JPS6026319B2 - solid state laser device - Google Patents
solid state laser deviceInfo
- Publication number
- JPS6026319B2 JPS6026319B2 JP2906277A JP2906277A JPS6026319B2 JP S6026319 B2 JPS6026319 B2 JP S6026319B2 JP 2906277 A JP2906277 A JP 2906277A JP 2906277 A JP2906277 A JP 2906277A JP S6026319 B2 JPS6026319 B2 JP S6026319B2
- Authority
- JP
- Japan
- Prior art keywords
- laser
- reflective film
- face
- modulator
- coated
- 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
- H01S5/00—Semiconductor lasers
- H01S5/10—Construction or shape of the optical resonator, e.g. extended or external cavity, coupled cavities, bent-guide, varying width, thickness or composition of the active region
- H01S5/1028—Coupling to elements in the cavity, e.g. coupling to waveguides adjacent the active region, e.g. forward coupled [DFC] structures
Landscapes
- Physics & Mathematics (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- General Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Optics & Photonics (AREA)
- Lasers (AREA)
Description
【発明の詳細な説明】
この発明は、拡がり角の小さなコヒーレント・レーザー
光を放射し同時に光強度の変調ができる小型の固体レー
ザー装置に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a compact solid-state laser device that can emit coherent laser light with a small divergence angle and simultaneously modulate the light intensity.
最近、光通信の重要性が急速に増しているが、中でも光
源は最も重要な構成要素である。従来の小型固体レーザ
ーおよび変調器の装置としては、第1図に示すものがあ
った。Recently, the importance of optical communications has been rapidly increasing, and the light source is the most important component. A conventional compact solid-state laser and modulator device is shown in FIG.
第1図において、1はしーザー発振部、D‘ま変調部を
示しており、レーザー活性煤質1は、発光ダイオード2
で発生して集光レンズ3を通った光によって励起される
。レーザー活性煤質1の両端はある曲率をもった球面に
なっており、こ)に反射膜4,5がコーティングしてあ
る。この両端の反射膜4,5によって光共振器が構成さ
れ、この内部で増幅作用が行われ、レーザー光が図中の
レーザー活性煤質1の右方に放射される。放射さた光は
偏光子6を通り、直線偏向化され、電気光学効果をもつ
結晶で作られた変調器7に入り、次いで検光子8に入る
。そして、偏光子6と検光子8の偏向方向は直交するよ
うに配置されている。検光子8を出た光は変調器7に加
えられる電圧により変調された光信号となる。従釆の固
体レーザーおよび変調器装置は、以上のように構成され
ているので、レーザー発振部1と変調部0が個々に分れ
て構成されており、それぞれの光学的調整が微妙で難し
い。In FIG. 1, 1 indicates a laser oscillation section and a D'ma modulation section, and a laser active soot substance 1 is a light emitting diode 2.
It is excited by the light that is generated and passed through the condenser lens 3. Both ends of the laser active soot material 1 are spherical surfaces with a certain curvature, and are coated with reflective films 4 and 5. The reflective films 4 and 5 at both ends constitute an optical resonator, and amplification is performed inside the resonator, and laser light is emitted to the right of the laser-activated soot material 1 in the figure. The emitted light passes through a polarizer 6, is linearly polarized, enters a modulator 7 made of a crystal with an electro-optic effect, and then enters an analyzer 8. The polarizer 6 and the analyzer 8 are arranged so that their polarization directions are perpendicular to each other. The light exiting the analyzer 8 becomes an optical signal modulated by the voltage applied to the modulator 7. Since the subordinate solid-state laser and modulator device are constructed as described above, the laser oscillation section 1 and the modulation section 0 are constructed separately, and optical adjustment of each is delicate and difficult.
またレーザー活性媒質1の端面は、曲率をもった球面に
なっているので、平板上の偏光子6との一体化は困難で
ある等々の欠点があった。この発明は、上記のような従
来の欠点を除去するためになされたもので、両端が平行
平面状の固体レーザーに、同じく平行平端面を持つ偏光
子、変調器および検光子を接着し、全体を一体化し、変
調されたコヒーレント・レーザー光を放射する装置を提
供することを目的とするものである。Furthermore, since the end face of the laser active medium 1 is a spherical surface with curvature, it is difficult to integrate it with the polarizer 6 on a flat plate. This invention was made in order to eliminate the above-mentioned drawbacks of the conventional technology.A polarizer, a modulator, and an analyzer, which also have parallel flat end surfaces, are bonded to a solid-state laser whose ends are parallel flat, and the entire The object of the present invention is to provide a device that integrates the above and emits modulated coherent laser light.
以下この発明について説明する。第2図はこの発明の一
実施例を示すもので、1′は両端が平行平面状のレーザ
ー活性媒質、9は平行変板状の集東性光学レンズでその
片側端面にはしーザー光波長の光に対して100%の反
射率を持つ反射膜4′がコーティングしてある。This invention will be explained below. Fig. 2 shows an embodiment of the present invention, in which 1' is a laser active medium whose both ends are parallel planes, 9 is a parallel plate-shaped east-focusing optical lens, and one end face has a laser beam wavelength. It is coated with a reflective film 4' that has a reflectance of 100% for the light.
一方、レーザー猪性媒質1′の一方の端面にもし−ザー
発振波長の光に対して90〜99.7%の反射率を持つ
反射膜5′がコーティングされている。6′は平板状の
偏光子、7′は電気光学効果を持つ結晶からなる変調器
であり、8′は平板状の検光子である。10,11はそ
れぞれ集光性光学レンズ9と変調器7′を支持するプラ
スチックであり、その他は第1図と同じものである。上
記の各部分は相互の屈折率になるべく近い屈折率の値を
持つ接着剤で接着する。次に動作について説明する。On the other hand, one end face of the laser medium 1' is coated with a reflective film 5' having a reflectance of 90 to 99.7% for light at the laser oscillation wavelength. 6' is a flat polarizer, 7' is a modulator made of a crystal having an electro-optic effect, and 8' is a flat analyzer. Reference numerals 10 and 11 are plastics supporting the condensing optical lens 9 and the modulator 7', respectively, and the rest is the same as in FIG. Each of the above parts is bonded with an adhesive having a refractive index value as close as possible to the refractive index of each other. Next, the operation will be explained.
集光レンズ3によって発光ダィオ−ド2の光は集光性光
学レンズ9を通り、レーザー活性煤質1′に集光され、
これを励起する。反射膜4′および5′によってレーザ
ー共振器が構成され、レーザー光は反射膜5′の部分透
過性により反射膜5′を透過し、偏光板6′に入る。偏
光板6′を出た光を偏光し変調器7′に入る。この時の
偏光の方向は変調器7′の電極がついている結晶方位お
よびそれと直交する結晶方位の双方に対して45oの角
度をなすようにする。変調器7′に加えられる電圧によ
って変調器7′を出る光の偏光方はもとの偏光ベクトル
と異なる。従って検光子8′の偏光ベクトルの方向を偏
光板6′の偏光ベクトルと直交するようにしておくと、
光は電圧により振動変調を受けることになる。以上説明
したように、この発明によれば各部の構成要素はすべて
平行平板状であり、それぞれを適当な屈折率をもつ接着
剤で接合することにより、レーザー発振部と変調部が一
体化され、全体が4・型でかつそれぞれの構成要素間の
微妙な光学的調整を不要にすることができる。The light from the light emitting diode 2 passes through the condensing optical lens 9 and is condensed onto the laser active soot material 1' by the condensing lens 3.
Excite this. The reflective films 4' and 5' constitute a laser resonator, and the laser beam passes through the reflective film 5' due to the partial transparency of the reflective film 5' and enters the polarizing plate 6'. The light exiting the polarizing plate 6' is polarized and enters the modulator 7'. The direction of polarization at this time is set to form an angle of 45° with respect to both the crystal orientation in which the electrodes of the modulator 7' are attached and the crystal orientation perpendicular thereto. The voltage applied to the modulator 7' causes the polarization of the light leaving the modulator 7' to be different from the original polarization vector. Therefore, if the direction of the polarization vector of the analyzer 8' is set perpendicular to the polarization vector of the polarizing plate 6',
The light will undergo vibrational modulation due to the voltage. As explained above, according to the present invention, the components of each part are all parallel plate shapes, and by bonding each part with an adhesive having an appropriate refractive index, the laser oscillation part and the modulation part are integrated. The entire structure is a 4-inch type, and delicate optical adjustment between each component can be eliminated.
またレーザー共振器はいわゆる半球面系共振器となって
いるので、この発明のよう結晶側から光を取り出す方式
による方がより小さなビーム拡がり角をもつコヒーレン
トな光を得ることができる。このことは光フアィバへの
結合においてきわめて高い結合効率を期待できる。Furthermore, since the laser resonator is a so-called hemispherical resonator, coherent light with a smaller beam divergence angle can be obtained by using the method of the present invention in which light is extracted from the crystal side. This means that extremely high coupling efficiency can be expected in coupling to optical fibers.
第1図は従来の固体レーザー装置の一例を示す構成略図
、第2図はこの発明の一実施例を示す構成略図である。
図中、1′はしーザー活性煤質、2は発光ダイオード、
3は集光レンズ、4′,5′は反射膜、6′は偏光板、
7′は変調器、8′は検出板、9は平行端面を持つ集光
性光学レンズである。なお、図中の同一符号は同一また
は相当部分を示す。第1図籍2図FIG. 1 is a schematic structural diagram showing an example of a conventional solid-state laser device, and FIG. 2 is a schematic structural diagram showing an embodiment of the present invention. In the figure, 1' is Caesar active soot, 2 is a light emitting diode,
3 is a condenser lens, 4' and 5' are reflective films, 6' is a polarizing plate,
7' is a modulator, 8' is a detection plate, and 9 is a condensing optical lens with parallel end surfaces. Note that the same reference numerals in the figures indicate the same or corresponding parts. Figure 1, Figure 2
Claims (1)
の集束性光学レンズの他方の端面に、一方の端面に反射
膜をコーテイングしたレーザー活性媒質の他方の端面を
接着し、前記レーザー活性媒質の反射膜に偏光板、電気
光学効果を有する結晶からなる変調器および検光板を順
次互いに接着し一体化したことを特徴とする固体レーザ
ー装置。 2 集光性光学レンズの一方の端面にコーテイングされ
た反射膜のレーザー発振波長における反射率を100%
とし、レーザー活性媒質の一方の端面にコーテイングさ
れれた反射膜の反射率を90〜99.7%にして変調器
側からレーザー光を取り出す特許請求の範囲第1項記載
の固体レーザー装置。[Scope of Claims] 1. The other end face of a laser active medium whose one end face is coated with a reflective film is adhered to the other end face of a parallel plate-shaped focusing optical lens whose one end face is coated with a reflective film, A solid-state laser device characterized in that a polarizing plate, a modulator made of a crystal having an electro-optic effect, and an analyzer plate are successively adhered to each other and integrated with the reflective film of the laser active medium. 2. The reflectance at the laser oscillation wavelength of the reflective film coated on one end surface of the condensing optical lens is 100%.
2. The solid-state laser device according to claim 1, wherein the laser beam is extracted from the modulator side by setting the reflectance of a reflective film coated on one end face of the laser active medium to 90 to 99.7%.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2906277A JPS6026319B2 (en) | 1977-03-15 | 1977-03-15 | solid state laser device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2906277A JPS6026319B2 (en) | 1977-03-15 | 1977-03-15 | solid state laser device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS53113495A JPS53113495A (en) | 1978-10-03 |
| JPS6026319B2 true JPS6026319B2 (en) | 1985-06-22 |
Family
ID=12265869
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP2906277A Expired JPS6026319B2 (en) | 1977-03-15 | 1977-03-15 | solid state laser device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6026319B2 (en) |
-
1977
- 1977-03-15 JP JP2906277A patent/JPS6026319B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS53113495A (en) | 1978-10-03 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| US7841746B2 (en) | Light source device, lighting device, projector, and monitoring device | |
| US5007694A (en) | Light wavelength converter | |
| JPH09197457A (en) | Light generating device and manufacturing method thereof | |
| JPH03150509A (en) | Method for connecting between waveguide substrate and optical fiber, and reflection preventive film with ultraviolet-ray cutting-off function used for the method | |
| JPS6026319B2 (en) | solid state laser device | |
| JPS63316082A (en) | optical device | |
| JPS62141653A (en) | Light pickup | |
| JPH06250130A (en) | Optical isolator | |
| JPH06331314A (en) | Method and apparatus for measuring displacement | |
| JP4111076B2 (en) | Wavelength conversion laser device | |
| JPS6025916B2 (en) | solid state laser device | |
| JPH1098222A (en) | Wavelength conversion solid-state laser | |
| JPH03179328A (en) | Light wavelength converting method | |
| JP2003043435A (en) | Optical frequency comb generator | |
| JP2000114633A (en) | Wavelength conversion solid-state laser device | |
| JPH09293921A (en) | Semiconductor laser pumped solid-state laser device | |
| JP2536931B2 (en) | Spatial light modulator | |
| JPH04158588A (en) | Semiconductor laser exciting solid laser device | |
| JP2759115B2 (en) | Measurement device for third-order nonlinear optical characteristics | |
| JP2948645B2 (en) | Two-wavelength light source element | |
| JPH09161298A (en) | Optical recording master mastering apparatus and method | |
| KR100355387B1 (en) | Acousto-optic modulating system | |
| JPH05235456A (en) | Laser equipment | |
| JPH09293920A (en) | Solid state laser device stimulated by semiconductor laser and photo detector | |
| JPH0464134B2 (en) |