JPS6025916B2 - solid state laser device - Google Patents
solid state laser deviceInfo
- Publication number
- JPS6025916B2 JPS6025916B2 JP713777A JP713777A JPS6025916B2 JP S6025916 B2 JPS6025916 B2 JP S6025916B2 JP 713777 A JP713777 A JP 713777A JP 713777 A JP713777 A JP 713777A JP S6025916 B2 JPS6025916 B2 JP S6025916B2
- Authority
- JP
- Japan
- Prior art keywords
- optical
- crystal
- laser device
- optical modulator
- face
- 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
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01S—DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
- H01S3/00—Lasers, i.e. devices using stimulated emission of electromagnetic radiation in the infrared, visible or ultraviolet wave range
- H01S3/05—Construction or shape of optical resonators; Accommodation of active medium therein; Shape of active medium
- H01S3/06—Construction or shape of active medium
- H01S3/0627—Construction or shape of active medium the resonator being monolithic, e.g. microlaser
Landscapes
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Engineering & Computer Science (AREA)
- Plasma & Fusion (AREA)
- Optics & Photonics (AREA)
- Lasers (AREA)
Description
【発明の詳細な説明】
この発明は光強度の変調ができるように構成された固体
レーザ装置に関し、特にその4・型化を図ったものであ
る。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a solid-state laser device configured to modulate light intensity, and particularly to a four-type solid-state laser device.
第1図は従来の光変調器を有する固体レーザ装置の構成
を示す概念図で、1は発光ダイオード、2は集光レンズ
、3は光共振器で、レーザ活性物質4の両端面は所定曲
率の球面に形成され、発生するレーザ光を100%反射
する反射膜5と、90〜97%の反射率をもつ反射膜6
とがコーティングされている。FIG. 1 is a conceptual diagram showing the configuration of a conventional solid-state laser device having an optical modulator, in which 1 is a light emitting diode, 2 is a condensing lens, 3 is an optical resonator, and both end faces of a laser active material 4 have a predetermined curvature. A reflective film 5 that is formed on a spherical surface and reflects 100% of the generated laser light, and a reflective film 6 that has a reflectance of 90 to 97%.
is coated with.
7は偏光子、8はLITa03結晶などの電気光学効果
をもつ物質で構成された光変調器、9は検光子で偏光子
7とは偏光方向が直交するように配置されている。Reference numeral 7 denotes a polarizer, 8 an optical modulator made of a material having an electro-optic effect such as LITa03 crystal, and 9 an analyzer, which are arranged so that the polarization direction is orthogonal to the polarizer 7.
このように構成された装置では、レーザ活性物質4は発
光ダイオード1の光で励起されてレーザ光を発生し、レ
ーザ光は反射膜6を通って偏光子7に入り、直線偏光化
させて光変調器8に入り、光変調器8に設けられた電極
に印加される信号電圧に応じて透過する光量が変調され
、検光子9を通って変調されたレーザ光となって射出さ
れる。In the device configured in this way, the laser active material 4 is excited by the light from the light emitting diode 1 to generate laser light, and the laser light passes through the reflective film 6 and enters the polarizer 7, where it is linearly polarized and converted into light. The amount of light entering the modulator 8 and passing therethrough is modulated according to a signal voltage applied to an electrode provided on the optical modulator 8, and is emitted as a modulated laser light through an analyzer 9.
従来のレーザ装置は、光共振器3と偏光子7、光変調器
8および検光子9はそれぞれ個別の素子に形成されてお
り、これらを細立てる際の調整が高精度であることを要
求されるため、精密な支持機構と、精密な調整作業を必
要とした。更に偏光子7および検光子9を必要とするの
で透過損失が大きいという欠点もあった。In conventional laser devices, the optical resonator 3, the polarizer 7, the optical modulator 8, and the analyzer 9 are each formed as separate elements, and the adjustment of these elements is required to be highly accurate. This required a precise support mechanism and precise adjustment work. Furthermore, since a polarizer 7 and an analyzer 9 are required, there is also a drawback that transmission loss is large.
この発明は上記従来のレーザ装置の欠点の解消を目的と
するもので、光共振器3の反射面の形状を平面となし、
かつ光共振器3、光変調器8およびその他構成上必要な
要素を一体に形成し、もって小型化と取扱いの簡便ごと
を実現したものである。The purpose of this invention is to eliminate the drawbacks of the conventional laser device described above, and the shape of the reflecting surface of the optical resonator 3 is made flat,
Furthermore, the optical resonator 3, the optical modulator 8, and other structurally necessary elements are integrally formed, thereby realizing miniaturization and ease of handling.
以下、この発明の一実施例を説明する。An embodiment of this invention will be described below.
第2図はこの発明の一実施例の概略的構成を示す断面図
で、10は平行平板状の集東性光学レンズで、発光ダイ
オード1の光が入射する端面には反射膜5がコーティン
グされ、他方の端面はN肥50,4結晶に平面で当接し
、NdF50,4結晶4の他面には反射膜6がコーティ
ングされて、集東性レンズ10、N研ぐ,4結晶4、反
射膜6が合成樹脂11で一体に固着されて光共振器3を
構成する。FIG. 2 is a sectional view showing a schematic configuration of an embodiment of the present invention, in which reference numeral 10 denotes a parallel plate-like east focusing optical lens, and the end surface on which the light of the light emitting diode 1 enters is coated with a reflective film 5. , the other end face is in plane contact with the NdF50,4 crystal, the other face of the NdF50,4 crystal 4 is coated with a reflective film 6, and the east focusing lens 10, the NdF50,4 crystal 4, and the reflective film are coated. 6 are fixed together with a synthetic resin 11 to form an optical resonator 3.
この光共振器3に更に同軸に光変調器8および検光子9
が合成樹脂12で一体に固着される。このように構成す
ると、集東性レンズ10の作用により、反射膜5,6を
平面状に形成できるため、各横成素子を何れも平面に形
成でき、従って一体に合成樹脂で固着せる構成とするこ
とができるまたレーザ活性物質としてNdP50,4結
晶を用いると、透過したレーザ光はN船50,4結晶の
方位によって特定の方向に偏光する。An optical modulator 8 and an analyzer 9 are further coaxially connected to this optical resonator 3.
are fixed together with synthetic resin 12. With this configuration, the reflective films 5 and 6 can be formed into a flat shape due to the action of the east-focusing lens 10, so each horizontal element can be formed into a flat surface, and therefore, it is possible to have a configuration in which they are integrally fixed with synthetic resin. Furthermore, when NdP50,4 crystal is used as the laser active material, the transmitted laser light is polarized in a specific direction depending on the orientation of the NdP50,4 crystal.
例えばN船50,4のb板を用いると、レーザ光はb板
面内のc軸方向に偏光する。従って光変調器8を形成す
るLITa03結晶のc軸とx軸の両者に45oの角度
をなす方向と、N肥50,4結晶4のb板の面内に含ま
れるc軸方向とを一致させ、さらに検光子9の偏光ベク
トルの方向をNdP50,4結晶のb板の面内に含まれ
るc軸と直交するように検光子9を配置すれば光変調器
8の対向するc面に設けた電極に印放される信号電圧に
より、通過するレーザ光は変調を受けることになり、従
来装置の偏光子7を省略できる。For example, when the b-plate of the N ships 50, 4 is used, the laser beam is polarized in the c-axis direction within the plane of the b-plate. Therefore, the direction that forms an angle of 45° to both the c-axis and the x-axis of the LITa03 crystal forming the optical modulator 8 and the c-axis direction included in the plane of the b-plate of the N-50,4 crystal 4 are made to match. Furthermore, if the analyzer 9 is arranged so that the direction of the polarization vector of the analyzer 9 is orthogonal to the c-axis included in the plane of the b-plate of the NdP50. The passing laser light is modulated by the signal voltage applied to the electrodes, and the polarizer 7 of the conventional device can be omitted.
なお、上記の実施例では反射膜6をN肥50,4結晶4
の出射面にコーティングした例を示したが、光変調器8
の端面にコーティングする構成、または厚さ100〃m
程度の光学研磨した石英板にコーティングしたものを介
挿せる構成としてもよい。In the above embodiment, the reflective film 6 is made of N fertilizer 50,4 crystal 4.
An example in which the output surface of the optical modulator 8 is coated is shown.
Structure of coating on the end face of or 100 m thick
A structure may also be adopted in which a coated quartz plate that has been optically polished to a certain degree can be inserted.
また光変調器8にはSro.258も.75Nb206
結晶を適用しうろことはいうまでもない。この発明は集
東性レンズ10を適用することにより装置を構成する各
秦の接合面を全て平面に形成することができるので、適
当な屈折率をもつ合成樹脂により、光共振器と光変調器
を含む全素子を一体に構成することができ、更に光共振
器を構成するレーザ活性物質にN肥50,4結晶を適用
することにより、その出力レーザ光が一定の偏光を持た
せることができるので、従釆装置で必要とした偏光素子
を1個省略でき、透過損失を軽減できる。Further, the optical modulator 8 has Sro. 258 too. 75Nb206
Needless to say, the crystals are applied to the scales. In this invention, by applying the east-focusing lens 10, all of the joint surfaces of the respective parts constituting the device can be formed into flat surfaces, so that the optical resonator and the optical modulator can be All elements including the laser beam can be constructed as one, and by applying N-50,4 crystal to the laser active material that constitutes the optical resonator, the output laser light can be made to have a certain polarization. Therefore, one polarizing element required in the secondary device can be omitted, and transmission loss can be reduced.
またこの発明に係る装置の光共振器は、直接結晶側から
光をとり出す構成となっているので、いわゆる半球面系
共振器となっており、小さなビーム拡がり角をもつコヒ
ーレントな光を得る事ができ、光フアィバのように小面
積の伝搬系への結合を極めて高い結合効率で実現できる
という利点をも有するものである。図面の簡単な説明.
第1図は従来の光変調器を有する固体レーザ装置の概略
構成図、第2図はこの発明の一実施例の構成と示す概略
断面図である。Furthermore, the optical resonator of the device according to the present invention is configured to take out light directly from the crystal side, so it is a so-called hemispherical resonator, and it is possible to obtain coherent light with a small beam divergence angle. It also has the advantage that it can be coupled to a small-area propagation system like an optical fiber with extremely high coupling efficiency. A brief explanation of the drawing. FIG. 1 is a schematic configuration diagram of a solid-state laser device having a conventional optical modulator, and FIG. 2 is a schematic sectional view showing the configuration of an embodiment of the present invention.
図において1は発光素子、2はしンズ、3は光共振器、
5,6は反射膜、7は偏光子、8は光変調器、9は検光
子、11,12は合成樹脂である。In the figure, 1 is a light emitting element, 2 is a lens, 3 is an optical resonator,
5 and 6 are reflective films, 7 is a polarizer, 8 is a light modulator, 9 is an analyzer, and 11 and 12 are synthetic resins.
なお、図中同一符号はそれぞれ同一または相当部分を示
す。第1図
第2図Note that the same reference numerals in the figures indicate the same or corresponding parts. Figure 1 Figure 2
Claims (1)
レンズの一方の端面に面接するNdP_5O_1_4結
晶と、この外端面および上記集束性光学レンズの外端面
にそれぞれ面接し、それぞれ励起されるレーザ光に対し
て所定の反射率をもつ二つの反射膜とで構成される光共
振器、この光共振器の上記NdP_5O_1_4結晶と
上記一方の反射膜を介して面接する光変調器およびこの
光変調器の他面に面接し、上記光共振器から射出される
レーザ光の偏光方向に対して所定角度の偏光角をもつよ
うに配設された検光子を備え、上記光共振器、光変調器
および偏光子を所定の屈折率をもつ合成樹脂で一体に固
着してなる固定レーザ装置。 2 一方の反射膜がNdP_5O_1_4結晶との外面
にコーテイングされている特許請求の範囲第1項記載の
固体レーザ装置。 3 一方の反射膜が光変調器のレーザ光入射側端面にコ
ーテイングされている特許請求の範囲第1項記載の固体
レーザ装置。 4 光学平面研磨した石英薄板の一面に反射膜をコーテ
イングし、この石英薄板をNdP_5O_1_4結晶と
光変調器との間に介挿せることを特徴とする特許請求の
範囲第1項記載の固体レーザ装置。[Scope of Claims] 1. A converging optical lens whose both ends are flat, an NdP_5O_1_4 crystal which faces one end face of this lens, and which faces each of this outer end face and an outer end face of the above-mentioned convergent optical lens, an optical resonator composed of two reflective films each having a predetermined reflectance with respect to excited laser light, and an optical modulator that interfaces with the NdP_5O_1_4 crystal of this optical resonator via one of the reflective films. and an analyzer facing the other surface of the optical modulator and disposed so as to have a polarization angle of a predetermined angle with respect to the polarization direction of the laser beam emitted from the optical resonator, , a fixed laser device in which an optical modulator and a polarizer are fixed together with a synthetic resin having a predetermined refractive index. 2. The solid-state laser device according to claim 1, wherein one of the reflective films is coated on the outer surface of the NdP_5O_1_4 crystal. 3. The solid-state laser device according to claim 1, wherein one of the reflective films is coated on the laser beam incident side end face of the optical modulator. 4. The solid-state laser device according to claim 1, characterized in that a reflective film is coated on one surface of a thin quartz plate which has been optically polished, and the thin quartz plate can be inserted between the NdP_5O_1_4 crystal and the optical modulator.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP713777A JPS6025916B2 (en) | 1977-01-24 | 1977-01-24 | solid state laser device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP713777A JPS6025916B2 (en) | 1977-01-24 | 1977-01-24 | solid state laser device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5392690A JPS5392690A (en) | 1978-08-14 |
| JPS6025916B2 true JPS6025916B2 (en) | 1985-06-20 |
Family
ID=11657680
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP713777A Expired JPS6025916B2 (en) | 1977-01-24 | 1977-01-24 | solid state laser device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6025916B2 (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH033378A (en) * | 1989-05-31 | 1991-01-09 | Matsushita Electric Ind Co Ltd | solid state laser device |
| JP2670637B2 (en) * | 1990-06-25 | 1997-10-29 | 富士写真フイルム株式会社 | Laser diode pumped solid state laser |
| JP2981671B2 (en) * | 1990-05-10 | 1999-11-22 | 富士写真フイルム株式会社 | Laser diode pumped solid state laser |
-
1977
- 1977-01-24 JP JP713777A patent/JPS6025916B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5392690A (en) | 1978-08-14 |
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