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JP7037135B2 - Optical isolator and its manufacturing method - Google Patents

Optical isolator and its manufacturing method Download PDF

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JP7037135B2
JP7037135B2 JP2018114322A JP2018114322A JP7037135B2 JP 7037135 B2 JP7037135 B2 JP 7037135B2 JP 2018114322 A JP2018114322 A JP 2018114322A JP 2018114322 A JP2018114322 A JP 2018114322A JP 7037135 B2 JP7037135 B2 JP 7037135B2
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optical isolator
cylindrical magnet
isolator element
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JP2019219435A (en
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和啓 峯島
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株式会社Smmプレシジョン
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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 optical communication, an optical information system, etc., and in particular, an optical isolator in which an optical element is adhesively fixed in a through hole of a cylindrical magnet by using an adhesive. It relates to the 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。 The optical isolator is generally composed of a Faraday rotator, a permanent magnet for saturating the Faraday rotator, an incident side polarizing element, and an emitted side polarizing element. Further, as for the Faraday rotator, one in which the plane of polarization of light is adjusted to rotate by 45 degrees by adjusting the thickness of the Faraday rotator itself 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 polarizing element and entered in the forward direction with respect to the Faraday rotator is transmitted through the Faraday rotator so that the polarization plane of the incident linearly polarized light is rotated by 45 degrees. It transmits the emitting side polarizing element adjusted so that the amount of transmitted light is maximized at the rotation position. Therefore, it is transmitted to the next optical system as light with 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。 Further, in the optical isolator, when there is reflected return light, the plane of polarization of the linearly polarized light that has passed through the emitter on the emitting side is rotated by 45 degrees by passing through the Faraday rotator, so that the plane of polarization is orthogonal to the splitter on the incident side. It is extinguished because it becomes. In this way, the function of the optical isolator is fulfilled.

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。 By the way, in an optical isolator, an antireflection film is applied to the surface of each optical element such as a Faraday rotator, an incident side polarizing element, and an emitted side polarizing element, and each optical element is integrated with an adhesive (optical isolator). (Called an element) is often used. Although the antireflection film is applied to the entrance / exit end faces of each optical element, light is slightly reflected on the entrance / exit end faces of each optical element to prevent the reflected light from returning to the original optical path. Therefore, the input / output end surface of the optical isolator element may be intentionally tilted several degrees from the surface 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。 Then, as a method of inclining the input / output end surface 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 surface is inclined with respect to a plane perpendicular to the optical axis. A method of producing an optical isolator element having a parallel quadrilateral shape (see Patent Document 2) and adhering the optical isolator element to the inside of a through hole of a cylindrical magnet is known.

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 that it does not require a holder compared to 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 the plane perpendicular to the optical axis. The end face angle sometimes deviated from the setting at the time of design.

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 input / output end surface angle 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 the 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)JP-A-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 by paying attention to such a problem, and the problem is that an optical isolator element is provided in a through hole of a cylindrical magnet at an input / exit end face angle as designed without using a holder. It is an object of the present invention to provide an optical isolator that can be bonded and fixed, and a method for 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。 Therefore, in order to solve the above problems, the present inventor sets the entrance / exit end face angle of the optical isolator element with respect to the plane perpendicular to the optical axis at the time of design when the optical isolator element is bonded 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 bonded inside a through hole of a cylindrical magnet, in consideration of symmetry, the four ridges of the optical isolator element located near the inner wall surface (inner wall surface of the through hole) of the cylindrical magnet ( The four ridges of the optical isolator element formed by connecting the corners of the polarizing element and the corners of the Faraday rotator) and their peripheral parts 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 (inner diameter of the through hole) is set to a slightly larger tolerance so that the optical isolator element can be securely 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 becomes large. Therefore, when the four ridges of the optical isolator element 10 having a parallelepiped shape and the peripheral portions thereof are bonded to the inner wall of the cylindrical magnet 1, the adhesive 20 is used as shown in FIGS. 3 (a) to 3 (b). It is difficult to control the shrinkage direction (the direction of hardening and shrinkage is indicated by an arrow in FIGS. 3a to 3b) due to non-uniform hardening shrinkage, and the central axis β of the optical isolator element 10 and the central 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 with each other and are overlapped or parallel to each other). As a result, the entrance / exit end face angle of the optical isolator element 10 with respect to the plane perpendicular to the optical axis P shown in FIG. 1 (d) is set at the time of design (the entrance / exit end face angle of the optical isolator element is set to θ at the time of design). It turned out that it deviated from. The present invention has been completed by such investigation 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
It comprises a parallel hexahedron-shaped optical isolator element having at least two polarizing elements and one Faraday rotator and bonded to each other on the light transmitting surface thereof, and a cylindrical magnet in which the optical isolator element is housed. The optical isolator element is fixed in the cylindrical magnet by adhering the ridgeline portion and its peripheral portion of the optical isolator element formed by connecting the corners of the polarizing element and the corners of the Faraday rotator to the inner wall of the cylindrical magnet. In the method of manufacturing an optical isolator,
After inserting the optical isolator element into the cylindrical magnet, the adhesive is applied only to the two adjacent ridges of the optical isolator element and their peripheral portions, and then the adhesive is applied only to the two adjacent ridges of the optical isolator element and their surroundings. It is characterized by adhering only the part 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 the coating operation 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, the third invention according to the present invention is
It comprises a parallel hexahedron-shaped optical isolator element having at least two polarizing elements and one Faraday rotator and bonded to each other on the light transmitting surface thereof, and a cylindrical magnet in which the optical isolator element is housed. The optical isolator element is fixed in the cylindrical magnet by adhering the ridgeline portion and its peripheral portion of the optical isolator element formed by connecting the corners of the polarizing element and the corners of the Faraday rotator to the inner wall of the cylindrical magnet. In the optical isolator
It is characterized in that only the two adjacent ridges of the optical isolator element and their peripheral portions are adhered 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 inserting the optical isolator element into the cylindrical magnet, the adhesive is applied only to the two adjacent ridges of the optical isolator element and their peripheral parts, and only the above two ridges of the optical isolator element and their peripheral parts are applied. Is adhered to the inner wall of the cylindrical magnet, so that the shrinkage direction when the adhesive is cured and shrunk can be limited to substantially one direction. Therefore, since it is unlikely that the central axis of the optical isolator element and the central axis of the cylindrical magnet intersect each other, it is possible to suppress the deviation of the input / output end face angle 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。1 (a) is a front view of the optical isolator according to the present invention, FIG. 1 (b) is a schematic cross-sectional view taken along the line AA'in FIG. 1 (a), and FIG. 1 (c) is an optical isolator according to the present invention. 1 (d) is an explanatory view of an entrance / exit end face angle (θ) at the time of design with respect to a plane perpendicular to the optical axis P of the optical isolator element 10 fixed to the 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 input / exit end face angle (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. In the graph showing the relationship with the input / output end face angle (angle after assembly), the reference numeral ◇ indicates that two adjacent ridges of an optical isolator element having a parallelepiped shape and their peripheral portions are adhered to the inner wall of a cylindrical magnet. The relationship between the tip angle and the post-assembly angle of the optical isolator (adhesion of two ridges) is shown. The relationship between the tip angle of the optical isolator (adhesion of four ridges) 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 peripheral portions of an 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 of an optical isolator element having a parallelepiped shape and their peripheral portions 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 according to 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 inserted into a cylindrical magnet 1 having a circular through hole and a through hole of the cylindrical magnet 1 as shown in FIGS. 1 (a) to 1 (d). It is composed of the optical isolator element 10 and the 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 polarizing element 2 on the side where light is incident, a Faraday rotator 3 and a second polarizing element 4 on the side where light is emitted, and these are attached by using an optical adhesive. It has a combined parallelepiped shape. Further, only the two adjacent positions of the ridge line formed by connecting the corners of the first splitter 2 and the corners of the Faraday rotator 3 and the corners of the second splitter 4 and their peripheral portions are cylindrical magnets. It is adhesively fixed to the inner wall of 1.

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。 The parallelepiped means a hexahedron in which three sets of opposing faces are parallel to each other.

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。 In the optical isolator according to the present invention, as shown in FIGS. 4A to 4B, only two adjacent ridges of the optical isolator element 10 and their peripheral portions are adhered to the inner wall of the cylindrical magnet 1. Therefore, it is possible to control the shrinkage direction (the curing shrinkage direction is indicated by an arrow in FIGS. 4a to 4b) when the adhesives 5 and 6 are cured and shrunk in substantially one direction. Therefore, it is unlikely that the central axis β of the optical isolator element 10 and the central axis α of the cylindrical magnet 1 intersect each other (the central axis β of the optical isolator element 10 and the central axis α of the cylindrical magnet 1 are substantially parallel to each other. Therefore, it is possible to suppress the deviation of the input / output end surface angle of the optical isolator element 10 with respect to the surface 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 as the conventional one can be used as the optical isolator element and the cylindrical magnet.

(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 an optical isolator element having a parallel hexahedron shape having at least two deflectors and one Faraday rotator and these being bonded to each other on the light transmitting surface, "for a single type optical isolator". "Optical element" (polarizer / Faraday rotator / deflector), "Double type optical element for optical isolator" (polarizer / Faraday rotator / modulator / deflector / Faraday rotator / Faraday rotator), and "semi-double type optical element for optical isolator" (Faraday rotator / Faraday rotator / Faraday rotator / Faraday rotator) and the like are exemplified.

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。 The shape of the optical isolator element 10 is a parallelepiped (a pair of facing faces having a parallelepiped shape) shown in FIG. 1D, which is composed of a polarizing element having a parallel quadrilateral cross section and a Faraday rotor. , The remaining two pairs of faces facing each other have a square or rectangular shape), or a parallelepiped (cube or rectangular parallelepiped shape) 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) Method for manufacturing an optical isolator Next, a method for manufacturing an 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 placed on a mounting table having a V-groove or the like 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 come into contact with 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 in contact with the inner wall of the through hole of the cylindrical magnet and their peripheral portions 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 will flow without staying in the vicinity of the ridgeline portion of the optical isolator element, and it will be difficult to bond the two adjacent ridgeline portions of the optical isolator element and their peripheral portions. 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 peripheral portion thereof, and as a result, the adhesive area becomes small and sufficient adhesive strength is obtained. Will be difficult. As the type of adhesive to be applied, either a thermosetting type adhesive or an ultraviolet curable type 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 mixed type adhesive is applied, the viscosity increases with the passage of time after mixing the main agent and the curing agent, so that the viscosity becomes 0.6 Pa · s or more and 1.7 Pa · s or less. It is preferable to finish the adhesive application work 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。 The 11 mm square first and Faraday rotators and second stators are bonded in advance with an adhesive, and the optical element is cut with a dicing saw according to the method for manufacturing an optical element described in Patent Document 2, and the light transmitting surface is formed. An optical isolator element having a size of 1.4 mm square was manufactured. The light transmitting surface of the optical isolator element is tilted by 6 ± 0.5 degrees from the 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。 Further, 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 placed on a mounting table on which a V-groove was formed so that the 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。 Next, a commercially available thermosetting epoxy adhesive (manufactured by Daizo Co., Ltd., model number:) was applied to the two adjacent ridges of the optical isolator element in contact with the inner wall of the through hole of the cylindrical magnet and their peripheral portions using a dispenser. NB3200) was applied. The initial viscosity of this adhesive before curing was 0.66 Pa · s. The adhesive used in this example was a two-component mixed type adhesive, and the viscosity increased with time, but the viscosity at the end of the adhesive application work 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。 Further, for comparison, an optical isolator according to a comparative example was also produced in which an adhesive was applied to and cured the four ridges of the optical isolator element, which are the same as those in the example, and their peripheral portions.

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 shows a graph comparing the angles of the light transmitting surfaces with respect to the end faces of the cylindrical magnets of the optical isolator elements according to the examples and the comparative examples. Since the end face of the cylindrical magnet is installed perpendicular to the optical axis, the angle of the light transmitting surface of the optical isolator element with respect to the end face of the cylindrical magnet is the angle of the entrance / exit end face of the optical isolator element with respect to the surface perpendicular to the optical axis. Is the same as. Further, in FIG. 2, the reference numeral ◇ indicates the chip angle and the post-assembly of the optical isolator (adhesion of two ridges) according to the embodiment in which the two adjacent ridges of the optical isolator element and their peripheral portions are bonded to the inner wall of the cylindrical magnet. The symbol □ indicates the relationship with the angle, and the chip angle and the post-assembly angle of the optical isolator (4 ridge line bonding) according to the comparative example in which the four ridges of the optical isolator element and their peripheral parts are bonded to the inner wall of the cylindrical magnet. The relationship with each is shown.

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 reference numeral ◇ is relative to the input / output end surface angle (6 ± 0.5 degrees described above) at the time of design. It is within the range of ± 1 degree. On the other hand, it was confirmed that the angle of the light transmitting surface with respect to the cylindrical magnet end face of the optical isolator according to the comparative example indicated by the symbol □ deviates by 5 degrees from the input / output end face angle (6 ± 0.5 degrees) at the time of design. Ru.

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 adhered and fixed in the through hole of the cylindrical magnet at the input / output end face angle as designed without using a holder by the method for manufacturing an optical isolator 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。 According to the optical isolator according to the present invention, since the deviation of the input / output end face angle of the optical isolator element with respect to the plane perpendicular to the optical axis is suppressed, it is an industry incorporated in semiconductor modules used in optical communication, optical information systems, and the like. 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
1 Cylindrical magnet 2 1st splitter 3 Faraday rotator 4 2nd splitter 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 at design time Input / output end face angle of the element

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。
It comprises a parallel hexahedron-shaped optical isolator element having at least two polarizing elements and one Faraday rotator and bonded to each other on the light transmitting surface thereof, and a cylindrical magnet in which the optical isolator element is housed. The optical isolator element is fixed in the cylindrical magnet by adhering the ridgeline portion and its peripheral portion of the optical isolator element formed by connecting the corners of the polarizing element and the corners of the Faraday rotator to the inner wall of the cylindrical magnet. In the method of manufacturing an optical isolator,
After inserting the optical isolator element into the cylindrical magnet, the adhesive is applied only to the two adjacent ridges of the optical isolator element and their peripheral portions, and then the adhesive is applied only to the two adjacent ridges of the optical isolator element and their surroundings. A method for manufacturing an optical isolator, which comprises adhering only a portion to the 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。 The first aspect of the present invention is that the adhesive is composed of 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. The method for manufacturing an optical isolator according to the description. 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。
It comprises a parallel hexahedron-shaped optical isolator element having at least two polarizing elements and one Faraday rotator and bonded to each other on the light transmitting surface thereof, and a cylindrical magnet in which the optical isolator element is housed. The optical isolator element is fixed in the cylindrical magnet by adhering the ridgeline portion and its peripheral portion of the optical isolator element formed by connecting the corners of the polarizing element and the corners of the Faraday rotator to the inner wall of the cylindrical magnet. In the optical isolator
An optical isolator characterized in that only the two adjacent ridges of the optical isolator element and their peripheral portions are adhered to the inner wall of the cylindrical magnet.
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