JPH05341230A - Optical isolator - Google Patents

Optical isolator

Info

Publication number
JPH05341230A
JPH05341230A JP16992692A JP16992692A JPH05341230A JP H05341230 A JPH05341230 A JP H05341230A JP 16992692 A JP16992692 A JP 16992692A JP 16992692 A JP16992692 A JP 16992692A JP H05341230 A JPH05341230 A JP H05341230A
Authority
JP
Japan
Prior art keywords
polarization
optical
polarized light
plane
rotator
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
JP16992692A
Other languages
Japanese (ja)
Inventor
Kazuhiro Nakajima
和宏 中島
Hiroo Numajiri
裕夫 沼尻
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.)
Sumitomo Metal Mining Co Ltd
Original Assignee
Sumitomo Metal Mining Co 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 Sumitomo Metal Mining Co Ltd filed Critical Sumitomo Metal Mining Co Ltd
Priority to JP16992692A priority Critical patent/JPH05341230A/en
Publication of JPH05341230A publication Critical patent/JPH05341230A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To obtain the optical isolator of a polarized wave non-dependence type by disposing in order a Faraday rotator and a polarized light rotator on two optical paths between two elements. CONSTITUTION:A plane of polarization of polarized light components of two optical paths (a), (b) rotates by 90 degrees against a plane of polarization in a state separted at the time of incidence by a Faraday rotator 7 and a polarized light rotator 8, therefore, is not synthesized in a polarized light separating/ synthesizing element 4 of an incident side. In this case, the polarized light component of the optical path (a) is reflected by a reflecting prism 6 for constituting the element 4, passes through a polarized beam splitter 5 as it is and is emitted in the direction for making an angle of 90 degrees against an optical axis of an incident light, therefore, does not return to the incident side. Also, the polarized light component of the optical path (b) is reflected by the splitter 5 for constituting the element 4, and emitted in the direction for making 90 degrees against the optical axis of the incident light in the same as the polarized light component of the optical path (a), therefore, does not return to the incident side. In such a way, a function as the optical isolator is displayed without considering entirely the plane of polarization of an incident light.

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、光アイソレータ、特に
入射光の偏光面を考慮することなく作動しうるようにし
た偏波無依存型光アイソレータに関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an optical isolator, and more particularly to a polarization independent optical isolator which can operate without considering the polarization plane of incident light.

【0002】[0002]

【従来の技術】図2は従来の光アイソレータの構成例を
示している。この光アイソレータでは入射光が第一の偏
光子1を通過した後にファラデー回転子2によってその
偏光面が45度回転し、更に該第一の偏光子1に対して
45度傾いた偏光面を有する第二の偏光子3を通過す
る。一方、上記入射光とは逆方向の反射戻り光は第二の
偏光子3に対して偏光面が一致した成分のみが該第二の
偏光子3を通過し、この後上記ファラデー回転子2によ
ってその偏光面が更に45度回転する。従って、ファラ
デー回転子2を通過したかかる反射戻り光は第一の偏光
子1に対してその偏光面が90度回転していることにな
り、これにより、上記入射光の入射側までには到達する
ことができなくなる。このように従来の光アイソレータ
によれば上記逆方向の反射戻り光が遮断され、この種の
光アイソレータ機能が発揮される。
2. Description of the Related Art FIG. 2 shows a configuration example of a conventional optical isolator. In this optical isolator, after the incident light passes through the first polarizer 1, the Faraday rotator 2 rotates its polarization plane by 45 degrees, and further has a polarization plane inclined by 45 degrees with respect to the first polarizer 1. It passes through the second polarizer 3. On the other hand, in the reflected return light in the opposite direction to the incident light, only the component whose polarization plane matches that of the second polarizer 3 passes through the second polarizer 3, and then the Faraday rotator 2 The plane of polarization is further rotated 45 degrees. Therefore, the reflected return light that has passed through the Faraday rotator 2 has its polarization plane rotated by 90 degrees with respect to the first polarizer 1, and thereby reaches the incident side of the incident light. Can not do. As described above, according to the conventional optical isolator, the reflected return light in the opposite direction is blocked, and this type of optical isolator function is exhibited.

【0003】[0003]

【発明が解決しようとする課題】しかしながら、かかる
従来の光アイソレータでは、入射光の偏光面に対して第
一の偏光子1の偏光面を一致させておく必要があるた
め、特に偏光面を予め特定することができない光伝送系
においては、その機能を有効に発揮することができない
という問題があった。これは入射光の偏光面の傾きに依
存せざるを得ない構造になっているためである。
However, in such a conventional optical isolator, it is necessary to match the polarization plane of the first polarizer 1 with the polarization plane of the incident light. In the optical transmission system which cannot be specified, there is a problem that the function cannot be effectively exhibited. This is because the structure has no choice but to depend on the inclination of the polarization plane of the incident light.

【0004】本発明はこのような実情に鑑み、入射光の
偏光面を全く考慮することなく光アイソレータとしての
機能が発揮されるようにした偏波無依存型の光アイソレ
ータを提供することを目的とする。
In view of the above situation, it is an object of the present invention to provide a polarization-independent optical isolator capable of exerting its function as an optical isolator without considering the plane of polarization of incident light. And

【0005】[0005]

【課題を解決するための手段】上記目的を達成するた
め、本発明の光アイソレータは、任意の偏光面を有する
偏光を、互いに90度の角度をなす偏光面を持つ2つの
偏光に分離すると共に一方の偏光は入射光と同一の光軸
で出射し、他方の偏光は該光軸と並行な別の光軸で出射
する偏光分離・合成素子一対を対向配置し、該2素子間
の2光路上にファラデー回転子及び偏光回転子を順に配
設した点に特徴がある。
In order to achieve the above object, the optical isolator of the present invention splits a polarized light having an arbitrary polarization plane into two polarizations having polarization planes forming an angle of 90 degrees with each other. One polarized light is emitted on the same optical axis as the incident light, and the other polarized light is emitted on another optical axis parallel to the optical axis. It is characterized in that a Faraday rotator and a polarization rotator are sequentially arranged on the road.

【0006】[0006]

【作用】本発明によれば任意の偏光面を有する入射光は
先ず入射側の偏光分離・合成素子によって互いに90度
の角度をなす偏光面を有する二つの偏光に分離される。
次に、ファラデー回転子によって各々の光路の偏光成分
の偏光面が45度回転した後、偏光回転子によってさら
に45度、合計90度回転するためかかる二つの偏光成
分は出射側の偏光分離・合成素子により合成される。
According to the present invention, the incident light having an arbitrary polarization plane is first separated by the polarization separating / combining element on the incident side into two polarized lights having polarization planes forming an angle of 90 degrees with each other.
Next, the Faraday rotator rotates the polarization plane of the polarization component of each optical path by 45 degrees, and then the polarization rotator further rotates by 45 degrees, for a total of 90 degrees, so these two polarization components are separated / combined on the output side. It is synthesized by the element.

【0007】他方、任意の偏光面を有する逆方向の光は
まず出射側の偏光分離・合成素子により特定の偏光面を
有する二つの光路に分離される。次に偏光回転子によっ
てその偏光面が45度回転した後、ファラデー回転子に
よって再びもとの偏光面にそれぞれもどされる。そのた
めかかる二つの光路の偏光面は入射時に分離された状態
の偏光面に対して90度回転していることになり、入射
側の偏光分離・合成素子において合成されることはな
く、入射光の光軸と90度をなす方向に出射されるので
入射側へは戻らない。
On the other hand, light in the opposite direction having an arbitrary polarization plane is first split into two optical paths having a specific polarization plane by the polarization splitting / combining element on the output side. Then, the plane of polarization is rotated by 45 degrees by the polarization rotator, and then returned to the original plane of polarization by the Faraday rotator. Therefore, the polarization planes of these two optical paths are rotated by 90 degrees with respect to the polarization planes separated at the time of incidence, and are not combined by the polarization separation / combining element on the incident side. Since the light is emitted in a direction forming 90 degrees with the optical axis, it does not return to the incident side.

【0008】[0008]

【実施例】以下、図1は本発明の光アイソレータの1構
成例を示す図である。図の上段は各素子の配列を表すと
共に入射光の光路を示し、中上段は入射光の各段階にお
ける偏光面の変化を示し、中下段及び下段は同様に戻り
光についてのものである。まず図1において、4は偏光
ビームスプリッタ5及び反射プリズム6から成る偏光分
離・合成素子である。また、7はファラデー回転子であ
り8はλ/2板より成る偏光回転子である。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS FIG. 1 is a diagram showing one structural example of an optical isolator according to the present invention. The upper part of the figure shows the arrangement of each element and shows the optical path of the incident light, the middle upper part shows the change of the polarization plane at each stage of the incident light, and the middle lower part and the lower part are for return light. First, in FIG. 1, reference numeral 4 is a polarization splitting / combining element including a polarization beam splitter 5 and a reflecting prism 6. Further, 7 is a Faraday rotator, and 8 is a polarization rotator composed of a λ / 2 plate.

【0009】上記の場合、入射光はまず偏光分離・合成
素子4を構成する偏光ビームスプリッタ5の作用により
互いに90度の角度をなす特定な偏光面を有する二つの
偏光に分離される。このとき二つの偏光のうち一方は入
射光と同一の光軸を持つ光路bを、他方は光路bと90
度の角度をなす光軸を有する光路aを進行する。
In the above case, the incident light is first split into two polarized lights having specific polarization planes forming an angle of 90 degrees by the action of the polarization beam splitter 5 constituting the polarization splitting / combining element 4. At this time, one of the two polarizations is the optical path b having the same optical axis as the incident light, and the other is the optical paths b and 90.
The optical path a having an optical axis forming an angle of degrees is advanced.

【0010】光路aには偏光分離・合成素子4を構成す
る反射プリズム6が配設されており、光路aを進行する
偏光は反射プリズム6によって反射されて光路bと平行
な光軸を有する偏光となる。すなわち入射光は偏光分離
・合成素子4によって、互いに90度の角度をなす特定
な偏光面をもち入射光に平行な光軸をもつ二つの光路
a,bの偏光成分に分離されたことになる。
A reflecting prism 6 which constitutes the polarization splitting / combining element 4 is disposed on the optical path a, and the polarized light traveling on the optical path a is reflected by the reflecting prism 6 and has a light axis parallel to the optical path b. Becomes That is, the incident light is separated by the polarization separating / combining element 4 into polarized light components of two optical paths a and b having specific polarization planes forming an angle of 90 degrees with each other and having an optical axis parallel to the incident light. .

【0011】次に、これら分離された2つの偏光成分は
上記ファラデー回転子7によって偏光面が45度回転
し、偏光回転子8によってさらに45度回転、合計90
度回転する。その結果光路a,bの偏光成分の偏光面は
分離された状態とちょうど入れ替わった状態になる。し
たがって光路a,bの偏光成分は入射側の偏光分離・合
成素子4と同様に構成されて成る出射側の偏光分離・合
成素子4によって合成され出射する。
Next, the polarization planes of the two separated polarization components are rotated by 45 degrees by the Faraday rotator 7 and further rotated by 45 degrees by the polarization rotator 8 for a total of 90 degrees.
Rotate once. As a result, the polarization planes of the polarization components of the optical paths a and b are in a state where they are just replaced with the separated states. Therefore, the polarization components of the optical paths a and b are combined by the polarization separating / combining element 4 on the exit side, which is configured in the same manner as the polarization separating / combining element 4 on the incident side, and is emitted.

【0012】他方、出射側より入射する戻り光は、まず
偏光分離・合成素子4の作用により互いに90度の角度
をなす特定な偏光面をもつ二つの光路a,bの偏光成分
に分離される。そして、偏光回転子8の作用によって偏
光面が45度回転し、ファラデー回転子7によって再び
もとの偏光面にそれぞれ戻される。
On the other hand, the return light entering from the exit side is first separated by the action of the polarization splitting / combining element 4 into polarization components of two optical paths a and b having specific polarization planes forming an angle of 90 degrees with each other. . Then, the polarization plane is rotated by 45 degrees by the action of the polarization rotator 8, and is returned to the original polarization plane again by the Faraday rotator 7.

【0013】したがってかかる二つの光路a,bの偏光
成分の偏光面は入射時に分離された状態の偏光面に対し
て90度回転していることになり、入射側の偏光分離・
合成素子4において合成されることはない。このとき光
路aの偏光成分は偏光分離・合成素子4を構成する反射
プリズム6によって反射され、偏光ビームスプリッタ5
をそのまま通過して入射光の光軸と90度をなす方向に
出射されるので入射側へは戻らない。また、光路bの偏
光成分は偏光分離・合成素子4を構成する偏光ビームス
プリッタ5によって反射され、光路aの偏光成分と同様
に入射光の光軸と90度をなす方向に出射されるので入
射側へは戻らない。
Therefore, the polarization planes of the polarization components of the two optical paths a and b are rotated by 90 degrees with respect to the polarization planes separated at the time of incidence.
It is not combined in the combining element 4. At this time, the polarization component of the optical path a is reflected by the reflection prism 6 that constitutes the polarization splitting / combining element 4, and the polarization beam splitter 5
The light does not return to the incident side because it passes through as it is and is emitted in a direction forming 90 degrees with the optical axis of the incident light. Further, the polarization component of the optical path b is reflected by the polarization beam splitter 5 constituting the polarization separation / combination element 4, and is emitted in the direction forming an angle of 90 degrees with the optical axis of the incident light like the polarization component of the optical path a. Do not go back to your side.

【0014】[0014]

【発明の効果】このように本発明によれば、入射光の偏
光面が予め特定できないような光伝送系であっても偏光
面の状態を考慮することなく光アイソレータとしての機
能を十分有効に発揮させることができるので実用的効果
の点でも優れている。また、空間ビーム光や光ファイバ
ー用として利用することができるのはもちろんである
が、その場合に既存の光アイソレータと簡単に置換する
ことが可能であり、工業上極めて有用である。
As described above, according to the present invention, even in an optical transmission system in which the plane of polarization of incident light cannot be specified in advance, the function as an optical isolator is sufficiently effective without considering the state of the plane of polarization. Since it can be demonstrated, it is also excellent in practical effects. In addition, it can be used as a space beam light or an optical fiber, but in that case, it can be easily replaced with an existing optical isolator, which is extremely useful industrially.

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

【図1】本発明の光アイソレータの構成例を示す図であ
る。
FIG. 1 is a diagram showing a configuration example of an optical isolator of the present invention.

【図2】従来の光アイソレータの構成例を示す図であ
る。
FIG. 2 is a diagram showing a configuration example of a conventional optical isolator.

【符号の説明】[Explanation of symbols]

1 第一の偏光子 2 ファラデー回転子 3 第二の偏光子 4 偏光分離・合成素子 5 偏光ビームスプリッタ 6 反射プリズム 7 ファラデー回転子 8 偏光回転子 1 First Polarizer 2 Faraday Rotor 3 Second Polarizer 4 Polarization Separation / Combining Element 5 Polarization Beam Splitter 6 Reflection Prism 7 Faraday Rotator 8 Polarization Rotator

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 任意の偏光面を有する偏光を、互いに9
0度の角度をなす偏光面を持つ2つの偏光に分離すると
共に一方の偏光は入射光と同一の光軸で出射し、他方の
偏光は該光軸と並行な別の光軸で出射する偏光分離・合
成素子一対を対向配置し、該2素子間の2光路上にファ
ラデー回転子及び偏光回転子を順に配設したことを特徴
とする光アイソレータ。
1. Polarized light beams having arbitrary planes of polarization are separated from each other by 9
A polarized light that is split into two polarized lights having a plane of polarization that forms an angle of 0 degree, and one polarized light is emitted on the same optical axis as the incident light, and the other polarized light is emitted on another optical axis parallel to the optical axis. An optical isolator, wherein a pair of separation / combination elements are arranged to face each other, and a Faraday rotator and a polarization rotator are sequentially arranged on two optical paths between the two elements.
JP16992692A 1992-06-05 1992-06-05 Optical isolator Pending JPH05341230A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP16992692A JPH05341230A (en) 1992-06-05 1992-06-05 Optical isolator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP16992692A JPH05341230A (en) 1992-06-05 1992-06-05 Optical isolator

Publications (1)

Publication Number Publication Date
JPH05341230A true JPH05341230A (en) 1993-12-24

Family

ID=15895509

Family Applications (1)

Application Number Title Priority Date Filing Date
JP16992692A Pending JPH05341230A (en) 1992-06-05 1992-06-05 Optical isolator

Country Status (1)

Country Link
JP (1) JPH05341230A (en)

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