JPS6362730B2 - - Google Patents

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Publication number
JPS6362730B2
JPS6362730B2 JP21801784A JP21801784A JPS6362730B2 JP S6362730 B2 JPS6362730 B2 JP S6362730B2 JP 21801784 A JP21801784 A JP 21801784A JP 21801784 A JP21801784 A JP 21801784A JP S6362730 B2 JPS6362730 B2 JP S6362730B2
Authority
JP
Japan
Prior art keywords
polarization
light
prism
polarizing prism
polarized 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.)
Expired
Application number
JP21801784A
Other languages
Japanese (ja)
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JPS6197629A (en
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 filed Critical
Priority to JP21801784A priority Critical patent/JPS6197629A/en
Publication of JPS6197629A publication Critical patent/JPS6197629A/en
Publication of JPS6362730B2 publication Critical patent/JPS6362730B2/ja
Granted legal-status Critical Current

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Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は偏光分離用偏光プリズムと偏光合成用
偏光プリズムを備えた光スイツチの改良に関する
ものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to an improvement of an optical switch equipped with a polarizing prism for separating polarized light and a polarizing prism for combining polarized light.

光デバイス用の偏光プリズムには、誘電体多層
膜を使用したものと複屈折結晶を使用したものと
があるが、前者は漏話が大きく(偏光分離度が悪
い)、後者は偏光の分離角度が小さく大きな結晶
を必要とする欠点があり、いずれも改善策が必要
である。
Polarizing prisms for optical devices include those that use dielectric multilayer films and those that use birefringent crystals, but the former has large crosstalk (poor polarization separation), and the latter has a large polarization separation angle. It has the disadvantage of requiring small and large crystals, both of which require improvement measures.

〔従来の技術〕[Conventional technology]

誘電体多層膜の偏光分離膜を備えた偏光プリズ
ムを使用した従来の光スイツチを第5図に示す。
図中、1は偏光分離用偏光プリズム、2は偏光合
成用偏光プリズム、31はこの両偏光プリズム1,
2の間に設けられた磁気光学結晶、32は1/2波長
板、41,42は出力側に設けられた光フアイバ等
の受光部である。磁気光学結晶31は、加わる磁
場が光の進行方向と同一の場合は偏波面を右方向
に45゜回転し逆方向の場合は偏波面を左方向に45゜
回転する。また1/2波長板32はつねに偏波面を左
方向に45゜回転する。各偏光プリズム1,2は、
誘電体多層膜の偏光分離膜5,6を備えている。
本図は磁気光学結晶31の磁場が矢印方向の場合
を示しており、この場合、光フアイバ7から偏光
プリズム1に入射する光ビーム8は、偏光プリズ
ム1により――↑↓――のP偏光9と―●―のS偏光1

とに分離され、磁気光学結晶31,1/2波長板32
を通り偏光面は回転されず偏光プリズム2に入射
する。偏光プリズム2に入射した光は、該偏光プ
リズム2により合成され、光ビームAとなつて受
光部42に入射し結合される。また、磁気光学結
晶31の磁場を本図と逆方向にした場合磁気光学
結晶31,1/2波長板32を通過した光は偏光面が
90゜回転され、偏光プリズム2により合成される
光ビームは受光部41に入射、結合される。
FIG. 5 shows a conventional optical switch using a polarizing prism equipped with a dielectric multilayer polarization separation film.
In the figure, 1 is a polarizing prism for separating polarized light, 2 is a polarizing prism for combining polarized light, 3 1 is a polarizing prism for both polarizing prisms 1,
2 is a magneto-optical crystal provided between the two, 3 2 is a 1/2 wavelength plate, and 4 1 and 4 2 are light receiving sections such as optical fibers provided on the output side. The magneto-optic crystal 31 rotates the plane of polarization by 45 degrees to the right when the applied magnetic field is in the same direction as the traveling direction of the light, and rotates the plane of polarization by 45 degrees to the left when the applied magnetic field is in the opposite direction. Further, the 1/2 wavelength plate 32 always rotates the plane of polarization by 45 degrees to the left. Each polarizing prism 1, 2 is
It is provided with polarization separation films 5 and 6 made of dielectric multilayer films.
This figure shows a case where the magnetic field of the magneto-optic crystal 31 is in the direction of the arrow. Polarized light 9 and S polarized light 1 of -●-
0
are separated into a magneto-optic crystal 3 1 and a 1/2 wavelength plate 3 2
The plane of polarization is not rotated and enters the polarizing prism 2. The light incident on the polarizing prism 2 is combined by the polarizing prism 2, becomes a light beam A, enters the light receiving section 42 , and is combined. In addition, when the magnetic field of the magneto-optic crystal 3 1 is set in the opposite direction to that shown in this figure, the light passing through the magneto-optic crystal 3 1 and the 1/2 wavelength plate 3 2 has a polarization plane.
The light beams rotated by 90 degrees and combined by the polarizing prism 2 are incident on and coupled to the light receiving section 4 1 .

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

ところが、偏光分離膜5,6の偏光分離度が悪
いため、P偏光9にS偏光成分が含まれ、逆にS
偏光10にP偏光成分が含まれてしまう。すなわ
ち漏話成分が生じる。従つてこのような構成の従
来の光スイツチにおいては、偏光合成用偏光プリ
ズムにより分離したP偏光9とS偏光10を合成
した合成光Aを一方の受光部に入射、結合する際
に漏話成分の光路が他方の受光部の光路に一致し
漏話が大きくなるという欠点があつた。すなわち
偏光分離膜6はP偏光9を反射し、S偏光10を
透過するが、P偏光9に含まれるS偏光(漏話成
分)は透過され、かつS偏光10に含まれるP偏
光(漏話成分)は反射し、合成された漏話成分B
として受光部41に入力される。つまり第5図に
点線で示す漏話成分Bは、偏光プリズム2による
合成光ビームを受光部41に入射、結合する場合
の(磁気光学結晶31の磁場を逆方向に向けた時)
光路を通るのである。
However, because the degree of polarization separation of the polarization separation films 5 and 6 is poor, the S polarization component is included in the P polarization 9, and conversely, the S polarization component is
The polarized light 10 contains a P-polarized light component. In other words, a crosstalk component occurs. Therefore, in the conventional optical switch having such a configuration, when the combined light A, which is a combination of the P polarized light 9 and the S polarized light 10 separated by the polarization combining polarizing prism, enters and combines into one light receiving section, the crosstalk component is removed. There was a drawback that the optical path coincided with the optical path of the other light receiving section, resulting in increased crosstalk. That is, the polarization separation film 6 reflects the P-polarized light 9 and transmits the S-polarized light 10, but the S-polarized light (crosstalk component) contained in the P-polarized light 9 is transmitted, and the P-polarized light (crosstalk component) contained in the S-polarized light 10 is transmitted. is reflected and synthesized crosstalk component B
It is input to the light receiving section 41 as follows. In other words, the crosstalk component B shown by the dotted line in FIG. 5 is obtained when the combined light beam from the polarizing prism 2 is incident on and coupled to the light receiving section 41 (when the magnetic field of the magneto-optic crystal 31 is directed in the opposite direction).
It passes through the optical path.

〔問題点を解決するための手段〕[Means for solving problems]

本発明は上述の問題点を解決できる光スイツチ
を提供することを目的としたもので、そのための
手段として、光の入射側に設けられた偏光分離用
偏光プリズムと光の出射側に設けられた偏光合成
用偏光プリズムとを備え、前記偏光合成用偏光プ
リズムで合成された光ビームを2つの受光部に選
択的に結合させる光スイツチにおいて、前記偏光
分離用偏光プリズムと前記偏光合成用偏光プリズ
ムの間に、合成光ビームを結合しない側の前記受
光部に漏話成分が結合しないように該漏話成分に
並進又は角度ずれを起させるための複屈折板を挿
入している。
The purpose of the present invention is to provide an optical switch capable of solving the above-mentioned problems, and as a means for that purpose, a polarizing prism for polarization separation provided on the light incidence side and a polarization prism provided on the light output side. an optical switch for selectively coupling a light beam combined by the polarization prism for polarization synthesis to two light receiving sections, wherein the polarization prism for polarization separation and the polarization prism for polarization synthesis are provided. In between, a birefringent plate is inserted to cause a translational or angular shift in the crosstalk component so that the crosstalk component is not coupled to the light receiving section on the side where the combined light beam is not coupled.

〔作用〕[Effect]

偏光プリズムで発生した光ビームの漏話成分
は、両偏光プリズム間に挿入された複屈折板によ
り並進又は角度ずれを起し、合成光ビームの光路
がずれるため受光部に結合しなくなる。
The crosstalk component of the light beam generated by the polarizing prism is translated or angularly shifted by a birefringent plate inserted between both polarizing prisms, and the optical path of the combined light beam is shifted, so that it is no longer coupled to the light receiving section.

〔実施例〕〔Example〕

以下、第1図乃至第4図に関連して本発明の実
施例を説明する。
Embodiments of the present invention will be described below with reference to FIGS. 1 to 4.

第1図は本発明に係る光スイツチの概要図で、
図中、11,12は水晶の波長板、13,14は
方解石又はルチル等の平板状複屈折板である。複
屈折板13は、C軸13aを備えた、P偏光とS
偏光とで屈折率が異なるものであり、偏光プリズ
ム1と磁気光学結晶31の間に挿入されている。
波長板11は、偏光プリズム1と複屈折板13の
間に複屈折板13の下方部分に対向させて挿入さ
れている。複屈折板14は、C軸14aを備え、
磁気光学結晶31と偏光プリズム2の間に挿入さ
れている。波長板12は、偏光プリズム2と複屈
折板14の間に複屈折板14の上方部分に対向さ
せて挿入されている。
FIG. 1 is a schematic diagram of an optical switch according to the present invention.
In the figure, 11 and 12 are crystal wave plates, and 13 and 14 are flat birefringent plates made of calcite, rutile, or the like. The birefringent plate 13 has a C-axis 13a, and is used for P-polarized light and S-polarized light.
It has a different refractive index depending on the polarized light, and is inserted between the polarizing prism 1 and the magneto-optic crystal 31 .
The wavelength plate 11 is inserted between the polarizing prism 1 and the birefringent plate 13 so as to face the lower part of the birefringent plate 13. The birefringent plate 14 has a C axis 14a,
It is inserted between the magneto-optic crystal 3 1 and the polarizing prism 2 . The wavelength plate 12 is inserted between the polarizing prism 2 and the birefringent plate 14 so as to face the upper part of the birefringent plate 14 .

いま、磁気光学結晶31の磁場を矢印方向にし
ておいて光フアイバ7から偏光プリズム1に光ビ
ーム15を入射させると、該光ビーム15は偏光
プリズム1により――↑↓――のP偏光16と―●―の

偏光17とに分離される。P偏光16は、波長板
11を通過する際に偏光面が90゜回転させられる
とともに、複屈折板13,14を通過する際に漏
話成分が点線で示すように屈折され並進ずれを生
じる。また、S偏光17は、複屈折板13,14
を通過する際に漏話成分が点線で示すように屈折
され並進ずれを起すとともに、波長板12を通過
する際に偏光面が90゜回転される。これらの光は
偏光プリズム2に入射し合成され光ビーム18と
なつて受光部42に入射し結合されるが、同時に
偏光プリズム2から上方に出射する漏話成分は上
述のように並進ずれを起しているための受光部4
の光路と一致せず該受光部41と結合されない。
Now, when the magnetic field of the magneto-optic crystal 31 is set in the direction of the arrow and a light beam 15 is made to enter the polarizing prism 1 from the optical fiber 7, the light beam 15 is converted into P-polarized light by the polarizing prism 1. 16 and -●- S
It is separated into polarized light 17. The polarization plane of the P-polarized light 16 is rotated by 90 degrees when passing through the wave plate 11, and the crosstalk component is refracted as shown by the dotted line when passing through the birefringence plates 13 and 14, causing a translational shift. Further, the S polarized light 17 is transmitted through the birefringent plates 13 and 14.
When passing through the wave plate 12, the crosstalk component is refracted as shown by the dotted line, causing a translational shift, and when passing through the wave plate 12, the plane of polarization is rotated by 90 degrees. These lights enter the polarizing prism 2 and are combined into the light beam 18, which enters the light receiving section 42 and is combined. At the same time, however, the crosstalk component that exits the polarizing prism 2 upward causes a translational shift as described above. Light receiving part 4 for
1 and is not coupled to the light receiving section 4 1 .

また、第2図に示すように磁気光学結晶31
磁場を上述と逆方向にしておいて光フアイバ7か
ら偏光プリズム1に光ビーム15を入射させた場
合は、偏光プリズム1により分離されたP偏光1
6、S偏光17は、複屈折板13を通過するまで
上述と同様に進むが、磁気光学結晶31及び1/2波
長板32を通過する際に偏光面が90゜回転される。
その後これらの光は、複屈折板14を通過する際
に屈折して漏話成分と光路が一致する。その後S
偏光17は波長板12により偏光方向を90゜変え
られる。この場合は、偏光プリズム2により合成
されて上方に出射する光ビーム19は受光部41
に入射し結合され、同時に偏光プリズム2から右
方に出射する漏話成分は受光部42と結合されな
い。
In addition, as shown in FIG. 2, when the magnetic field of the magneto-optic crystal 31 is set in the opposite direction to that described above and the light beam 15 is incident on the polarizing prism 1 from the optical fiber 7, the light beam 15 is separated by the polarizing prism 1. P polarized light 1
6. The S-polarized light 17 proceeds in the same manner as described above until it passes through the birefringent plate 13, but the plane of polarization is rotated by 90 degrees when passing through the magneto-optic crystal 3 1 and the 1/2 wavelength plate 3 2 .
Thereafter, these lights are refracted when passing through the birefringent plate 14, and their optical paths coincide with the crosstalk components. Then S
The polarization direction of the polarized light 17 can be changed by 90 degrees by the wave plate 12. In this case, the light beam 19 combined by the polarizing prism 2 and emitted upward is the light receiving part 4 1
A crosstalk component that enters and is coupled to the polarizing prism 2 and simultaneously exits to the right from the polarizing prism 2 is not coupled to the light receiving section 4 2 .

このように、偏光プリズムの偏光分離膜の漏話
が大きくても漏話成分が受光部に結合されないた
め、実質上漏話を低減することができる。
In this way, even if the crosstalk of the polarization separation film of the polarizing prism is large, the crosstalk component is not coupled to the light receiving section, so that crosstalk can be substantially reduced.

第3図及び第4図に応用例を示す。 Application examples are shown in FIGS. 3 and 4.

第3図の場合は、第1,2図の複屈折板13,
14の代りにC軸20,21を有するくさび型複
屈折板22,23を用いている。この場合は通過
光に角度ずれが起り、この角度ずれを利用して前
例と同様に漏話成分が受光部に結合されないよう
にすることができる。
In the case of Fig. 3, the birefringent plate 13 of Figs. 1 and 2,
14 is replaced by wedge-shaped birefringent plates 22 and 23 having C axes 20 and 21. In this case, an angular shift occurs in the passing light, and this angular shift can be used to prevent the crosstalk component from being coupled to the light receiving section as in the previous example.

第4図a,bの場合は、C軸24を有する1対
の平板状複屈折板25を対称に張り合せたもの
と、C軸26を有する1対の平板状複屈折板27
を対称に張り合せたものとを、張り合せ面をS偏
光28、P偏光29の2つの光路の中間に設けた
ものである。この場合の偏光分離用プリズムによ
り分離された各光の結合成分、漏話成分の経路は
磁気光学結晶に加わる磁界の向きによつて図示の
ようになる。本例の場合、波長板は不要である。
なお、各複屈折板をC軸のある平面が図の紙面に
対して垂直となるように配置しても良い。
In the case of FIGS. 4a and 4b, a pair of flat birefringent plates 25 having a C-axis 24 are laminated symmetrically, and a pair of flat birefringent plates 27 having a C-axis 26.
are symmetrically pasted together, and the joining surface is provided in the middle of the two optical paths of the S-polarized light 28 and the P-polarized light 29. In this case, the paths of the coupled components and crosstalk components of each light separated by the polarization separation prism are as shown in the figure, depending on the direction of the magnetic field applied to the magneto-optic crystal. In this example, a wave plate is not required.
Note that each birefringent plate may be arranged so that the plane with the C axis is perpendicular to the plane of the drawing.

〔発明の効果〕〔Effect of the invention〕

以上述べたように、本発明によれば、偏光分離
用偏光プリズムと偏光合成用偏光プリズムの間に
設けられた複屈折板等により偏光プリズム光ビー
ムの漏話成分に並進又は角度ずれが起り、これに
より漏話成分が受光部に結合されないため、実質
上漏話を低減することが可能である。
As described above, according to the present invention, a translational or angular shift occurs in the crosstalk component of the polarizing prism light beam due to the birefringence plate or the like provided between the polarizing prism for polarizing separation and the polarizing prism for combining polarized light. Since the crosstalk component is not coupled to the light receiving section, it is possible to substantially reduce crosstalk.

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

第1図乃至第4図は本発明に係る光スイツチの
実施例を示すもので、第1図は光スイツチの構
成、作用説明図、第2図は磁気光学結晶の磁場方
向を第1図と逆にした場合の光スイツチの作用説
明図、第3図及び第4図は光スイツチの応用例を
示す構成、作用説明図である。第5図は従来の光
スイツチの構成、作用説明図である。 図中、1は偏光分離用偏光プリズム、2は偏光
合成用偏光プリズム、31は磁気光学結晶、32
1/2波長板、41,42は受光部、5,6は偏光分
離膜、7は光フアイバ、11,12は波長板、1
3,14,22,23,25,27は複屈折板、
20,21,24,26はC軸である。
1 to 4 show an embodiment of the optical switch according to the present invention. FIG. 1 shows the structure and operation of the optical switch, and FIG. 2 shows the direction of the magnetic field of the magneto-optic crystal. FIGS. 3 and 4 are explanatory views of the operation of the optical switch when the optical switch is reversed. FIGS. FIG. 5 is an explanatory diagram of the structure and operation of a conventional optical switch. In the figure, 1 is a polarizing prism for polarization separation, 2 is a polarization prism for polarization synthesis, 3 1 is a magneto-optic crystal, 3 2 is a half-wave plate, 4 1 and 4 2 are light receiving parts, and 5 and 6 are polarization separation parts. 7 is an optical fiber, 11 and 12 are wavelength plates, 1
3, 14, 22, 23, 25, 27 are birefringent plates,
20, 21, 24, and 26 are C axes.

Claims (1)

【特許請求の範囲】 1 光の入射側に設けられ、入射光を2つの偏光
に分離する偏光分離用偏光プリズム1と、該偏光
分離用偏光プリズムにより分離された2つの偏光
の偏光面を夫々所定角度回転させる回転素子31
2と、該回転素子の出射側に設けられた偏光合
成用偏光プリズム2とを備え、前記回転素子を制
御することにより前記偏光合成用偏光プリズムで
合成された光ビームを2つの受光部に選択的に結
合させる光スイツチであつて、 前記偏光分離用偏光プリズムと前記回転素子と
の間、および前記回転素子と前記偏光合成用偏光
プリズムの間に、合成光ビームを結合しない側の
前記受光部に漏話成分が結合しないように該漏話
成分に並進又は角度ずれを起させる複屈折板1
3,14,22,23又は25,27をそれぞれ
挿入したことを特徴とする光スイツチ。
[Scope of Claims] 1. A polarizing prism 1 for polarization separation, which is provided on the light incidence side and separates the incident light into two polarized lights, and a polarization plane of the two polarized lights separated by the polarization prism for polarization separation, respectively. Rotating element 3 1 that rotates a predetermined angle,
3 2 , and a polarization prism 2 for polarization synthesis provided on the output side of the rotating element, and by controlling the rotation element, the light beam combined by the polarization prism for polarization synthesis is sent to two light receiving parts. An optical switch for selectively coupling, the light receiving device on the side that does not couple the combined light beam between the polarizing prism for polarization separation and the rotating element, and between the rotating element and the polarizing prism for combining polarized light. A birefringent plate 1 that causes a translational or angular shift in the crosstalk component so that the crosstalk component is not coupled to the crosstalk component.
An optical switch characterized in that 3, 14, 22, 23 or 25, 27 are inserted respectively.
JP21801784A 1984-10-17 1984-10-17 Optical switch Granted JPS6197629A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP21801784A JPS6197629A (en) 1984-10-17 1984-10-17 Optical switch

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP21801784A JPS6197629A (en) 1984-10-17 1984-10-17 Optical switch

Publications (2)

Publication Number Publication Date
JPS6197629A JPS6197629A (en) 1986-05-16
JPS6362730B2 true JPS6362730B2 (en) 1988-12-05

Family

ID=16713320

Family Applications (1)

Application Number Title Priority Date Filing Date
JP21801784A Granted JPS6197629A (en) 1984-10-17 1984-10-17 Optical switch

Country Status (1)

Country Link
JP (1) JPS6197629A (en)

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
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