JP2019219435A - Optical isolator and manufacturing method thereof - Google Patents

Optical isolator and manufacturing method thereof Download PDF

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JP2019219435A
JP2019219435A JP2018114322A JP2018114322A JP2019219435A JP 2019219435 A JP2019219435 A JP 2019219435A JP 2018114322 A JP2018114322 A JP 2018114322A JP 2018114322 A JP2018114322 A JP 2018114322A JP 2019219435 A JP2019219435 A JP 2019219435A
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optical isolator
cylindrical magnet
isolator element
optical
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JP7037135B2 (en
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和啓 峯島
Kazuhiro Mineshima
和啓 峯島
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SMM Precision Co Ltd
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Abstract

To provide an optical isolator capable of fitting and fixing an optical isolator element into a through hole of a cylindrical magnet at designed incident and emitting end face angles even if a holder is not used, and to provide a manufacturing method thereof.SOLUTION: An optical isolator includes: a nearly parallelepiped optical isolator element 10 that includes at least two polarizers 2, 4 and one Faraday rotor 3 and allows them to be laminated on the light transmission surface; and a cylindrical magnet 1 for housing the optical isolator element. In the optical isolator element, a ridge line part of the optical isolator element formed by connecting corner parts of the polarizers and a corner part of the Faraday rotor and the peripheral parts are adhered to an inner wall of the cylindrical magnet to fix the optical isolator element into the cylindrical magnet, and only the two adjacent ridge line parts of the optical isolator element and the peripheral parts are adhered to the inner wall of the cylindrical magnet.SELECTED DRAWING: Figure 1

Description

本発明は、光通信や光情報システム等で使用される半導体モジュールに組み込まれる光アイソレータに係り、特に、円筒型磁石の貫通孔内に接着剤を用いて光学素子が接着固定された光アイソレータとその製造方法の改良に関するものである。   The present invention relates to an optical isolator incorporated in a semiconductor module used in an optical communication or an optical information system or the like, and more particularly to an optical isolator in which an optical element is adhesively fixed using an adhesive in a through hole of a cylindrical magnet. The present invention relates to improvement of the manufacturing method.

光アイソレータは、一般に、ファラデー回転子、このファラデー回転子を飽和させるための永久磁石、入射側偏光子、出射側偏光子とで構成される。また、ファラデー回転子に関しては、ファラデー回転子そのものの厚みを調整することにより、光の偏波面が45度回転するように調整されているものを使用している。   An optical isolator generally includes a Faraday rotator, a permanent magnet for saturating the Faraday rotator, an incident-side polarizer, and an output-side polarizer. As the Faraday rotator, a Faraday rotator whose thickness is adjusted so that the plane of polarization of light is rotated by 45 degrees is used.

そして、光アイソレータにおいて、入射側偏光子を通過しファラデー回転子に対して順方向に入ってきた直線偏光は、ファラデー回転子を透過することにより入射した直線偏光の偏波面が45度回転され、その回転位置で透過光量が最大となるように調整された出射側偏光子を透過する。よって、殆ど損失のない光として次の光学系へと伝送される。   Then, in the optical isolator, the linearly polarized light that has passed through the incident-side polarizer and entered the forward direction with respect to the Faraday rotator rotates the polarization plane of the incident linearly polarized light by transmitting the Faraday rotator by 45 degrees, At the rotation position, the light passes through the exit-side polarizer adjusted so that the amount of transmitted light is maximized. Therefore, the light is transmitted to the next optical system as light having almost no loss.

また、光アイソレータにおいて、反射戻り光がある場合、出射側偏光子を透過した直線偏光は、ファラデー回転子を透過することにより偏波面が45度回転され、これにより入射側偏光子と直交することになるため消光する。このようにして、光アイソレータの機能が果たされることになる。   In the case where there is reflected return light in the optical isolator, the plane of polarization of the linearly polarized light that has passed through the output-side polarizer is rotated by 45 degrees by transmitting through the Faraday rotator, and is thereby orthogonal to the incident-side polarizer. It becomes quenched because it becomes. In this way, the function of the optical isolator is performed.

ところで、光アイソレータにおいて、ファラデー回転子、入射側偏光子、出射側偏光子といった各光学素子の表面には反射防止膜が施され、また、各光学素子を接着剤で一体化したもの(光アイソレータ素子と称する)が用いられることが多い。尚、各光学素子の入出射端面には上記反射防止膜が施されているものの各光学素子の入出射端面では僅かに光が反射され、この反射光が元の光路を戻ってしまうことを防止するため、意図的に光アイソレータ素子の入出射端面を光軸に垂直な面から数度傾けることがある。   Incidentally, in an optical isolator, an antireflection film is applied to the surface of each optical element such as a Faraday rotator, an incident-side polarizer, and an output-side polarizer, and each optical element is integrated with an adhesive (optical isolator). Element) is often used. Although the above-mentioned antireflection film is applied to the input / output end face of each optical element, light is slightly reflected at the input / output end face of each optical element, and this reflected light is prevented from returning to the original optical path. Therefore, the input / output end face of the optical isolator element may be intentionally inclined several degrees from a plane perpendicular to the optical axis.

そして、光アイソレータ素子の入出射端面を傾斜させる方法として、傾斜面を有するホルダーに光アイソレータ素子を固定する方法(特許文献1参照)、入出射端面が光軸に垂直な面に対し傾斜する断面平行四辺形状の光アイソレータ素子(特許文献2参照)を作製し、これを円筒型磁石の貫通孔内に接着する方法が知られている。   As a method for inclining the input / output end face of the optical isolator element, a method of fixing the optical isolator element to a holder having an inclined surface (see Patent Document 1), a cross section in which the input / output end face is inclined with respect to a plane perpendicular to the optical axis There is known a method of manufacturing a parallelogram-shaped optical isolator element (see Patent Document 2) and bonding the same in a through hole of a cylindrical magnet.

後者の方法は、前者の方法に較べてホルダーを要しないというメリットがあるものの、光アイソレータ素子を円筒型磁石の貫通孔内に接着する際、光軸に垂直な面に対する光アイソレータ素子の入出射端面角度が設計時の設定からずれてしまうことがあった。   The latter method has the advantage of not requiring a holder as compared with the former method, but when the optical isolator element is bonded into the through hole of the cylindrical magnet, the optical isolator element enters and exits from a plane perpendicular to the optical axis. The end face angle sometimes deviated from the design setting.

そして、光軸に垂直な面に対する光アイソレータ素子の入出射端面角度が設計時の設定からずれた場合、設計時における光アイソレータの所望とする光学特性が得られなくなる問題が存在した。   Then, when the angle of the input / output end face of the optical isolator element with respect to the plane perpendicular to the optical axis deviates from the setting at the time of design, there is a problem that desired optical characteristics of the optical isolator at the time of design cannot be obtained.

特開2015−125374号公報(図10参照)Japanese Patent Application Laid-Open No. 2015-125374 (see FIG. 10) 特開2015−084016号公報(図4参照)JP-A-2015-084016 (see FIG. 4)

本発明はこのような問題点に着目してなされたもので、その課題とするところは、ホルダーを用いなくても設計通りの入出射端面角度で円筒型磁石の貫通孔内に光アイソレータ素子を接着、固定できる光アイソレータとその製造方法を提供することにある。   The present invention has been made in view of such a problem, and an object of the present invention is to place an optical isolator element in a through-hole of a cylindrical magnet at an input / output end face angle as designed without using a holder. An object of the present invention is to provide an optical isolator that can be bonded and fixed and a method of manufacturing the same.

そこで、上記課題を解決するため、本発明者は、円筒型磁石の貫通孔内に光アイソレータ素子を接着する際、光軸に垂直な面に対する光アイソレータ素子の入出射端面角度が設計時の設定からずれてしまう原因について調査、分析を行った。   In order to solve the above problems, the present inventor has set the angle of the input / output end face of the optical isolator element with respect to the plane perpendicular to the optical axis when designing the optical isolator element in the through hole of the cylindrical magnet. We investigated and analyzed the cause of the deviation.

従来、円筒型磁石の貫通孔内に光アイソレータ素子を接着する場合、対称性を考慮し、円筒型磁石の内壁面(貫通孔の内壁面)近傍に位置する光アイソレータ素子の4つの稜線部(偏光子の角部とファラデー回転子の角部を結んで形成される光アイソレータ素子の4つの稜線部)とその周辺部を接着剤により円筒型磁石の内壁面に接着していた。   Conventionally, when an optical isolator element is adhered in a through hole of a cylindrical magnet, considering the symmetry, four ridges of the optical isolator element located near the inner wall surface (the inner wall surface of the through hole) of the cylindrical magnet are considered. The four ridges of the optical isolator element formed by connecting the corner of the polarizer and the corner of the Faraday rotator) and the periphery thereof were bonded to the inner wall surface of the cylindrical magnet with an adhesive.

しかし、円筒型磁石の内径(貫通孔の内径)は、光アイソレータ素子が円筒型磁石の貫通孔内に確実に納められるよう、若干、大きめに公差が定められているため、内径が大きめの円筒型磁石を用いた場合には、円筒型磁石の内壁と光アイソレータ素子のクリアランス(隙間)が大きくなる。このため、平行六面体形状を有する光アイソレータ素子10の4つの稜線部とその周辺部を円筒型磁石1の内壁に接着する際、図3(a)〜(b)に示すように接着剤20の不均一な硬化収縮により収縮方向(図3a〜bにおいて硬化収縮方向を矢印で示す)を制御することが難しく、光アイソレータ素子10の中心軸βと円筒型磁石1の中心軸αが交差してしまう(光アイソレータ素子10の中心軸βと円筒型磁石1の中心軸αは交差せずに互いに重なり合うか平行になっていることが好ましい)配置関係になり易い。この結果、図1(d)に示す光軸Pに垂直な面に対する光アイソレータ素子10の入出射端面角度が設計時の設定(設計時において光アイソレータ素子の入出射端面角度はθに設定されている)からずれてしまうことが判明した。本発明はこのような調査、分析により完成されたものである。   However, the inner diameter of the cylindrical magnet (the inner diameter of the through-hole) is set slightly larger to ensure that the optical isolator element can be accommodated in the through-hole of the cylindrical magnet. When a type magnet is used, the clearance (gap) between the inner wall of the cylindrical magnet and the optical isolator element increases. For this reason, when bonding the four ridges of the optical isolator element 10 having a parallelepiped shape and the periphery thereof to the inner wall of the cylindrical magnet 1, as shown in FIGS. It is difficult to control the shrinking direction (the hardening shrinking direction is indicated by an arrow in FIGS. 3A and 3B) due to uneven curing shrinkage, and the center axis β of the optical isolator element 10 and the center axis α of the cylindrical magnet 1 intersect. (It is preferable that the central axis β of the optical isolator element 10 and the central axis α of the cylindrical magnet 1 do not intersect but overlap each other or are parallel to each other). As a result, the angle of the input / output end face of the optical isolator element 10 with respect to the plane perpendicular to the optical axis P shown in FIG. 1D is set at the time of design (the angle of the input / output end face of the optical isolator element is set to θ at the time of design). ). The present invention has been completed through such research and analysis.

すなわち、本発明に係る第1の発明は、
少なくとも2つの偏光子と1つのファラデー回転子を有しかつこれ等がその光透過面で貼り合わされて成る平行六面体形状の光アイソレータ素子と、この光アイソレータ素子が収容される円筒型磁石とを備え、上記偏光子の角部とファラデー回転子の角部を結んで形成される光アイソレータ素子の稜線部とその周辺部を円筒型磁石の内壁に接着させて光アイソレータ素子が円筒型磁石内に固定されている光アイソレータの製造方法において、
上記光アイソレータ素子を円筒型磁石内に挿入した後、光アイソレータ素子の隣り合う2つの上記稜線部とその周辺部にのみ接着剤を塗布して、光アイソレータ素子の上記2つの稜線部とその周辺部のみを円筒型磁石の内壁に接着させることを特徴とし、
第2の発明は、
第1の発明に記載の光アイソレータの製造方法において、
上記接着剤が熱硬化型接着剤で構成され、かつ、塗布作業中における熱硬化型接着剤の粘度が0.6Pa・s以上1.7Pa・s以下であることを特徴とする。
That is, the first invention according to the present invention is:
A parallelepiped-shaped optical isolator element having at least two polarizers and one Faraday rotator and bonded to each other at a light transmitting surface thereof, and a cylindrical magnet accommodating the optical isolator element. The ridge of the optical isolator element formed by connecting the corner of the polarizer and the corner of the Faraday rotator and the periphery thereof are adhered to the inner wall of the cylindrical magnet, and the optical isolator is fixed in the cylindrical magnet. In the method of manufacturing an optical isolator,
After the optical isolator element is inserted into the cylindrical magnet, an adhesive is applied only to the two adjacent ridges of the optical isolator element and the periphery thereof, and the two ridges of the optical isolator element and the periphery thereof are applied. Characterized in that only the part is adhered to the inner wall of the cylindrical magnet,
The second invention is
In the method for manufacturing an optical isolator according to the first invention,
The adhesive is composed of a thermosetting adhesive, and the viscosity of the thermosetting adhesive during application is 0.6 Pa · s or more and 1.7 Pa · s or less.

また、本発明に係る第3の発明は、
少なくとも2つの偏光子と1つのファラデー回転子を有しかつこれ等がその光透過面で貼り合わされて成る平行六面体形状の光アイソレータ素子と、この光アイソレータ素子が収容される円筒型磁石とを備え、上記偏光子の角部とファラデー回転子の角部を結んで形成される光アイソレータ素子の稜線部とその周辺部を円筒型磁石の内壁に接着させて光アイソレータ素子が円筒型磁石内に固定されている光アイソレータにおいて、
光アイソレータ素子の隣り合う2つの上記稜線部とその周辺部のみが円筒型磁石の内壁に接着されていることを特徴とする。
Further, a third invention according to the present invention provides:
A parallelepiped-shaped optical isolator element having at least two polarizers and one Faraday rotator and bonded to each other at a light transmitting surface thereof, and a cylindrical magnet accommodating the optical isolator element. The ridge of the optical isolator element formed by connecting the corner of the polarizer and the corner of the Faraday rotator and the periphery thereof are adhered to the inner wall of the cylindrical magnet, and the optical isolator is fixed in the cylindrical magnet. Optical isolator
Only the two adjacent ridges of the optical isolator element and the periphery thereof are bonded to the inner wall of the cylindrical magnet.

本発明に係る光アイソレータの製造方法によれば、
光アイソレータ素子を円筒型磁石内に挿入した後、光アイソレータ素子の隣り合う2つの稜線部とその周辺部にのみ接着剤を塗布して、光アイソレータ素子の上記2つの稜線部とその周辺部のみを円筒型磁石の内壁に接着させているため、接着剤が硬化収縮する際の収縮方向を概ね一方向に制限することが可能となる。従って、光アイソレータ素子の中心軸と円筒型磁石の中心軸が交差してしまう配置関係になり難いため、光軸に垂直な面に対する光アイソレータ素子の入出射端面角度のずれを抑制することが可能となる。
According to the method for manufacturing an optical isolator according to the present invention,
After the optical isolator element is inserted into the cylindrical magnet, the adhesive is applied only to the two adjacent ridges of the optical isolator element and the periphery thereof, and only the two ridges of the optical isolator element and the periphery thereof are applied. Is adhered to the inner wall of the cylindrical magnet, so that the shrinking direction when the adhesive cures and shrinks can be restricted to substantially one direction. Therefore, since it is difficult for the central axis of the optical isolator element and the central axis of the cylindrical magnet to intersect, it is possible to suppress the deviation of the angle of the input / output end face of the optical isolator element with respect to the plane perpendicular to the optical axis. It becomes.

図1(a)は本発明に係る光アイソレータの正面図、図1(b)は図1(a)におけるA−A’面の概略断面図、図1(c)は本発明に係る光アイソレータの概略斜視図、図1(d)は円筒型磁石に固定される光アイソレータ素子10の光軸Pに垂直な面に対する設計時における入出射端面角度(θ)の説明図。1A is a front view of an optical isolator according to the present invention, FIG. 1B is a schematic cross-sectional view taken along the line AA ′ in FIG. 1A, and FIG. 1C is an optical isolator according to the present invention. FIG. 1 (d) is an explanatory view of an incident / exit end face angle (θ) at the time of design with respect to a plane perpendicular to the optical axis P of an optical isolator element 10 fixed to a cylindrical magnet. 光軸に垂直な面に対する光アイソレータ素子の設計時における入出射端面角度(チップ角度)と、上記光アイソレータ素子が円筒型磁石の内壁に接着固定された後における光アイソレータの光軸に垂直な面に対する入出射端面角度(組立後角度)との関係を示すグラフ図で、符号◇は平行六面体形状を有する光アイソレータ素子の隣り合う2つの稜線部とその周辺部を円筒型磁石の内壁に接着させた光アイソレータ(2稜線接着)のチップ角度と組立後角度との関係を示し、符号□は平行六面体形状を有する光アイソレータ素子の4つの稜線部とその周辺部を円筒型磁石の内壁に接着させた光アイソレータ(4稜線接着)のチップ角度と組立後角度との関係をそれぞれ示す。The angle of the input / output end face (chip angle) at the time of designing the optical isolator element with respect to the plane perpendicular to the optical axis, and the plane perpendicular to the optical axis of the optical isolator after the optical isolator element is adhered and fixed to the inner wall of the cylindrical magnet. Is a graph showing the relationship between the input and output end face angles (assembled angles) of the optical isolator element having a parallelepiped shape, and the adjacent two ridges and the periphery thereof are adhered to the inner wall of the cylindrical magnet. Shows the relationship between the chip angle of the optical isolator (adhesion with two ridges) and the angle after assembling, and the symbol □ indicates that the four ridges of the optical isolator element having a parallelepiped shape and its peripheral portion are bonded to the inner wall of the cylindrical magnet. The relationship between the chip angle of the optical isolator (four-edge bonding) and the angle after assembly is shown. 図3(a)は平行六面体形状を有する光アイソレータ素子の4つの稜線部とその周辺部を円筒型磁石の内壁に接着させた光アイソレータの断面図、図3(b)はその正面図。FIG. 3A is a cross-sectional view of an optical isolator in which four ridges and a peripheral portion of the optical isolator element having a parallelepiped shape are adhered to an inner wall of a cylindrical magnet, and FIG. 3B is a front view thereof. 図4(a)は平行六面体形状を有する光アイソレータ素子の隣り合う2つの稜線部とその周辺部を円筒型磁石の内壁に接着させた光アイソレータの断面図、図4(b)はその正面図。FIG. 4A is a cross-sectional view of an optical isolator in which two adjacent ridges and a peripheral portion of the optical isolator element having a parallelepiped shape are adhered to the inner wall of a cylindrical magnet, and FIG. 4B is a front view thereof. .

以下、本発明に係る実施の形態について詳細に説明する。   Hereinafter, embodiments of the present invention will be described in detail.

(1)光アイソレータ
本発明に係る光アイソレータは、図1(a)〜(d)に示すように円形状の貫通孔を有する円筒型磁石1と、円筒型磁石1の貫通孔内に挿入された光アイソレータ素子10と、光アイソレータ素子10を円筒型磁石1の貫通孔内壁に接合させる接着剤5、6とで構成されている。
(1) Optical Isolator The optical isolator according to the present invention is, as shown in FIGS. 1A to 1D, a cylindrical magnet 1 having a circular through-hole, and inserted into the through-hole of the cylindrical magnet 1. The optical isolator element 10 and adhesives 5 and 6 for joining the optical isolator element 10 to the inner wall of the through-hole of the cylindrical magnet 1.

また、光アイソレータ素子10は、光が入射する側の第1偏光子2、ファラデー回転子3および光が出射する側の第2偏光子4を有し、これ等が光学接着剤を用いて貼り合わされた平行六面体形状を有している。また、上記第1偏光子2の角部とファラデー回転子3の角部および第2偏光子4の角部を結んで形成される稜線部の隣り合う2箇所とその周辺部のみが円筒型磁石1の内壁に接着固定されている。   Further, the optical isolator element 10 has a first polarizer 2, a Faraday rotator 3 on the side where light enters, and a second polarizer 4 on the side where light exits, and these are attached using an optical adhesive. It has a fitted parallelepiped shape. Also, only two adjacent ridges formed by connecting the corners of the first polarizer 2 with the corners of the Faraday rotator 3 and the corners of the second polarizer 4 and the periphery thereof are cylindrical magnets only. 1 is adhesively fixed to the inner wall.

尚、平行六面体とは、三組の相対する面がそれぞれ平行な六面体を意味する。   In addition, a parallelepiped means a hexahedron whose three opposing surfaces are respectively parallel.

そして、本発明に係る光アイソレータは、図4(a)〜(b)に示すように光アイソレータ素子10の隣り合う2つの稜線部とその周辺部のみが円筒型磁石1の内壁に接着させているため、接着剤5、6が硬化収縮する際の収縮方向(図4a〜bにおいて硬化収縮方向を矢印で示す)を概ね一方向に制御することが可能となる。従って、光アイソレータ素子10の中心軸βと円筒型磁石1の中心軸αが交差してしまう配置関係になり難い(光アイソレータ素子10の中心軸βと円筒型磁石1の中心軸αが略平行になっている)ため、光軸に垂直な面に対する光アイソレータ素子10の入出射端面角度のずれを抑制することが可能となる。   Then, in the optical isolator according to the present invention, as shown in FIGS. 4A and 4B, only two adjacent ridges of the optical isolator element 10 and the periphery thereof are bonded to the inner wall of the cylindrical magnet 1. Therefore, it is possible to control the contraction direction (the curing contraction direction is indicated by an arrow in FIGS. 4A and 4B) when the adhesives 5 and 6 cure and contract in substantially one direction. Accordingly, it is difficult for the central axis β of the optical isolator element 10 to intersect with the central axis α of the cylindrical magnet 1 (the central axis β of the optical isolator element 10 is substantially parallel to the central axis α of the cylindrical magnet 1). Therefore, it is possible to suppress the deviation of the angle of the input / output end face of the optical isolator element 10 with respect to the plane perpendicular to the optical axis.

また、本発明に係る光アイソレータにおいては、光アイソレータ素子、円筒型磁石として、従来と同様のものを使用することができる。   Further, in the optical isolator according to the present invention, the same optical isolator element and cylindrical magnet as those in the related art can be used.

(2)光アイソレータ素子
少なくとも2つの偏光子と1つのファラデー回転子を有しかつこれ等がその光透過面で貼り合わされて成る平行六面体形状の光アイソレータ素子としては、「シングル型の光アイソレータ用光学素子」(偏光子/ファラデー回転子/偏光子)、シングル型の光アイソレータ用光学素子を組み合わせた「ダブル型の光アイソレータ用光学素子」(偏光子/ファラデー回転子/偏光子/偏光子/ファラデー回転子/偏光子)、および、「セミダブル型の光アイソレータ用光学素子」(偏光子/ファラデー回転子/偏光子/ファラデー回転子/偏光子)等が例示される。
(2) Optical Isolator Element As a parallelepiped-shaped optical isolator element having at least two polarizers and one Faraday rotator, which are bonded together on their light transmitting surfaces, a “single-type optical isolator” "Optical element" (polarizer / Faraday rotator / polarizer), "Double type optical isolator for optical isolator" combining optical element for optical isolator (Polarizer / Faraday rotator / polarizer / polarizer / Faraday rotator / polarizer) and "semi-double type optical element for optical isolator" (polarizer / Faraday rotator / polarizer / Faraday rotator / polarizer) and the like.

また、光アイソレータ素子10の形状としては、断面平行四辺形状の偏光子とファラデー回転子とで構成される図1(d)に示す平行六面体(対峙する一組の面が平行四辺形状を有し、対峙する残り二組の面が正方形若しくは長方形状を有する)、あるいは、断面正方形若しくは長方形状の偏光子とファラデー回転子とで構成される図4(a)に示す平行六面体(立方体若しくは直方体形状を有する)が例示される。   Further, as the shape of the optical isolator element 10, a parallelepiped shown in FIG. 1D composed of a polarizer having a parallelogram cross section and a Faraday rotator (a set of opposing faces has a parallelogram shape). The remaining two pairs of opposing faces have a square or rectangular shape, or a parallelepiped (cubic or rectangular parallelepiped) shown in FIG. Is exemplified).

(3)光アイソレータの製造方法
次に、本発明に係る光アイソレータの製造方法について説明する。
(3) Manufacturing Method of Optical Isolator Next, a manufacturing method of the optical isolator according to the present invention will be described.

まず、V溝等が形成された載置台上に円筒型磁石をその貫通孔が水平になるように載置し、光アイソレータ素子を円筒型磁石の貫通孔に挿入する。このとき、光アイソレータ素子の挿入方向を揃える必要はない。貫通孔に挿入された光アイソレータ素子は自重により、隣り合う2つの稜線部が円筒型磁石の貫通孔内壁に接することになる。   First, a cylindrical magnet is mounted on a mounting table on which a V-groove or the like is formed so that its through-hole is horizontal, and an optical isolator element is inserted into the through-hole of the cylindrical magnet. At this time, it is not necessary to align the insertion directions of the optical isolator elements. Due to the weight of the optical isolator element inserted into the through-hole, two adjacent ridges contact the inner wall of the through-hole of the cylindrical magnet.

次に、円筒型磁石の貫通孔内壁に接する光アイソレータ素子の隣り合う2つの稜線部とその周辺部に対しディスペンサを用いて接着剤を塗布する。   Next, an adhesive is applied to two adjacent ridges of the optical isolator element which is in contact with the inner wall of the through hole of the cylindrical magnet and a peripheral portion thereof using a dispenser.

このとき、接着剤の粘度は0.6Pa・s以上1.7Pa・s以下であることが好ましい。接着剤の粘度が低過ぎると、接着剤が光アイソレータ素子の上記稜線部近傍に留まらず流れてしまい、光アイソレータ素子の隣り合う2つの稜線部とその周辺部で接着させることが困難となる。また、接着剤の粘度が高過ぎると、光アイソレータ素子の隣り合う2つの稜線部とその周辺部全体に接着剤を行き渡らせるのが難しく、結果として接着面積が小さくなり、十分な接着強度を得ることが困難になる。適用する接着剤の種類としては熱硬化型および紫外線硬化型接着剤のいずれも適用できるが、耐環境性の観点からはエポキシ系樹脂で構成される接着剤が好ましい。   At this time, the viscosity of the adhesive is preferably 0.6 Pa · s or more and 1.7 Pa · s or less. If the viscosity of the adhesive is too low, the adhesive flows instead of staying in the vicinity of the ridge of the optical isolator element, and it is difficult to bond the two adjacent ridges of the optical isolator element and its peripheral portion. Further, if the viscosity of the adhesive is too high, it is difficult to spread the adhesive over the two adjacent ridges of the optical isolator element and the entire periphery thereof, and as a result, the bonding area becomes small and sufficient bonding strength is obtained. It becomes difficult. As the kind of the adhesive to be applied, any of a thermosetting adhesive and an ultraviolet curing adhesive can be applied, but from the viewpoint of environmental resistance, an adhesive composed of an epoxy resin is preferable.

尚、二液混合タイプの接着剤が適用される場合、主剤と硬化剤を混合した後、時間の経過と共に粘度が上昇するため、粘度が0.6Pa・s以上1.7Pa・s以下となる時間内で接着剤の塗布作業を終了させることが好ましい。   When a two-component adhesive is used, the viscosity increases with the lapse of time after the main agent and the curing agent are mixed, so that the viscosity becomes 0.6 Pa · s or more and 1.7 Pa · s or less. It is preferable to finish the operation of applying the adhesive within the time.

最後に、上記接着剤を硬化させることで光アイソレータが完成する。   Finally, the optical isolator is completed by curing the adhesive.

以下、本発明の実施例について具体的に説明する。   Hereinafter, examples of the present invention will be specifically described.

予め11mm角の第1偏光子、ファラデー回転子、第2偏光子を接着剤により接着し、かつ、特許文献2に記載された光学素子の製造方法により、ダイシングソーで切断して、光透過面の大きさが1.4mm角の光アイソレータ素子を作製した。尚、光アイソレータ素子の光透過面は光軸に垂直な面から6±0.5度傾斜させている。   A first polarizer, a Faraday rotator, and a second polarizer of 11 mm square are bonded in advance with an adhesive, and are cut with a dicing saw by a method of manufacturing an optical element described in Patent Document 2 to obtain a light transmitting surface. An optical isolator element having a size of 1.4 mm square was manufactured. The light transmitting surface of the optical isolator element is inclined by 6 ± 0.5 degrees from a surface perpendicular to the optical axis.

また、未着磁の外径3mm、内径2mm、長さ2mmの円筒型磁石を用意した。円筒型磁石の内径は光アイソレータ素子の光透過面の対角長さより若干大きくなっている。   In addition, an unmagnetized cylindrical magnet having an outer diameter of 3 mm, an inner diameter of 2 mm, and a length of 2 mm was prepared. The inner diameter of the cylindrical magnet is slightly larger than the diagonal length of the light transmitting surface of the optical isolator element.

まず、V溝が形成された載置台上に、上記円筒型磁石をその貫通孔が水平になるように載置した後、用意した上記光アイソレータ素子を円筒型磁石の貫通孔に挿入した。   First, the cylindrical magnet was mounted on a mounting table on which a V-groove was formed so that its through-hole was horizontal, and then the prepared optical isolator element was inserted into the through-hole of the cylindrical magnet.

次いで、円筒型磁石の貫通孔内壁に接する光アイソレータ素子の隣り合う2つの稜線部とその周辺部に対し、ディスペンサを用いて市販の熱硬化型エポキシ系接着剤(株式会社ダイゾー社製、型番:NB3200)を塗布した。この接着剤の硬化前における初期粘度は0.66Pa・sであった。本実施例で使用した接着剤は二液混合タイプの接着剤であり、粘度は時間と共に上昇するが、接着剤の塗布作業が終了したときの粘度は1.7Pa・sであった。   Then, using a dispenser, a commercially available thermosetting epoxy adhesive (manufactured by Daizo Co., Ltd., model number: 2) on the adjacent two ridges of the optical isolator element that is in contact with the inner wall of the through hole of the cylindrical magnet and the periphery thereof NB3200) was applied. The initial viscosity of the adhesive before curing was 0.66 Pa · s. The adhesive used in the present example was a two-part mixed type adhesive, and although the viscosity increased with time, the viscosity when the application of the adhesive was completed was 1.7 Pa · s.

最後に塗布した接着剤を硬化させて実施例に係る光アイソレータを完成させた。   Finally, the applied adhesive was cured to complete the optical isolator according to the example.

また、比較のために、実施例と同一である光アイソレータ素子の4つの稜線部とその周辺部に対し接着剤を塗布、硬化させた比較例に係る光アイソレータも作製した。   For comparison, an optical isolator according to a comparative example was also prepared in which an adhesive was applied to the four ridges of the optical isolator element and the periphery thereof, which were the same as those in the example, and cured.

そして、実施例と比較例に係る光アイソレータ素子の円筒型磁石端面に対する光透過面の角度を比較したグラフ図を図2に示す。尚、円筒型磁石端面は光軸に対して垂直に設置されるため、円筒型磁石端面に対する光アイソレータ素子における光透過面の角度は、光軸に垂直な面に対する光アイソレータ素子の入出射端面角度と同じである。また、図2中、符号◇は光アイソレータ素子の隣り合う2つの稜線部とその周辺部を円筒型磁石の内壁に接着させた実施例に係る光アイソレータ(2稜線接着)のチップ角度と組立後角度との関係を示し、符号□は光アイソレータ素子の4つの稜線部とその周辺部を円筒型磁石の内壁に接着させた比較例に係る光アイソレータ(4稜線接着)のチップ角度と組立後角度との関係をそれぞれ示す。   FIG. 2 is a graph comparing the angles of the light transmitting surface with respect to the cylindrical magnet end surfaces of the optical isolator elements according to the example and the comparative example. Since the cylindrical magnet end face is installed perpendicular to the optical axis, the angle of the light transmitting surface of the optical isolator element with respect to the cylindrical magnet end face is determined by the angle of the input / output end face of the optical isolator element with respect to the plane perpendicular to the optical axis. Is the same as In FIG. 2, the symbol ◇ indicates the chip angle of the optical isolator (two-edge bonding) according to the embodiment in which the two adjacent ridges of the optical isolator element and the periphery thereof are bonded to the inner wall of the cylindrical magnet. The symbol □ indicates the chip angle and the assembling angle of the optical isolator (four-edge bonding) according to the comparative example in which the four ridges of the optical isolator element and the periphery thereof are bonded to the inner wall of the cylindrical magnet. The relationship with is shown below.

図2のグラフ図から、符号◇で示される実施例に係る光アイソレータの円筒型磁石端面に対する光透過面の角度は、設計時における入出射端面角度(上述した6±0.5度)に対し±1度の範囲に収まっている。他方、符号□で示される比較例に係る光アイソレータの円筒型磁石端面に対する光透過面の角度は、設計時における入出射端面角度(6±0.5度)に対し5度のずれが確認される。   From the graph of FIG. 2, the angle of the light transmitting surface with respect to the cylindrical magnet end surface of the optical isolator according to the embodiment indicated by the symbol ◇ is larger than the incident / exit end surface angle (6 ± 0.5 degrees described above) at the time of design. It is within ± 1 degree. On the other hand, the angle of the light transmitting surface with respect to the cylindrical magnet end surface of the optical isolator according to the comparative example indicated by the symbol □ was deviated by 5 degrees from the input / output end surface angle (6 ± 0.5 degrees) at the time of design. You.

従って、本発明に係る光アイソレータの製造方法によりホルダーを用いなくても設計通りの入出射端面角度で円筒型磁石の貫通孔内に光アイソレータ素子を接着、固定できることが確認される。   Therefore, it is confirmed that the optical isolator element can be bonded and fixed in the through-hole of the cylindrical magnet at the designed input / output end face angle without using the holder by the optical isolator manufacturing method according to the present invention.

本発明に係る光アイソレータによれば、光軸に垂直な面に対する光アイソレータ素子の入出射端面角度のずれが抑制されるため、光通信や光情報システム等で使用される半導体モジュールに組み込まれる産業上の利用可能性を有している。   ADVANTAGE OF THE INVENTION According to the optical isolator which concerns on this invention, since the deviation | shift of the entrance / exit end surface angle of an optical isolator element with respect to the surface perpendicular | vertical to an optical axis is suppressed, the industrial built into the semiconductor module used for optical communication, an optical information system, etc. Has the above availability.

1 円筒型磁石
2 第1偏光子
3 ファラデー回転子
4 第2偏光子
5、6 接着剤
10 光アイソレータ素子
20 接着剤
α 円筒型磁石の中心軸
β 光アイソレータ素子の中心軸
θ 設計時における光アイソレータ素子の入出射端面角度
Reference Signs List 1 cylindrical magnet 2 first polarizer 3 Faraday rotator 4 second polarizer 5, 6 adhesive 10 optical isolator element 20 adhesive α central axis of cylindrical magnet β central axis of optical isolator element θ optical isolator in design Element entrance / exit end face angle

Claims (3)

少なくとも2つの偏光子と1つのファラデー回転子を有しかつこれ等がその光透過面で貼り合わされて成る平行六面体形状の光アイソレータ素子と、この光アイソレータ素子が収容される円筒型磁石とを備え、上記偏光子の角部とファラデー回転子の角部を結んで形成される光アイソレータ素子の稜線部とその周辺部を円筒型磁石の内壁に接着させて光アイソレータ素子が円筒型磁石内に固定されている光アイソレータの製造方法において、
上記光アイソレータ素子を円筒型磁石内に挿入した後、光アイソレータ素子の隣り合う2つの上記稜線部とその周辺部にのみ接着剤を塗布して、光アイソレータ素子の上記2つの稜線部とその周辺部のみを円筒型磁石の内壁に接着させることを特徴とする光アイソレータの製造方法。
A parallelepiped-shaped optical isolator element having at least two polarizers and one Faraday rotator and bonded to each other at a light transmitting surface thereof, and a cylindrical magnet accommodating the optical isolator element. The edge of the optical isolator element formed by connecting the corner of the polarizer and the corner of the Faraday rotator and the peripheral portion thereof are adhered to the inner wall of the cylindrical magnet, and the optical isolator is fixed in the cylindrical magnet. In a method for manufacturing an optical isolator,
After the optical isolator element is inserted into the cylindrical magnet, an adhesive is applied only to the two adjacent ridges of the optical isolator element and the periphery thereof, and the two ridges of the optical isolator element and the periphery thereof are applied. A method of manufacturing an optical isolator, wherein only a portion is adhered to an inner wall of a cylindrical magnet.
上記接着剤が熱硬化型接着剤で構成され、かつ、塗布作業中における熱硬化型接着剤の粘度が0.6Pa・s以上1.7Pa・s以下であることを特徴とする請求項1に記載の光アイソレータの製造方法。   2. The method according to claim 1, wherein the adhesive is a thermosetting adhesive, and the viscosity of the thermosetting adhesive during the coating operation is 0.6 Pa · s or more and 1.7 Pa · s or less. A manufacturing method of the optical isolator according to the above. 少なくとも2つの偏光子と1つのファラデー回転子を有しかつこれ等がその光透過面で貼り合わされて成る平行六面体形状の光アイソレータ素子と、この光アイソレータ素子が収容される円筒型磁石とを備え、上記偏光子の角部とファラデー回転子の角部を結んで形成される光アイソレータ素子の稜線部とその周辺部を円筒型磁石の内壁に接着させて光アイソレータ素子が円筒型磁石内に固定されている光アイソレータにおいて、
光アイソレータ素子の隣り合う2つの上記稜線部とその周辺部のみが円筒型磁石の内壁に接着されていることを特徴とする光アイソレータ。
A parallelepiped-shaped optical isolator element having at least two polarizers and one Faraday rotator and bonded to each other at a light transmitting surface thereof, and a cylindrical magnet accommodating the optical isolator element. The ridge of the optical isolator element formed by connecting the corner of the polarizer and the corner of the Faraday rotator and the periphery thereof are adhered to the inner wall of the cylindrical magnet, and the optical isolator is fixed in the cylindrical magnet. Optical isolator
An optical isolator characterized in that only two adjacent ridge portions and a peripheral portion of the optical isolator element are bonded to the inner wall of the cylindrical magnet.
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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH03107915A (en) * 1989-09-22 1991-05-08 Matsushita Electric Ind Co Ltd Optical isolator
JPH06265819A (en) * 1993-03-10 1994-09-22 Tokin Corp Optical isolator
JP2001125043A (en) * 1999-10-28 2001-05-11 Kyocera Corp Optical isolator
JP2003005131A (en) * 2001-06-26 2003-01-08 Fdk Corp Optical isolator
JP2008129145A (en) * 2006-11-17 2008-06-05 Sumitomo Metal Mining Co Ltd Optical isolator element, optical isolator, and method for manufacturing them
US20120194906A1 (en) * 2009-04-09 2012-08-02 Trumpf Laser Gmbh + Co. Kg Optical insulator with parallelepiped magnets
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CN105137622A (en) * 2015-10-19 2015-12-09 无限光通讯(深圳)有限公司 Angle fixing method for internal optical chip of free space isolator

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