JPH04343285A - Semiconductor laser device - Google Patents

Semiconductor laser device

Info

Publication number
JPH04343285A
JPH04343285A JP14278091A JP14278091A JPH04343285A JP H04343285 A JPH04343285 A JP H04343285A JP 14278091 A JP14278091 A JP 14278091A JP 14278091 A JP14278091 A JP 14278091A JP H04343285 A JPH04343285 A JP H04343285A
Authority
JP
Japan
Prior art keywords
laser
rays
semiconductor laser
lens
parallel
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
JP14278091A
Other languages
Japanese (ja)
Inventor
Junichi Shimada
純一 嶋田
Osamu Oguchi
大口 脩
Akinori Watabe
昭憲 渡部
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.)
Nippon Telegraph and Telephone Corp
Original Assignee
Nippon Telegraph and Telephone 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 Nippon Telegraph and Telephone Corp filed Critical Nippon Telegraph and Telephone Corp
Priority to JP14278091A priority Critical patent/JPH04343285A/en
Publication of JPH04343285A publication Critical patent/JPH04343285A/en
Pending legal-status Critical Current

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  • Semiconductor Lasers (AREA)

Abstract

PURPOSE:To enable a semiconductor laser device to be lessened in size and weight. CONSTITUTION:Laser rays emitted from a semiconductor laser 1 are made to impinge on a lens 4. The lens 4 is possessed of a curved surface, so that it converts the incident laser rays into convergent rays in parallel with a semiconductor substrate. The lens 4 has a distribution of refractive indexes in the thicknesswise direction, but it has a small aperture, so that it can be focused outside of a laser ray projecting window 3. Therefore, laser rays diverging from the lens 4 are converted into parallel laser rays vertical to the semiconductor substrate once, and then the parallel laser rays are converted into convergent rays through the curvature of the laser projecting window 3 in the direction vertical to the semiconductor substrate. By this setup, as mentioned above, when the projected light rays from a semiconductor laser device are effectively used, the light rays can be outputted as convergent rays or parallel rays without using an additional lens, and thus the device concerned can be lessened in size and weight and enlarged in application for various fields.

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、光産業で用いられる安
価,高性能,高効率な光源である半導体レーザ装置に関
するものである。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a semiconductor laser device which is an inexpensive, high performance, and highly efficient light source used in the optical industry.

【0002】0002

【従来の技術】図4は従来の半導体レーザ装置を説明す
る図である。従来の半導体レーザ装置においては、半導
体レーザの出射ビーム径が数μm以下と非常に小さいた
め、回折によりそのビーム径は数10度の角度で発散す
る。このため、半導体レーザからの出射光を有効に利用
するには、その光を平行光或いは集束光に変換するため
の別個のレンズを必要としている。
2. Description of the Related Art FIG. 4 is a diagram illustrating a conventional semiconductor laser device. In conventional semiconductor laser devices, the diameter of the emitted beam from the semiconductor laser is very small, several micrometers or less, so the beam diameter diverges at an angle of several tens of degrees due to diffraction. Therefore, in order to effectively utilize the light emitted from the semiconductor laser, a separate lens is required to convert the light into parallel light or focused light.

【0003】0003

【発明が解決しようとする課題】従来の半導体レーザ装
置は、他のレンズを用いて半導体レーザからの出射光の
有効利用を図っているため、装置の小型軽量化には不向
きであるという問題があった。したがって本発明は、半
導体レーザからの出射光が数10度の角度で発散すると
いう課題を解決し、平行光或いは集束光を出射できる半
導体レーザを提供することを目的とする。
[Problem to be Solved by the Invention] Conventional semiconductor laser devices use another lens to effectively utilize the light emitted from the semiconductor laser, so there is a problem in that they are not suitable for reducing the size and weight of the device. there were. Therefore, an object of the present invention is to solve the problem that light emitted from a semiconductor laser diverges at an angle of several tens of degrees, and to provide a semiconductor laser that can emit parallel light or focused light.

【0004】0004

【課題を解決するための手段】上述の問題を解決するた
め本発明は、半導体レーザ部を構成する半導体基板上の
レンズ部をその膜厚方向に屈折率分布を持たせるか、ま
たは半導体基板と平行な方向に曲線形状を持たせるよう
にするとともに、容器に取り付けられたレーザ光出射窓
を半導体基板と垂直な方向に屈折率分布を持たせるか、
またはこの方向に曲線形状を持たせるようにしたもので
ある。
[Means for Solving the Problems] In order to solve the above-mentioned problems, the present invention provides a lens section on a semiconductor substrate constituting a semiconductor laser section with a refractive index distribution in the film thickness direction, or In addition to giving it a curved shape in the parallel direction, the laser beam exit window attached to the container should have a refractive index distribution in the direction perpendicular to the semiconductor substrate.
Alternatively, it may have a curved shape in this direction.

【0005】[0005]

【作用】半導体レーザから出射される発散光は、半導体
基板上に設けられた分布屈折率膜からなるレンズと、レ
ーザ光出射窓に設けられたレンズとにより平行光或いは
集束光に変換される。
[Operation] Diverging light emitted from a semiconductor laser is converted into parallel light or convergent light by a lens made of a distributed refractive index film provided on a semiconductor substrate and a lens provided in a laser beam exit window.

【0006】[0006]

【実施例】以下、本発明について図面を参照して説明す
る。図1は、本発明に係る半導体レーザ装置の一実施例
を示す構成図である。この半導体レーザ装置は、集束光
を出射する半導体レーザ装置である。同図において、容
器2に取り付けられた半導体レーザ部1から出射された
レーザ光は、レンズ部4へ入射する。このレンズ部4は
、(b)の上面図に示すように曲線形状を有しており、
これにより発散するレーザ光を半導体レーザ基板と平行
な方向の集束光に変換する。また、このレンズ部4は、
(a)の側面図に示すように、膜厚方向に屈折率分布を
有している。しかし、レンズ部4は、薄膜からなるため
開口が小さく、焦点距離を膜厚の2乗程度にすることは
できない。したがって、レーザ光出射窓3の外側で焦点
を結ばせるためには、このレンズ部4により発散するレ
ーザ光を半導体レーザ基板と垂直な方向に一旦平行光と
して変換する。そして、レンズ部4を通過したレーザ光
はレーザ光出射窓3に入射し、半導体レーザ基板に垂直
な方向の曲率により集束光に変換される。
DESCRIPTION OF THE PREFERRED EMBODIMENTS The present invention will be explained below with reference to the drawings. FIG. 1 is a configuration diagram showing an embodiment of a semiconductor laser device according to the present invention. This semiconductor laser device is a semiconductor laser device that emits focused light. In the figure, laser light emitted from a semiconductor laser section 1 attached to a container 2 enters a lens section 4. This lens portion 4 has a curved shape as shown in the top view of (b),
This converts the diverging laser light into focused light in a direction parallel to the semiconductor laser substrate. Moreover, this lens section 4 is
As shown in the side view of (a), it has a refractive index distribution in the film thickness direction. However, since the lens portion 4 is made of a thin film, the aperture is small, and the focal length cannot be set to about the square of the film thickness. Therefore, in order to focus the laser beam outside the laser beam emission window 3, the laser beam diverging by the lens portion 4 is once converted into parallel light in a direction perpendicular to the semiconductor laser substrate. The laser beam that has passed through the lens section 4 enters the laser beam exit window 3 and is converted into a focused beam by the curvature in the direction perpendicular to the semiconductor laser substrate.

【0007】図2は、本発明の半導体レーザ装置の第2
の実施例を示す構成図であり、半導体レーザ基板に平行
な方向には集束し、垂直な方向には平行なレーザ光を出
射する半導体レーザ装置である。容器2に取り付けられ
た半導体レーザ部1から出射されたレーザ光は、レンズ
部4へ入射する。このレンズ部4は、(b)の上面図に
示すように曲線形状を有しており、これにより発散する
レーザ光を半導体レーザ基板と平行な方向の集束光に変
換する。また、このレンズ部4は、(a)の側面図に示
すように、膜厚方向に屈折率分布を有しており、これに
より発散するレーザ光を半導体レーザ基板と垂直な方向
の集束光に変換する。しかし、レンズ部4は薄膜からな
り、開口が小さく焦点距離が短いため、再び発散光とな
る。 この発散レーザ光はレーザ光出射窓3に入射し、半導体
レーザ基板に垂直な方向の曲率により、より幅の広い平
行光に変換される。
FIG. 2 shows the second structure of the semiconductor laser device of the present invention.
1 is a configuration diagram showing an embodiment of the present invention, which is a semiconductor laser device that emits laser light that is focused in a direction parallel to a semiconductor laser substrate and parallel in a perpendicular direction. Laser light emitted from the semiconductor laser section 1 attached to the container 2 enters the lens section 4 . This lens section 4 has a curved shape as shown in the top view of (b), and thereby converts diverging laser light into focused light in a direction parallel to the semiconductor laser substrate. Further, as shown in the side view of (a), this lens portion 4 has a refractive index distribution in the film thickness direction, thereby converting the diverging laser light into a focused light in the direction perpendicular to the semiconductor laser substrate. Convert. However, since the lens portion 4 is made of a thin film and has a small aperture and a short focal length, the light becomes diverging light again. This diverging laser beam enters the laser beam exit window 3 and is converted into a wider parallel beam due to the curvature in the direction perpendicular to the semiconductor laser substrate.

【0008】図3は、本発明の半導体レーザ装置の第3
の実施例を示す構成図であり、集束光を出射する半導体
レーザ装置である。容器2に取り付けられた半導体レー
ザ部1から出射されたレーザ光は、レンズ部4へ入射す
る。このレンズ部4は、(b)の上面図に示すように、
曲線形状を有しており、これにより発散するレーザ光を
半導体レーザ基板に平行な方向のみ集束光に変換する。 そして、半導体レーザ基板に垂直な方向には機能しない
ため、発散光のままである。このレーザ光は、レーザ光
出射窓3に入射し、半導体レーザ基板の垂直な方向の曲
率により集束光に変換される。
FIG. 3 shows the third structure of the semiconductor laser device of the present invention.
1 is a configuration diagram showing an embodiment of the present invention, which is a semiconductor laser device that emits focused light. Laser light emitted from the semiconductor laser section 1 attached to the container 2 enters the lens section 4 . As shown in the top view of (b), this lens portion 4 is
It has a curved shape, thereby converting diverging laser light into focused light only in the direction parallel to the semiconductor laser substrate. Since the light does not function in the direction perpendicular to the semiconductor laser substrate, it remains a divergent light. This laser light enters the laser light exit window 3 and is converted into a focused light by the vertical curvature of the semiconductor laser substrate.

【0009】なお、以上の実施例においては、レーザ光
出射窓3が分布屈折率レンズ或いは回折レンズであって
も上記と同等の機能を有する。また、半導体レーザ部1
からの出射光が水平方向に十分広くほぼ平行光とみなす
ことができるので、レンズ部4が半導体基板に平行な方
向に曲線形状を有さず、垂直方向の屈折率分布のみを有
し、レーザ光出射窓3で基板に垂直な方向の曲率により
平行光に変換する構成もある。
In the above embodiments, even if the laser beam exit window 3 is a distributed refractive index lens or a diffraction lens, it has the same function as described above. In addition, the semiconductor laser section 1
Since the emitted light from the laser beam is sufficiently wide in the horizontal direction and can be regarded as almost parallel light, the lens portion 4 does not have a curved shape in the direction parallel to the semiconductor substrate and has only a refractive index distribution in the vertical direction. There is also a configuration in which the light is converted into parallel light by the curvature of the light exit window 3 in the direction perpendicular to the substrate.

【0010】0010

【発明の効果】以上説明したように本発明の半導体レー
ザ装置は、その出射光が平行光或いは集束光であるため
、他にレンズを必要とせず、したがって光学装置全体の
大幅な小型軽量化を図ることができる。したがって、半
導体レーザの光センサ,光通信及び光情報処理等への応
用範囲が拡大し産業上の利点が極めて大となる効果を奏
する。
[Effects of the Invention] As explained above, since the semiconductor laser device of the present invention emits parallel light or focused light, it does not require any other lens, and therefore the entire optical device can be significantly reduced in size and weight. can be achieved. Therefore, the scope of application of semiconductor lasers to optical sensors, optical communications, optical information processing, etc. is expanded, and industrial advantages are extremely large.

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

【図1】本発明に係る半導体レーザ装置の一実施例を示
す構成図であり、(a)はその断面図、(b)はその上
面図である。
FIG. 1 is a configuration diagram showing an embodiment of a semiconductor laser device according to the present invention, in which (a) is a cross-sectional view thereof, and (b) is a top view thereof.

【図2】上記半導体レーザ装置の第2の実施例を示す構
成図であり、(a)はその断面図、(b)はその上面図
である。
FIG. 2 is a configuration diagram showing a second embodiment of the semiconductor laser device, in which (a) is a cross-sectional view thereof, and (b) is a top view thereof.

【図3】上記半導体レーザ装置の第3の実施例を示す構
成図であり、(a)はその断面図、(b)はその上面図
である。
FIG. 3 is a configuration diagram showing a third embodiment of the semiconductor laser device, in which (a) is a cross-sectional view thereof, and (b) is a top view thereof.

【図4】従来の半導体レーザ装置の構成図である。FIG. 4 is a configuration diagram of a conventional semiconductor laser device.

【符号の説明】[Explanation of symbols]

1    半導体レーザ部 2    容器 3    レーザ光出射窓 1 Semiconductor laser section 2 Container 3 Laser light exit window

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】  半導体基板と活性層及び該活性層を挟
むクラッド層対からなる半導体レーザ部と、該半導体基
板上に形成された透明薄膜からなるレンズ部と、該半導
体基板を固定しかつ封止する容器と、該容器に取り付け
られたレーザ光出射窓からなる半導体レーザ装置におい
て、前記レンズ部が膜厚方向に屈折率分布を有するかま
たは前記半導体基板と平行な方向に曲線形状を有すると
ともに、前記レーザ光出射窓が半導体基板と垂直な方向
に度を有するようにしたことを特徴とする半導体レーザ
装置。
1. A semiconductor laser section consisting of a semiconductor substrate, an active layer, and a pair of cladding layers sandwiching the active layer, a lens section consisting of a transparent thin film formed on the semiconductor substrate, and a lens section for fixing and sealing the semiconductor substrate. In the semiconductor laser device, the lens portion has a refractive index distribution in a film thickness direction or a curved shape in a direction parallel to the semiconductor substrate. . A semiconductor laser device, wherein the laser beam exit window has a diagonal in a direction perpendicular to the semiconductor substrate.
JP14278091A 1991-05-20 1991-05-20 Semiconductor laser device Pending JPH04343285A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP14278091A JPH04343285A (en) 1991-05-20 1991-05-20 Semiconductor laser device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP14278091A JPH04343285A (en) 1991-05-20 1991-05-20 Semiconductor laser device

Publications (1)

Publication Number Publication Date
JPH04343285A true JPH04343285A (en) 1992-11-30

Family

ID=15323424

Family Applications (1)

Application Number Title Priority Date Filing Date
JP14278091A Pending JPH04343285A (en) 1991-05-20 1991-05-20 Semiconductor laser device

Country Status (1)

Country Link
JP (1) JPH04343285A (en)

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