JPS5883801A - Optical switch - Google Patents

Optical switch

Info

Publication number
JPS5883801A
JPS5883801A JP18186281A JP18186281A JPS5883801A JP S5883801 A JPS5883801 A JP S5883801A JP 18186281 A JP18186281 A JP 18186281A JP 18186281 A JP18186281 A JP 18186281A JP S5883801 A JPS5883801 A JP S5883801A
Authority
JP
Japan
Prior art keywords
lens
optical
light
wave
polarizer
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.)
Granted
Application number
JP18186281A
Other languages
Japanese (ja)
Other versions
JPH0341809B2 (en
Inventor
Yoshinori Oota
太田 義徳
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.)
NEC Corp
Original Assignee
NEC Corp
Nippon Electric 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 NEC Corp, Nippon Electric Co Ltd filed Critical NEC Corp
Priority to JP18186281A priority Critical patent/JPS5883801A/en
Publication of JPS5883801A publication Critical patent/JPS5883801A/en
Publication of JPH0341809B2 publication Critical patent/JPH0341809B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/24Coupling light guides
    • G02B6/26Optical coupling means
    • G02B6/35Optical coupling means having switching means
    • G02B6/3564Mechanical details of the actuation mechanism associated with the moving element or mounting mechanism details
    • G02B6/3582Housing means or package or arranging details of the switching elements, e.g. for thermal isolation
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/24Coupling light guides
    • G02B6/26Optical coupling means
    • G02B6/35Optical coupling means having switching means
    • G02B6/354Switching arrangements, i.e. number of input/output ports and interconnection types
    • G02B6/35442D constellations, i.e. with switching elements and switched beams located in a plane
    • G02B6/35481xN switch, i.e. one input and a selectable single output of N possible outputs
    • G02B6/3551x2 switch, i.e. one input and a selectable single output of two possible outputs

Abstract

PURPOSE:To reduce the optical insertion loss of an element, by providing a lens, which allows optical axes of optical beams transmitted through a lateral optical converter to cross on the focal plane, and a crystal plate which makes optical beams transmitted through the lens incident to the position of crossing of optical axes at a Brewster angle. CONSTITUTION:The light emitted from an incidence optical fiber 1 is converted to a parallel luminous flux 12 through a collimator lens 2 and is incident to a polarizer 3 and is separated to a P wave 14 and an S wave 13. A lens 4 is so provided that its focus position is the reflection position on the polarizer 3. A high NA value, for example, about 0.5NA value is given to the lens 4, and the angle formed by the P wave 14 and the S wave 13 emitted from the polarizer 3 is narrow and about 32 deg., and therefore, both optical axes are made parallel by the lens which has a high NA value and has the focus position arranged in said reflection position, and the P wave 14 and the S wave 13 become a P polarized light 16 and an S polarized light 15. The beam diameter isn the rear focus position of the lens 4 is reduced to a value obtained by multiplying the magnification of the ratio of focal length of the lens 2 to the lens 4 by the value of the beam diameter on the exit end face of the optical fiber 1.

Description

【発明の詳細な説明】 本発明はファイバを伝わる光ピー^e*;*を匍換える
光7アイパスイツチ、と(に機械的可動部をもえ1に%
A、電子式の光スィッチに関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention provides an optical 7-eye pass switch that changes the optical pulses transmitted through a fiber, and
A. Regarding electronic optical switches.

光7テイパ過儒システムにおいては、 vA1110信
頼性を高め、保守を容易にするために、常用・予備eg
inの切換中光部品の切換え、また測定用などに広く光
スィッチが用いられている。まえ達地闘O過儒システム
の41らず限定され大地域内での情報部層機器間を結ん
だデータの伝送システム。
In the Hikari 7 taper overconfucian system, in order to increase vA1110 reliability and ease maintenance, regular and spare
Optical switches are widely used for switching optical components during switching of in, and for measurement. A data transmission system that connects intelligence equipment within a limited area.

−わゆる光データハイウェイにおける。ハイウェイと端
末とOII続ノーv′&どにも光スィッチが利用されて
−る。すなわち、41定の端末を回避する必要がある場
合、九とえば端末の故障、保守点検。
- on the so-called optical data highway. Optical switches are used for highways, terminals, and OII connections. That is, when it is necessary to avoid 41 fixed terminals, 9, for example terminal failure, maintenance inspection.

無使用時などには光スィッチにようで経路をバイパスす
る。
When not in use, use an optical switch to bypass the route.

このよう1に目的に合うた光スィッチとして開発されて
きて−るもの、01つは、ブリズ^中ζラーを電磁的に
変位させるものである。すなわち、光7アイパ出射光を
平行ビームに変換し、この光路中にプηズム・や−ンラ
ーを挿入することKようて光陽を空間的に蜜化させて、
再び集光される光7アィパを選択するものである。ζO
方式の光スィッチは高いクロストークと低い光挿入損の
特性を有し、利用しやすいものであるが9機械的可動機
構を有す′るため、速い切換速度を得ることが困−であ
り、fJ換回・数にえいする寿命中 a<間隔の長い動
作に対する信頼性に不安があ”ゐ、丸とえば。
One of the optical switches that have been developed to meet the abovementioned purposes is one that electromagnetically displaces the ζ-ra during the blizzard. That is, by converting the light emitted from the optical system into a parallel beam and inserting a prism into the optical path, the beam is spatially condensed,
This is to select the light 7 eyeper to be focused again. ζO
Although this type of optical switch has the characteristics of high crosstalk and low optical insertion loss and is easy to use, it is difficult to obtain a high switching speed because it has a mechanical movable mechanism. For example, there are concerns about reliability for operations with long intervals.

長期間にわたってほとんど一意的に或状態を保持し、或
時爽然スイッチ動作を行なわせえときに正しく動作をし
ないという不安定さが存在する。したがって容易に素子
の交換や点検が困難な光海底中継器などへの利用は閤−
である。
There is instability in that the switch almost uniquely maintains a certain state for a long period of time, and when a switch operation is suddenly performed, the switch does not operate correctly. Therefore, it cannot be used in optical submarine repeaters, etc., where it is difficult to easily replace or inspect elements.
It is.

機械的な可動部を有すことなく、電子的にファイバ光を
スイッチする素子として社次Oようなものも知られてい
る。透過光の偏光方向を電圧を丸線電流の印加によって
9f1転させる機能をもつ九個光変換素子に入射光を透
過させ、ζO後、光の偏光方向によって党略の方向倉異
ならしめる偏光素子を透過させるととによって異なる光
アアイパに光を導びくものである。偏光変換素子として
は、電気光学結晶や液晶などの電気光学材料、鉄ガーネ
ート結晶中高談度船ガラスなどのような磁気光学材料が
用いられている。従来のこの種の光スィッチには難点が
いくつかある。そのひと2社。
There is also known an element that electronically switches fiber light without having a mechanically movable part, such as that of Shaji O. The incident light passes through nine light conversion elements that have the function of changing the polarization direction of the transmitted light by applying a voltage to 9F1 by applying a round wire current, and after ζO, it passes through a polarizing element that changes the polarization direction depending on the polarization direction of the light. It guides light to different optical aipaths depending on the direction of the light. As the polarization conversion element, electro-optic materials such as electro-optic crystals and liquid crystals, magneto-optic materials such as iron garnate crystal, medium-high polarization glass, and the like are used. Conventional optical switches of this type have several drawbacks. Two companies.

構成する偏光素子が高価であるかもしくは特性が不十分
である点である。上に述ぺえ光の偏光方向によって党略
を変える偏光素子としては、古くから知られている複屈
折の大きな材料である方解石を使った偏光プリズムや、
中はヤ複履折の大きな材料であるルチル結晶をプリズム
状に成形研磨しえもの、ガラスで□作り九全反射プ嗜ズ
ムの反射面上Kll電体の三層膜を形成し偏光素子とす
るものなどがある。方解石は自然石であって高価である
こと、ルチルプリズムも結晶材料一体が高価で4Mとと
もに、高い屈折率を有するえめにプ9ズム入射画には良
好な無反射膜を形成する必要があること、ガラス材料に
誘電体多層膜を設けた偏光素子では、多層膜の入射光に
たいする波長特性が敏感であるため、設計波長より、ず
れた波長の光の入射にたいして偏光特性が劣化するなど
の難点を有する。
The problem is that the constituent polarizing elements are expensive or have insufficient characteristics. As mentioned above, polarizing elements that change the polarization depending on the polarization direction of the light include polarizing prisms made of calcite, which is a material with high birefringence that has been known for a long time.
The inside is made of rutile crystal, which is a material with a large double refraction, formed into a prism shape and polished, and is made of glass.A three-layer film of Kll electric material is formed on the reflective surface of the total reflection prism, and a polarizing element is formed. There are things to do. Calcite is a natural stone and is expensive, and rutile prism is also an expensive crystal material, and like 4M, it has a high refractive index, and it is necessary to form a good anti-reflection film for the prism incident image. In polarizing elements made of glass material with a dielectric multilayer film, the wavelength characteristics of the multilayer film are sensitive to incident light, so there are drawbacks such as deterioration of the polarization characteristics when light of a wavelength deviates from the design wavelength is incident. have

また従来の光スィッチの有する一点の25@は。Also, the one point 25@ of a conventional optical switch is.

偏光変換素子の光透過新薗が大であることを必要とする
か、又は円筒レンズを必要としてか勤、印加する外場O
大なることまたは円IIvンズO収差による光透過損失
の増加を壜ぬがれtkい点にある。
The applied external field O may require a large light transmission capacity of the polarization conversion element or may require a cylindrical lens.
It is difficult to avoid an increase in light transmission loss due to large or circular lens O aberrations.

すなわち、光学系の配置は入射ファイに党を:y啼メー
トするコリメートリンズとヒの:y1メート光パ゛ を出射ファ1に集草する県東レンズを駿け、これらレン
ズ閤の光路中に前述の偏光変換素子や偏光素子を設ける
ものである。:lリメート光は断藺1■φ11変ある丸
め価光変換素子eIIf画は数−角又は数■φ以上を必
要とする。この丸め偏光変換素子に磁気光学材料を用I
A丸場合には反磁界係数が大と&L磁化を飽和させるに
畳する外部磁場が太きく1伽、この磁場を発生させる丸
めの電1腫も大きく1にうでいる。電気光学材料を用%
/%丸場舎には、電気光学効果O小″sIAIIIm素
子を利用して*抄、印加電圧が数百Vと高−0偏光変換
素子を板状の%のを用いれば′反磁界係数O低下中横■
電気光学素子を用いるヒと−で自る。10良め:11メ
ー)光を一次元方向にビーム―を縮小する円筒レンズを
偏光変換素子の前後に設けている。数胃OS点距離を有
する円筒レンズは高性能のものは得に〈〈、収差が大き
い九めに、素子の先挿入損失を悪くしている。
In other words, the arrangement of the optical system includes a collimating lens that directs the light beam to the input beam by y1 meters, and a Kento lens that collects the beam to the output beam 1, and the optical path of these lenses is The above-mentioned polarization conversion element and polarization element are provided. The rounded value light conversion element eIIf requires a number of angles or a number of angles or more. This rounded polarization conversion element uses magneto-optical material.
In the case of the A circle, when the demagnetizing field coefficient is large, the external magnetic field that is applied to saturate the &L magnetization is large, and the round electromagnetic field that generates this magnetic field is also large. % using electro-optic materials
/%Marubasha uses an sIAIIIm element with a small electro-optical effect O.If the applied voltage is several hundred V and a high-0 polarization conversion element is used in the form of a plate, the demagnetizing field coefficient O Declining horizontally■
This can be achieved by using an electro-optical element. 10 good: 11 meters) Cylindrical lenses that reduce the beam of light in one dimension are provided before and after the polarization conversion element. High-performance cylindrical lenses with several OS point distances have particularly large aberrations, which worsens the element's initial insertion loss.

本発明の目的は上記一点を除去し丸、7アイパ光スイツ
チを提供することに′hる。
The object of the present invention is to eliminate the above point and provide a 7-eye light switch.

本発−によれば、高い屈折率を有し両INK光学研磨を
1こしえ結晶板と、該結晶板にプリ為スター角で入射し
、該結晶板を透過し電光ビームの光軸と反射し走光ビー
ムの光軸とを平行化するレンズと、該レンズによって平
行化され九前記2つの光ビームが透過し、印加される外
場によりて該光ビームO偏光をSOW回転させる偏光変
換素子と。
According to the present invention, both INK optical polishers having a high refractive index are passed through a crystal plate, and the light beam is incident on the crystal plate at a pre-star angle, passes through the crystal plate, and is reflected from the optical axis of the electric beam. a lens that parallelizes the optical axis of the traveling light beam, and a polarization conversion element that transmits the two light beams that are parallelized by the lens and rotates the polarized light beam by an applied external field. .

皺個光変換素子を透過した光ビームの光軸を侭点画上で
交叉せしめるレンズと、光軸を交叉せしめた装置に、#
レンズを透過しえ光ビームをブルースター角で入射せL
J6るように配置した前記結晶板と同一の結晶板とによ
りて安価で高性能な光スィッチが得られる。
#
Let the light beam pass through the lens and enter at Brewster's angle L
An inexpensive and high-performance optical switch can be obtained by using the same crystal plates as the above-mentioned crystal plates arranged in such a manner as to be similar to the above-mentioned crystal plates.

古来シリコン結晶のよう傘高履折率O結晶板にブルース
ター角で光を入射させ透過光aSS偏光度を向上寄せる
偏光フィルタは知られて−る。しかしζヒでは偏光フィ
ルタで反射される光は利用されていない、高屈折率の結
晶板による透過光及び反射光相方なそ011に配置する
適切なパラメータを有するレンズによって光学的xmi
i*<集光する簡便な構成およびヒの光学系と偏光変換
素子とを履舎せえ工業的に益ある光スイッチO構威は本
実―看によりて初めてなされるものである。
Polarizing filters have been known since ancient times that improve the aSS polarization degree of transmitted light by making light incident on a high refractive index O crystal plate such as a silicon crystal at the Brewster's angle. However, in ζhi, the light reflected by the polarizing filter is not used, but the transmitted light and reflected light by the crystal plate with a high refractive index are optically xmi
A simple construction for condensing light and an industrially advantageous optical switch configuration combining an optical system and a polarization converting element were first realized through actual research.

本実W140詳細を更に実施例を用いて説明する。Details of the actual W140 will be further explained using examples.

第1図は本実1jlO第−e@施例で1は入射光7アイ
パ、2けツリメー)レンズ、3は入射側O領光素子、4
.6は集光レンズ、Sは偏光変換素子。
Fig. 1 shows the present example, 1 is the incident light 7 eyeper, 2 is the lens, 3 is the incident side O area light element, 4
.. 6 is a condenser lens, and S is a polarization conversion element.

7は出゛射側の偏光素子、8.9d集車レンズ、lへ1
1は出射光ファイバである。入射光ファイバ1を出射し
先光は=リメートレンズ2によって平行先車12と1に
り、 偏光子3に入射される。該偏光子30原理は後述
するがその機能は入射光12t!’11114と8m1
3に分離54kh、vンズ4Bうに股妙る。そして該レ
ンズは高いNA値たとえばOSS度の値を有するレンズ
とする。前記偏光子3を出射するP波14fl波13の
なす角度は談述の如く32変Il変と狭いため高Nム値
を有し前記焦点位置の配置を有するレンズ4によってそ
れらの光軸は平行化されP偏光16.8偏光15となる
。そしてレンズ40後側焦点位置でのビーム径はレンズ
2とレンズ4との焦点距離比の拡大率を光7アイパ1の
出射端面でのビーム径に乗じ九大きさに集束される。た
とえばプア径50―の光ファ4 /(をIK用−、レン
ズ2とレンズ4との焦点距離を等しいもOK選べば6等
倍結像であるためレンズ4のiuw焦点位置における光
ビーム径は50am11度となる。したがうてこのビー
ムを透過させ偏光を9Ca転させる機能を有する偏光変
換子5の第1図KsI−ける紙両働直方向の輪は小さい
すなわち薄い板状の形状を有するものでよい、該偏光変
換子5に入射さにた2つの直線偏光光15゜及び16は
、誼偏光変換子に印加される電圧中電流等の外場の状態
に応じて岡−の偏光状態かまえはそれに直交する偏光へ
と偏光状態が定められる。
7 is a polarizing element on the output side, 8.9d is a collection lens, 1 to l
1 is an output optical fiber. The forward light emitted from the input optical fiber 1 is transferred to the parallel forward wheels 12 and 1 by the remating lens 2, and is incident on the polarizer 3. The principle of the polarizer 30 will be described later, but its function is that the incident light is 12t! '11114 and 8m1
Separated into 3, 54kh, V's 4B sea urchin is strange. The lens is a lens having a high NA value, for example, an OSS value. Since the angle formed by the P wave 14fl wave 13 emitted from the polarizer 3 is as narrow as 32 degrees and Il angle as mentioned in the discussion, their optical axes are parallel to each other by the lens 4 having a high N value and having the focal position arrangement. The P-polarized light becomes 16.8 and the P-polarized light becomes 15. The beam diameter at the rear focal position of the lens 40 is focused to 9 by multiplying the beam diameter at the exit end surface of the light 7 eyeper 1 by the magnification ratio of the focal length ratio of the lenses 2 and 4. For example, if you choose the optical fiber 4/(for IK with a diameter of 50-) and the focal lengths of lenses 2 and 4 to be equal, the image will be 6 equal magnification, so the light beam diameter at the iuw focal position of lens 4 will be 50 am and 11 degrees.Therefore, the ring in the direction perpendicular to the paper in FIG. The two linearly polarized lights 15° and 16 incident on the polarization converter 5 change their polarization state depending on the state of the external field such as voltage or current applied to the polarization converter. The polarization state is determined to be polarized light orthogonal to that.

今、偏光変換子5 K J 5で偏光が91’11転せ
しめられ九とすると入射8偏光ISけr偏光へP偏光1
6は8偏光へと偏光変換され偏光変換素子5を出射する
。これらの先板が透過するレンズ6出射偏光子)は前述
のレンズ4.入射偏光子3とそれぞれ岡−0%のとし、
レン□ズ4011点位置を挾んで対称となるように配置
する。すなわちレンズ6の焦点位置の一方はレンズ40
焦点位置、他方は偏光子70光反射位置とする。レンズ
6を透過する2つの偏光d、光軸はレンズ60焦点位置
に崗って集束し、それぞれの光束は平行先車となる。
Now, the polarization converter 5 K J 5 inverts the polarization by 91'11, and if it is 9, then the incident polarized light IS becomes r polarized light and P polarized light 1.
6 is polarized into 8 polarized light and outputted from the polarization conversion element 5. The lens 6 (output polarizer) through which these front plates pass is the lens 4. Assuming that the input polarizer is 3 and Oka-0% respectively,
The lenses □ are arranged symmetrically across the 4011 point positions. That is, one of the focal positions of the lens 6 is the lens 40.
The focal position is the focal point, and the other is the polarizer 70 light reflection position. The optical axes of the two polarized lights d passing through the lens 6 are converged at the focal point of the lens 60, and each light beam becomes a parallel leading wheel.

レンズ6け前述のようにレンズ4と同一0411性のレ
ンズである丸め、2つの偏光17,18の光軸の集草角
変は入射の偏光子3を出射しレンズ4に向う2つの偏光
13.14のなす角度と同一である。前述の如く8偏光
である光ビーム15は偏光変換されている丸め、光ビー
ムlフはP偏光である。出射偏光子7に入射し九r偏光
である光ビーム17は偏光子7を透過し光ビーム20と
なりてレンズ9を介して出射ファイバIIK結合される
As mentioned above, lens 6 is a lens with the same 0411 characteristics as lens 4. The angle of collection of the optical axes of the two polarized lights 17 and 18 is changed so that the two polarized lights 13 exit the incident polarizer 3 and head towards the lens 4. It is the same as the angle formed by .14. As described above, the light beam 15, which is 8-polarized light, is a rounded light beam that has undergone polarization conversion, and the light beam 15 is P-polarized light. A light beam 17 which is incident on the output polarizer 7 and is 9r polarized light is transmitted through the polarizer 7 and becomes a light beam 20, which is coupled to the output fiber IIK via the lens 9.

まえP偏光である光ビーム16は偏光変換されると、8
偏光である18とな抄この光ビームは偏光子7で反射さ
れ先の光ビーム20と合流し出射ファイバIIK納会さ
れる。すなわち、光ファイ/(1を出射し丸洗ビームは
偏光子3によって偏光分離され、偏光変換子5によって
偏光回転を受は出射側偏光子7によって金波されて出射
ファイバ11に、納会される。一方偏光変換子5に印加
する電圧や電流等の外場の状態を、偏光の回転が生じな
いように設定すると、前述の光ビーム17は光ビーム1
3の偏光状態と同一の8偏光であり、この光ビームけ偏
光子7によって反射され光ビーム19となってレンズ8
を介して11とは別なる光ビームIOK結合される。ま
た光ビーム18はP偏光であるため偏光子7を透過し、
先の光ビーム19に合流してやけり光ファイバ10に納
会されゐ、この場合には光ファイバ1を出射すゐ先は、
出射光ファイバ10へ納金される。すなわち偏光変換子
の状IIO切換えkよって光フアイバ10出刃先を2つ
の出射光ファイバ161九は11の−ずれかへ結合させ
ることができる1%Aわゆる!×2光スイッ?Oj作が
実現される。
When the light beam 16, which is previously P-polarized, undergoes polarization conversion, it becomes 8
The polarized light beam 18 is reflected by the polarizer 7, merges with the previous light beam 20, and is delivered to the output fiber IIK. That is, the beam emitted from the optical fiber /(1 is polarized and separated by the polarizer 3, polarized by the polarization converter 5, polarized by the polarizer 7 on the output side, and sent to the output fiber 11. On the other hand, if the state of the external field such as the voltage and current applied to the polarization converter 5 is set so that rotation of polarization does not occur, the above-mentioned light beam 17 becomes the light beam 1.
This light beam is reflected by the polarizer 7 and becomes a light beam 19 that passes through the lens 8.
A separate light beam IOK from 11 is coupled via. Furthermore, since the light beam 18 is P-polarized light, it passes through the polarizer 7,
It merges with the previous light beam 19 and is finally delivered to the optical fiber 10. In this case, the destination from which the optical fiber 1 is emitted is
The money is sent to the output optical fiber 10. That is, by switching the shape of the polarization converter IIO, the tip of the optical fiber 10 can be coupled to either of the two output optical fibers 1619 or 11. ×2 light switch? Oj's work is realized.

次に偏光子O動作を鋭−する、第2園は偏光子の原理を
示す図で100はv9コン、ガ啼つム砒素。
Next, sharpen the operation of the polarizer O. The second diagram is a diagram showing the principle of a polarizer.

インジクムリン等o@IA単結晶板″ehる。これらの
結晶は光波長1j1mから2μ■寝度にわえうて透明な
結晶である。九とえばN!Of/l:yン単結晶で中ヤ
リア密度1.4X10aw  のものは光波長1.3J
1m−1Jim()領域での吸釈係数は6.1 as−
”以下と極めて良好な光透過特性を示す、まえ麿折率は
3.5欄度と非常に高くブリ為スタ角−は74度と大龜
−0光ビーム101をφ暑74度(θ諺16度)のプダ
晶スタ角で入射させると薄い結晶板の上下面でoxmが
加え合さりて0反射光102は8偏光成分だ砂と1−)
その反射率は84襲となる。遥遥光10Bは?偏光成分
が大部分でそO透過率は前述り1l収O効来が低い丸め
非常に高−0仁の遥遥光103に会まれる8偏愛虞分は
13弧である。嬉2光素子が得られる。まえ前述の如く
に0116度・と非常に洩−角度光ビームを入射させる
ことKなるえめ、第111に示す如<KNA値の高いレ
ンズを用−ることによりてP偏光8偏光の光軸を平行化
することができる。
Indicumlin etc. o@IA single crystal plate''eh. These crystals are very transparent crystals with a light wavelength of 1 m to 2 μm. For example, N!Of/l:y The light wavelength of Yaria density 1.4X10aw is 1.3J.
The absorption coefficient in the 1m-1 Jim() area is 6.1 as-
``The refractive index is very high at 3.5 degrees, and the star angle is 74 degrees, which means that the light beam 101 can be converted to a diameter of 74 degrees (the proverbial θ). When the light is incident at a puda crystal star angle of 16 degrees), oxm is added on the top and bottom surfaces of the thin crystal plate, and the 0 reflected light 102 has 8 polarized components.Sand and 1-)
Its reflectance is 84 times. What about Haruka Hikari 10B? Most of the polarized light components are present, and the O transmittance is as described above, and the 8 polarization potential encountered by the very high-0 rays of the far-field light 103 is 13 arcs. A happy two-photon element is obtained. As mentioned before, since the light beam must be incident at a very narrow angle of 0116 degrees, by using a lens with a high KNA value as shown in No. 111, the optical axis of the P-polarized light can be changed. Can be parallelized.

嬉1m1eCThける偏光変換子5は従来知られている
各種のものを使うζ、とがで龜る0例えばLITa01
結晶の電気光学効果倉使りえ偏光変換子中YIGのよう
な磁気光学結晶の7アツデ効果を用vhえ偏光変換子を
利用しえ場合には前述の如く、偏光変換子が置かれる位
置での光ビーム径は50 am と非常に小さいため1
%/hずれも厚さの薄い結晶板でよく、印加電圧量印加
磁場強度は低く(て済むという特長をtつ。
For the polarization converter 5, various conventionally known ones are used.For example, LITa01 is used.
The electro-optic effect of a crystal can be used as a polarization converter.If a magneto-optic crystal such as YIG is used, the polarization converter can be used as described above. Since the light beam diameter is very small at 50 am,
%/h deviation also requires a thin crystal plate, and the applied voltage and applied magnetic field strength are low.

第1閣K>いては1人カファイバ光を2つのいずれかO
出力ファイバに結合する■ゆる1×2光スイツチの実施
例について示しえ、入力側光7アイパを2本としその配
置を嬉111における出力ファイバと同様とすることで
2×2先スイツチを実現することは容品である。
1st cabinet K > If one person uses fiber optic, either one of the two O
An example of a loose 1 x 2 optical switch coupled to the output fiber will be shown. A 2 x 2 destination switch will be realized by using two optical 7-eyepers on the input side and arranging them in the same way as the output fiber in Yuki 111. That's a matter of fact.

また偏光素子から出射する8傷光光P個光光O光軸を平
行化するレンズは1つのレンズで同機能をlI!現する
場合を述べたが、それでれレンズを1つづつ合せて2つ
用いてもよい、ξOヒとは偏光変換素子から出射した光
軸が平行と倉りている光ビームをコリメートし出射側偏
光素子に導び〈レンズにつiて%同様にすること捻可能
である。
In addition, the lens that parallelizes the optical axes of the 8 damaged light beams P light beams O emitted from the polarizing element can perform the same function with just one lens! In this case, two lenses may be used, one at a time. It is possible to do the same thing with a polarizing element and a lens.

以上述べえ如く本発明によれば安価で高性能の光スィッ
チを得ることができる。
As described above, according to the present invention, an inexpensive and high-performance optical switch can be obtained.

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

第1mは本斃明の一実施例の構成を示す図で1は入力光
ファイバ、3は入力側偏光素子、4と6は高Nム値を膚
するシンズ、5鯰偏光変換素子、)吐出力側偏光素子、
10.11は出力光7アイパである。第2IIl鯰偏光
素子の動作を示す原ll1l″t”1OQd高屈折率結
晶板である。 鵬1図 鳩 2 図 03
The 1st m is a diagram showing the configuration of an embodiment of the present invention, where 1 is an input optical fiber, 3 is an input side polarizing element, 4 and 6 are thin beams with a high N value, 5 is a catfish polarization conversion element, and 5) discharge. power side polarizing element,
10.11 is the output light 7 eyeper. This is an original ll1l″t″1OQd high refractive index crystal plate showing the operation of the 2nd IIl catfish polarizing element. Peng 1 Figure Pigeon 2 Figure 03

Claims (1)

【特許請求の範囲】[Claims] 高い履折率を有し、開田に光学研磨を施ζしぇ結晶板と
、諌結晶板にブルースター角で入射り諌結晶板を透過す
る光ビームO光軸と反射す為光ビームO光軸とを平行化
するレンズと、該レンズによりて平行化された前記鵞り
O光ビームが透過し印加される外場によりて該光ビーム
0傷光を90度ll@せしめる1光麦換素子と、皺傭先
変換素子を透過しえ光ビームの光軸を焦点画上で交叉せ
しめるレンズと、光軸を交叉せし袷た位置に鍍レンズを
透過した光ビームをブルー−スター角で人、射せしめる
ように配置した曽記麺晶板と岡−〇結晶板とを有するし
とを畳黴゛とする先スイッチ。
The crystal plate has a high refractive index and has been optically polished.The optical axis of the light beam that is incident on the crystal plate at Brewster's angle and passes through the crystal plate is reflected. a lens that parallelizes the axis, and a one-light conversion element that allows the optical beam parallelized by the lens to pass through and make the optical beam distorted by 90 degrees by an applied external field. Then, a lens that passes through the wrinkled tip conversion element and causes the optical axes of the light beam to intersect on the focal image, and a light beam that has passed through the shank lens at the position where the optical axes intersect and cross is placed at the Brewster angle. , a tip switch that has a Zengki Noodle crystal plate and an Oka-〇 crystal plate arranged so as to emit light from the bottom.
JP18186281A 1981-11-13 1981-11-13 Optical switch Granted JPS5883801A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP18186281A JPS5883801A (en) 1981-11-13 1981-11-13 Optical switch

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP18186281A JPS5883801A (en) 1981-11-13 1981-11-13 Optical switch

Publications (2)

Publication Number Publication Date
JPS5883801A true JPS5883801A (en) 1983-05-19
JPH0341809B2 JPH0341809B2 (en) 1991-06-25

Family

ID=16108132

Family Applications (1)

Application Number Title Priority Date Filing Date
JP18186281A Granted JPS5883801A (en) 1981-11-13 1981-11-13 Optical switch

Country Status (1)

Country Link
JP (1) JPS5883801A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104122074A (en) * 2014-07-08 2014-10-29 国家电网公司 Optical fiber luminous flux testing device and method

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS56137329A (en) * 1980-03-28 1981-10-27 Fujitsu Ltd Polarized and separated light control device
JPS5850415U (en) * 1981-09-29 1983-04-05 富士通株式会社 optical crystal device

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4158141A (en) * 1978-06-21 1979-06-12 Hughes Aircraft Company Process for channeling ion beams

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS56137329A (en) * 1980-03-28 1981-10-27 Fujitsu Ltd Polarized and separated light control device
JPS5850415U (en) * 1981-09-29 1983-04-05 富士通株式会社 optical crystal device

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN104122074A (en) * 2014-07-08 2014-10-29 国家电网公司 Optical fiber luminous flux testing device and method

Also Published As

Publication number Publication date
JPH0341809B2 (en) 1991-06-25

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