to claim 1, wherein the output mirror constitutes an unstable resonator.
固体レーザ媒質の高反射面をヒートパイプの内面の一部
とする請求項１の固体レーザ装置。4. A heat pipe type heat sink,
2. The solid-state laser device according to claim 1, wherein the high reflection surface of the solid-state laser medium is a part of an inner surface of the heat pipe.
側にヒータを配置する請求項１の固体レーザ装置。5. The solid-state laser device according to claim 1, wherein a heater is arranged outside the laser oscillation mode of the solid-state laser medium.
に、固体レーザ媒質との接触面積を半径方向に変化させ
る空隙部を多数もつ熱伝達体を備える請求項１の固体レ
ーザ装置。6. The solid-state laser device according to claim 1, further comprising a heat transfer member between the solid-state laser medium and the heat sink, the heat-transfer body having a large number of void portions for changing a contact area with the solid-state laser medium in a radial direction.
様な強度分布となる励起光学系を用い、熱伝達体は前記
所定半径と同じ外径で、固体レーザ媒質との接触面に格
子状の溝を有する請求項６の固体レーザ装置。7. An excitation optical system in which an excitation intensity distribution has a uniform intensity distribution within a predetermined radius, wherein the heat transfer body has the same outer diameter as the predetermined radius and has a contact surface with a solid-state laser medium. 7. The solid-state laser device according to claim 6, comprising a lattice-shaped groove.
に弱くなる強度分布をもつ励起光学系を用い、熱伝達体
は固体レーザ媒質との接触面に半径方向の接触面積率の
分布が励起光強度分布と等しくなる同心円状の溝を有す
る請求項６の固体レーザ装置。8. An excitation optical system having an excitation intensity distribution in which an intensity distribution becomes strong at a center portion and weakens in a radial direction, and a heat transfer body has a distribution of a contact area ratio in a radial direction on a contact surface with a solid-state laser medium. 7. The solid-state laser device according to claim 6, wherein the solid-state laser device has a concentric groove which is equal to the excitation light intensity distribution.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP8460895A JP2658961B2 (en) | 1994-04-21 | 1995-03-17 | Solid-state laser device |
Applications Claiming Priority (3)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP8326694 | 1994-04-21 | ||
| JP6-83266 | 1994-04-21 | ||
| JP8460895A JP2658961B2 (en) | 1994-04-21 | 1995-03-17 | Solid-state laser device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH088477A true JPH088477A (en) | 1996-01-12 |
| JP2658961B2 JP2658961B2 (en) | 1997-09-30 |
Family
ID=26424318
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP8460895A Expired - Fee Related JP2658961B2 (en) | 1994-04-21 | 1995-03-17 | Solid-state laser device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2658961B2 (en) |
Cited By (8)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH114030A (en) * | 1997-06-12 | 1999-01-06 | Nec Corp | Excitation-type solid-state laser device |
| WO2003088435A1 (en) * | 2002-04-18 | 2003-10-23 | Mitsubishi Denki Kabushiki Kaisha | Laser oscillator and optical amplifier |
| JP2004521490A (en) * | 2001-01-22 | 2004-07-15 | ザ・ボーイング・カンパニー | High power side-pumped active mirror solid-state laser |
| JP2005039093A (en) * | 2003-07-16 | 2005-02-10 | Okazaki National Research Institutes | Laser device |
| JP2005354007A (en) * | 2004-06-14 | 2005-12-22 | Ricoh Co Ltd | Solid laser equipment |
| JP2008004752A (en) * | 2006-06-22 | 2008-01-10 | Ricoh Co Ltd | Laser crystal mounting structure |
| JPWO2005091446A1 (en) * | 2004-03-24 | 2008-02-07 | 独立行政法人科学技術振興機構 | Solid state laser equipment |
| WO2018147231A1 (en) * | 2017-02-08 | 2018-08-16 | 浜松ホトニクス株式会社 | Laser medium unit and laser device |
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1995
- 1995-03-17 JP JP8460895A patent/JP2658961B2/en not_active Expired - Fee Related
Cited By (15)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH114030A (en) * | 1997-06-12 | 1999-01-06 | Nec Corp | Excitation-type solid-state laser device |
| JP2004521490A (en) * | 2001-01-22 | 2004-07-15 | ザ・ボーイング・カンパニー | High power side-pumped active mirror solid-state laser |
| WO2003088435A1 (en) * | 2002-04-18 | 2003-10-23 | Mitsubishi Denki Kabushiki Kaisha | Laser oscillator and optical amplifier |
| JPWO2003088435A1 (en) * | 2002-04-18 | 2005-08-25 | 三菱電機株式会社 | Laser oscillator and optical amplifier |
| JP2005039093A (en) * | 2003-07-16 | 2005-02-10 | Okazaki National Research Institutes | Laser device |
| JP4879733B2 (en) * | 2004-03-24 | 2012-02-22 | 独立行政法人科学技術振興機構 | Solid state laser equipment |
| JPWO2005091446A1 (en) * | 2004-03-24 | 2008-02-07 | 独立行政法人科学技術振興機構 | Solid state laser equipment |
| JP2005354007A (en) * | 2004-06-14 | 2005-12-22 | Ricoh Co Ltd | Solid laser equipment |
| JP2008004752A (en) * | 2006-06-22 | 2008-01-10 | Ricoh Co Ltd | Laser crystal mounting structure |
| WO2018147231A1 (en) * | 2017-02-08 | 2018-08-16 | 浜松ホトニクス株式会社 | Laser medium unit and laser device |
| JP2018129391A (en) * | 2017-02-08 | 2018-08-16 | 浜松ホトニクス株式会社 | Laser medium unit and laser device |
| CN110291687A (en) * | 2017-02-08 | 2019-09-27 | 浜松光子学株式会社 | Laser medium unit and laser aid |
| US20190356105A1 (en) | 2017-02-08 | 2019-11-21 | Hamamatsu Photonics K.K. | Laser medium unit and laser device |
| US10862261B2 (en) | 2017-02-08 | 2020-12-08 | Hamamatsu Photonics K.K. | Laser medium unit and laser device |
| CN110291687B (en) * | 2017-02-08 | 2021-06-11 | 浜松光子学株式会社 | Laser medium unit and laser device |
Also Published As
| Publication number | Publication date |
|---|---|
| JP2658961B2 (en) | 1997-09-30 |
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