JPH11218649A - Optical coupling device with beam shaping function and laser diode module - Google Patents

Optical coupling device with beam shaping function and laser diode module

Info

Publication number
JPH11218649A
JPH11218649A JP2064198A JP2064198A JPH11218649A JP H11218649 A JPH11218649 A JP H11218649A JP 2064198 A JP2064198 A JP 2064198A JP 2064198 A JP2064198 A JP 2064198A JP H11218649 A JPH11218649 A JP H11218649A
Authority
JP
Japan
Prior art keywords
laser diode
lens
end surface
cross
light
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.)
Withdrawn
Application number
JP2064198A
Other languages
Japanese (ja)
Inventor
Hideyuki Kuwano
英之 桑野
Naomi Negishi
直美 根岸
Minoru Fujita
実 藤田
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.)
Hitachi Ltd
Original Assignee
Hitachi 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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP2064198A priority Critical patent/JPH11218649A/en
Publication of JPH11218649A publication Critical patent/JPH11218649A/en
Withdrawn legal-status Critical Current

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  • Semiconductor Lasers (AREA)
  • Optical Couplings Of Light Guides (AREA)

Abstract

PROBLEM TO BE SOLVED: To provide an optical coupling device which has both a light converging function and a beam shaping function and eliminates the need to adjust the assembly position of a lens and is superior in long-period stability by providing a concave cylindrical surface on one end surface of a converging rod lens and a convex cylindrical surface which operates coaxially with the above concave cylindrical surface on the other end surface. SOLUTION: The incidence end surface 2 of the converging rod lens is formed into the concave cylindrical curved surface which operates at right angles to the major axis of the elliptic cross section of an incident beam 4 and the output end surface 3 is formed into the convex cylindrical curved surface which operates axially. The radii of curvature of the concave and convex surfaces are so set that the beam waist positions of the major and minor axes of the beam cross section meet each other and the sectional shape at the beam waist position is circular. Consequently, an incident elliptic parallel beam 4 has the same beam waist position as to the major and minor axes and is optically coupled with a single-mode optical fiber 6 with high efficiency.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は、出射発散光の断面
形状が楕円又は長円状であるレーザダイオードを搭載し
た光通信用レーザダイオードモジュール及びその光学系
に係わり、特に、楕円又は長円状のビーム断面をほぼ円
形に整形するビーム整形機能を有する光学系に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a laser diode module for optical communication on which a laser diode having a cross-sectional shape of emitted divergent light is elliptical or elliptical, and an optical system thereof. The present invention relates to an optical system having a beam shaping function of shaping a beam section into a substantially circular shape.

【0002】[0002]

【従来の技術】レーザダイオードからの出力光を効率良
く光ファイバに結合させるためには、レーザダイオード
からの出射発散光をレンズなどの光学系によって集束さ
せ、この集束光のビームウエストにおける断面形状を光
ファイバのモードフィールド径と同じ寸法及び円形状に
することが重要である。
2. Description of the Related Art In order to efficiently couple output light from a laser diode to an optical fiber, divergent light emitted from the laser diode is focused by an optical system such as a lens, and the sectional shape of the focused light at the beam waist is adjusted. It is important to have the same size and circular shape as the mode field diameter of the optical fiber.

【0003】球レンズや集束形ロッドレンズなどの中心
軸対象なレンズを使用した場合、出射発散光の断面形状
が楕円又は長円状であるレーザダイオードの出力光を光
ファイバのモードフィールド径とほぼ同じ寸法に集束さ
せても、この集束光のビームウエストにおける断面形状
は円又は長円状のままであり、この形状の差が結合損失
を増大させる。この結合損失を低減するためには、ビー
ム断面形状を円形に整形する機能を有する光学系が必要
である。
When a lens having a center axis symmetrical, such as a spherical lens or a converging rod lens, is used, the output light of a laser diode having an elliptical or elliptical cross section of emitted divergent light is approximately equal to the mode field diameter of the optical fiber. Even when the beams are focused to the same size, the cross-sectional shape of the focused light at the beam waist remains a circle or an ellipse, and the difference between the shapes increases the coupling loss. In order to reduce the coupling loss, an optical system having a function of shaping the beam cross section into a circle is required.

【0004】従来のビーム整形機能付集束レンズの技術
として、2個のシリンドリカルレンズを対向配置し軸心
が直交するように結合せしめることにより、扁平な入射
光をほぼ円形の出射光に集束し光ファイバのコア形状と
一致させることにより高結合効率を得た例がある(特開
昭57−176014号公報)。
[0004] As a conventional focusing lens with a beam shaping function, two cylindrical lenses are arranged to face each other and are coupled so that their axes are orthogonal to each other. There is an example in which high coupling efficiency is obtained by matching the shape of the fiber core (Japanese Patent Laid-Open No. 57-176014).

【0005】[0005]

【発明が解決しようとする課題】上記の従来例では、2
個の対向配置したシリンドリカルレンズを軸心が直交す
るように配置させるため、組立位置調整が必要である。
また、2個のシリンドリカルレンズを透明な接着剤で接
着固定しているため、固定に要する時間が必要となり、
接着固定部が光学系の長期安定性に悪影響を与える。
In the above conventional example, two
In order to arrange the opposed cylindrical lenses so that their axes are orthogonal to each other, it is necessary to adjust the assembling position.
In addition, since the two cylindrical lenses are bonded and fixed with a transparent adhesive, time required for fixing is required,
The adhesive fixing portion adversely affects the long-term stability of the optical system.

【0006】本発明の目的は、上記従来の課題を解決す
るものであり、出射発散光の断面形状が楕円又は長円状
であるレーザダイオードを使用した場合、集光機能とビ
ーム整形機能の両方を合わせ持ち、かつレンズの組立位
置調整が不要で長期安定性に優れた光結合装置を提供す
ることにある。
SUMMARY OF THE INVENTION An object of the present invention is to solve the above-mentioned conventional problems. When a laser diode having an elliptical or elliptical cross-sectional shape of emitted divergent light is used, both a light condensing function and a beam shaping function are provided. It is an object of the present invention to provide an optical coupling device having excellent long-term stability without having to adjust the lens assembly position.

【0007】[0007]

【課題を解決するための手段】本発明による光結合装置
は、入射ビームを高効率でシングルモード光ファイバに
結合するものである。入射ビームの楕円状断面の長軸の
ビームウエスト位置におけるスポットサイズがシングル
モード光ファイバのモードフィールド径と一致するよう
な焦点距離を有する集束形ロッドレンズについて、レン
ズの入射端面を前記入射ビームの楕円状断面の長軸と直
交する軸に作用する凹シリンドリカル形状の曲面とし、
出力端面を入射端面と同じ方向の軸に作用する凸シリン
ドリカル形状の曲面としている。凹面、凸面それぞれの
曲率半径は、ビーム断面の長軸と短軸のビームウエスト
位置が一致し、かつビームウエスト位置におけるビーム
断面形状が円形となるように設定している。
SUMMARY OF THE INVENTION An optical coupling device according to the present invention couples an incident beam to a single mode optical fiber with high efficiency. For a focusing rod lens having a focal length such that the spot size at the beam waist position of the major axis of the elliptical cross section of the incident beam coincides with the mode field diameter of the single mode optical fiber, the incident end face of the lens is changed to the elliptical shape of the incident beam. With a concave cylindrical shape acting on an axis perpendicular to the long axis of the cross section,
The output end surface is a convex cylindrical curved surface acting on an axis in the same direction as the incident end surface. The radius of curvature of each of the concave surface and the convex surface is set such that the beam waist positions of the major axis and the minor axis of the beam cross section match, and the beam cross section at the beam waist position is circular.

【0008】即ち、上記手段によれば、レンズの入射端
面を入射ビームの楕円状断面の長軸と直交した軸に作用
する凹シリンドリカル面とすることにより長軸と直交し
た方向のみ入射角度が拡散側に増したように作用し、そ
の結果出力端面におけるビーム断面の長軸と短軸が同じ
寸法になる。また、出力端面を前記凹シリンドリカル面
と同じ軸に作用する凸シリンドリカル面とすることによ
り、出力端面通過後の長軸と直交した軸の集束角度を矯
正し長軸方向と一致させるように作用する。集束角度を
矯正することはビームウエスト位置及びビームウエスト
におけるビーム断面寸法を矯正することと等価である。
これらのように、1個のレンズに集束機能とビーム整形
機能の両方を備えている。さらに、レンズを一体整形し
固定部を無くしたことにより組立位置調整が不要とし、
長期安定性に対する影響を排除している。
That is, according to the above means, the incident end surface of the lens is a concave cylindrical surface acting on the axis perpendicular to the major axis of the elliptical cross section of the incident beam, so that the incident angle is diffused only in the direction perpendicular to the major axis. Acts as if it were increased on the side, so that the major and minor axes of the beam cross section at the output end face have the same dimensions. Further, by making the output end face a convex cylindrical face acting on the same axis as the concave cylindrical face, it acts so as to correct the convergence angle of the axis orthogonal to the long axis after passing through the output end face so as to match with the long axis direction. . Correcting the convergence angle is equivalent to correcting the beam waist position and the beam cross-sectional dimension at the beam waist.
As described above, one lens has both the focusing function and the beam shaping function. In addition, since the lens is integrally shaped and the fixed part is eliminated, adjustment of the assembly position is unnecessary,
Excludes effects on long-term stability.

【0009】[0009]

【発明の実施の形態】本発明の実施例の上面図を図1
(a)、側面図を図1(b)に示す。レンズ本体1は屈
折率分布形集束ロッドレンズであり、波長980nmに
おける中心軸上屈折率は1.595、屈折率分布定数は
0.333、レンズ長は3.573mmである。光の入
射端面2を凹シリンドリカル形状とし、出力端面3を凸
シリンドリカル形状としている。曲面方向は入射端面2
と出力端面3が同一軸に作用するよう配置されており、
曲率半径はそれぞれ0.695mm,1.253mmで
ある。点線はビーム4の軌跡を示す。入射端面2に波長
980nm、断面形状が縦長の楕円で長軸径0.490
mm、短軸径0.152mmの平行ビームを入射させ
る。
FIG. 1 is a top view of an embodiment of the present invention.
(A) and a side view is shown in FIG. 1 (b). The lens body 1 is a refractive index distribution type focusing rod lens, and has a central axis refractive index of 1.595, a refractive index distribution constant of 0.333, and a lens length of 3.573 mm at a wavelength of 980 nm. The light incident end face 2 has a concave cylindrical shape, and the output end face 3 has a convex cylindrical shape. Curved surface direction is incident end face 2
And the output end face 3 are arranged to act on the same axis,
The radii of curvature are 0.695 mm and 1.253 mm, respectively. The dotted line indicates the locus of the beam 4. The incidence end face 2 has a wavelength of 980 nm, a cross section of a vertically long ellipse and a major axis diameter of 0.490.
mm and a parallel beam having a minor axis diameter of 0.152 mm.

【0010】このとき、楕円断面の短軸と入射端面2の
曲率が作用する方向とを一致させる。入射平行ビームの
長軸は屈折率分布を有するレンズ本体1によって集束し
ビームウエスト5に集光する。入射平行ビームの短軸は
入射端面2の凹シリンドリカル面によっていったん拡散
ビームに変換され、屈折率分布を有するレンズ本体1を
通過する際に集束光に変換され出力端面3に到達する。
At this time, the minor axis of the elliptical cross section is made to coincide with the direction in which the curvature of the incident end face 2 acts. The long axis of the incident parallel beam is converged by the lens body 1 having a refractive index distribution and condensed on the beam waist 5. The short axis of the incident parallel beam is once converted into a diverging beam by the concave cylindrical surface of the incident end surface 2, and is converted into converged light when passing through the lens body 1 having a refractive index distribution, and reaches the output end surface 3.

【0011】出力端面3における長軸と短軸のビーム断
面寸法はほぼ一致しているが、集光角度が異なる。出力
端面3が平面である場合、集光角度が異なるため長軸と
短軸のビームウエスト位置及び断面直径寸法に差異が生
じ、この差異がシングルモード光ファイバ6との結合損
失増大の要因となる。
Although the beam cross-sections of the major axis and the minor axis at the output end face 3 are almost the same, the focusing angles are different. When the output end face 3 is a plane, the beam converging angles are different, so that the beam waist position and the cross-sectional diameter dimension of the long axis and the short axis are different, and this difference causes an increase in coupling loss with the single mode optical fiber 6. .

【0012】本実施例の場合、出力端面3の凸シリンド
リカル形状により短軸の集光角度を長軸の集光角度と一
致するように矯正している。これらの結果、入射楕円平
行ビームは長軸、短軸ともビームウエスト位置は同一と
なり、シングルモード光ファイバ6のモードフィールド
径とほぼ同一の断面径寸法を有し、シングルモード光フ
ァイバ6と高効率で光結合する。
In the case of this embodiment, the converging angle of the short axis is corrected by the convex cylindrical shape of the output end face 3 so as to match the converging angle of the long axis. As a result, the incident elliptical parallel beam has the same beam waist position in both the long axis and the short axis, has a cross-sectional diameter almost the same as the mode field diameter of the single mode optical fiber 6, and has a high efficiency with the single mode optical fiber 6. Optical coupling.

【0013】[0013]

【発明の効果】本発明によれば、1つのレンズに楕円平
行ビームをシングルモード光ファイバのモードフィール
ド径とほぼ同一の断面径寸法に集束する機能と、ほぼ円
形に整形する機能の2つの機能を持たせることが可能と
なり、シングルモード光ファイバへの結合効率を向上す
る効果がある。本発明の実施例は、端面が平面の屈折率
分布形集束ロッドレンズを用いたときの結合効率と比較
すると約20%高い結合効率が得られた。また、複数の
レンズを接着固定する必要がなく組立位置調整も不要と
なるため製作費用低減効果がある。さらに、接着部がな
いため長期安定性を向上させる効果がある。
According to the present invention, there are two functions, that is, a function of converging an elliptical parallel beam to one lens to a cross-sectional diameter dimension substantially equal to the mode field diameter of a single mode optical fiber, and a function of shaping the beam into a substantially circular shape. And the effect of improving the coupling efficiency to the single mode optical fiber is obtained. In the embodiment of the present invention, a coupling efficiency approximately 20% higher than that obtained by using a gradient index focusing rod lens having a flat end face was obtained. Further, there is no need to bond and fix a plurality of lenses, and it is not necessary to adjust the assembling position. Further, since there is no adhesive portion, there is an effect of improving long-term stability.

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

【図1】本発明の実施例では光結合装置の上面図(a)
及び側面図(b)。
FIG. 1 is a top view of an optical coupling device according to an embodiment of the present invention (a).
And a side view (b).

【符号の説明】[Explanation of symbols]

1…レンズ本体、 2…入射端面、
3…出射端面、4…ビーム、 5…
ビームウエスト、6…シングルモード光ファイバ。
1 ... lens body, 2 ... entrance end face,
3 ... Outgoing end face, 4 ... Beam, 5 ...
Beam waist, 6 ... Single mode optical fiber.

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】集束形ロッドレンズにおいて、片端面に凹
シリンドリカル面を有し、もう一方の端面に前記凹シリ
ンドリカル面と同一軸に作用する凸シリンドリカル面を
有することによって、1個のレンズに光を集束させる機
能とその集束光の断面形状を特定の形状に整形する機能
の2つの機能を持たせたことを特徴とするビーム整形機
能付光結合装置。
A converging rod lens has a concave cylindrical surface on one end surface and a convex cylindrical surface acting on the same axis as the concave cylindrical surface on the other end surface, so that one lens has an optical system. And a function of shaping the cross-sectional shape of the converged light into a specific shape.
【請求項2】出射発散光の断面形状が楕円又は長円状で
あるレーザダイオードと、前記レーザダイオードの出射
発散光を平行又は疑似平行光に変換するコリメータレン
ズと前記平行又は疑似平行光を集束させる集束レンズと
集束光が光結合される光ファイバからなる光学系を有
し、前記レーザダイオードと前記光学系を同一ケースに
収容、固定したレーザダイオードモジュールにおいて、
前記集光レンズに請求項1の光結合装置を使用したこと
を特徴とするレーザダイオードモジュール。
2. A laser diode in which the cross-sectional shape of the emitted divergent light is elliptical or elliptical, a collimator lens for converting the divergent light emitted from the laser diode into parallel or pseudo-parallel light, and focusing the parallel or pseudo-parallel light. A laser diode module having an optical system including a focusing lens to be focused and an optical fiber in which the focused light is optically coupled, wherein the laser diode and the optical system are housed in the same case and fixed.
A laser diode module using the optical coupling device according to claim 1 for the condenser lens.
【請求項3】出射発散光の断面形状が楕円又は長円状で
あるレーザダイオードと、前記レーザダイオードの出射
発散光を集束させる集束レンズと集束光が光結合される
光ファイバからなる光学系を有し、前記レーザダイオー
ドと前記光学系を同一ケースに収容、固定したレーザダ
イオードモジュールにおいて、前記集光レンズに請求項
1の光結合装置を使用したことを特徴とするレーザダイ
オードモジュール。
3. An optical system comprising a laser diode having a cross-sectional shape of an emitted divergent light having an elliptical or elliptical shape, a focusing lens for focusing the emitted divergent light of the laser diode, and an optical fiber for optically coupling the focused light. A laser diode module comprising a laser diode module and the optical system housed and fixed in the same case, wherein the optical coupling device according to claim 1 is used for the condenser lens.
JP2064198A 1998-02-02 1998-02-02 Optical coupling device with beam shaping function and laser diode module Withdrawn JPH11218649A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2064198A JPH11218649A (en) 1998-02-02 1998-02-02 Optical coupling device with beam shaping function and laser diode module

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2064198A JPH11218649A (en) 1998-02-02 1998-02-02 Optical coupling device with beam shaping function and laser diode module

Publications (1)

Publication Number Publication Date
JPH11218649A true JPH11218649A (en) 1999-08-10

Family

ID=12032863

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2064198A Withdrawn JPH11218649A (en) 1998-02-02 1998-02-02 Optical coupling device with beam shaping function and laser diode module

Country Status (1)

Country Link
JP (1) JPH11218649A (en)

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR20030032509A (en) * 2001-10-18 2003-04-26 엘지전자 주식회사 Optical device
JP2009283639A (en) * 2008-05-21 2009-12-03 Opnext Japan Inc Surface light emitting laser element and its production process
JP2011107725A (en) * 2011-02-07 2011-06-02 Scalar Corp Rod lens, and method and device for working the same
CN103576254A (en) * 2012-07-24 2014-02-12 阿尔卑斯电气株式会社 Light module
CN108363144B (en) * 2018-05-09 2020-12-29 上海飞博激光科技有限公司 High-power optical fiber circulator based on curved surface optical fiber end cap
CN114459459A (en) * 2022-03-07 2022-05-10 北京航空航天大学 Small space light integrated light receiving and transmitting integrated module adopting single lens

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR20030032509A (en) * 2001-10-18 2003-04-26 엘지전자 주식회사 Optical device
JP2009283639A (en) * 2008-05-21 2009-12-03 Opnext Japan Inc Surface light emitting laser element and its production process
JP2011107725A (en) * 2011-02-07 2011-06-02 Scalar Corp Rod lens, and method and device for working the same
CN103576254A (en) * 2012-07-24 2014-02-12 阿尔卑斯电气株式会社 Light module
CN108363144B (en) * 2018-05-09 2020-12-29 上海飞博激光科技有限公司 High-power optical fiber circulator based on curved surface optical fiber end cap
CN114459459A (en) * 2022-03-07 2022-05-10 北京航空航天大学 Small space light integrated light receiving and transmitting integrated module adopting single lens

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Effective date: 20050405