CN208432822U - Reflection-type magneto-optic switch - Google Patents

Reflection-type magneto-optic switch Download PDF

Info

Publication number
CN208432822U
CN208432822U CN201821301718.4U CN201821301718U CN208432822U CN 208432822 U CN208432822 U CN 208432822U CN 201821301718 U CN201821301718 U CN 201821301718U CN 208432822 U CN208432822 U CN 208432822U
Authority
CN
China
Prior art keywords
light beam
birefringece crystal
wave plate
collimater
reflection
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.)
Active
Application number
CN201821301718.4U
Other languages
Chinese (zh)
Inventor
顾连军
杜建义
李坡
王万新
孙万英
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.)
ZHUHAI PUAO OPTOELECTRONICS TECHNOLOGY Co Ltd
Original Assignee
ZHUHAI PUAO OPTOELECTRONICS TECHNOLOGY 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 ZHUHAI PUAO OPTOELECTRONICS TECHNOLOGY Co Ltd filed Critical ZHUHAI PUAO OPTOELECTRONICS TECHNOLOGY Co Ltd
Priority to CN201821301718.4U priority Critical patent/CN208432822U/en
Application granted granted Critical
Publication of CN208432822U publication Critical patent/CN208432822U/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Abstract

A kind of reflection-type magneto-optic switch, the combination comprising input collimater, the first output collimater, second output terminal collimator, prism, first birefringece crystal, the first half-wave plate pair, the combination of Farady rotator and magnetic element, second birefringece crystal, the second half-wave plate pair, right-angle prism.The magnetic element can apply saturation magnetic field on the Farady rotator, it is exported so as to cause the light beam inputted from input collimater from the first output collimater, or the magnetic element can not apply magnetic field on the Farady rotator, export so as to cause the light beam inputted from input collimater from second output terminal collimator.

Description

Reflection-type magneto-optic switch
Technical field
The utility model relates to a kind of reflection-type magneto-optic switches, more particularly to the reflection-type magneto-optic comprising faraday's crystal to open It closes.
Background technique
Photoswitch be used to cut between an input optical fibre and one or more output optical fibre in optical system Change light beam.For example, photoswitch be used to be connected and disconnected from transmission channel in light communication system to route by the light of modulates information Beam provides network protection, provides interconnection, and point slotting application.Photoswitch can be used for that light source is made to generate pulse, such as laser Device, or other function is realized using modulation or unmodulated light beam.
Photoswitch is realized there are many mode, is generally comprised mechanically, micro-electronic mechanical system technique (MEMS), electro-optical, Thermo-optic type, Mach Zehnder interference technique and magneto-optic formula etc..Wherein, magneto-optic shutter is using faraday's magnetic rotation effect come real The switching of existing optical path due to no any moving component, thus has superior reliability and switching speed response.
Magneto-optic shutter can be divided into transmission-type and two kinds reflective from light channel structure.Reflection-type magneto-optic volume of switch is small, at This is low;And since light beam passes through birefringece crystal and Farady rotator back and forth, higher channel separation can also be obtained Degree, thus application is more extensive.
Utility model content
The utility model relates to a kind of reflection-type magneto-optic switch, the reflection-type magneto-optic switch includes: input collimater, Female light beam is inputted the reflection-type magneto-optic and switched by the input collimater;First output collimater and second output terminal are quasi- Light beam is exported the reflection-type magneto-optic and switched by straight device, first output collimater and second output terminal collimator,;Rib Mirror, the prism can make light beam that deviation occur;The optical axis of first birefringece crystal, first birefringece crystal is located at level Face, first birefringece crystal are made of birefringent material, when female light beam is injected described first by the input collimater When birefringece crystal, it is orthogonal beamlet that female light beam is separated into two beam polarization states by first birefringece crystal;The Half of wave plate pair, first half-wave plate are inclined to that the two beam polarization states passed through from left to right can be become two beams for orthogonal light beam The identical light beam of polarization state;The combination of Farady rotator and magnetic element, the magnetic element is controllable magnetic element, described Magnetic element can apply saturation magnetic field on the Farady rotator or not apply magnetic field, the Farady rotator It can make to input the Faraday when not being applied magnetic field with the Farady rotator after being applied saturation magnetic field The light beam of crystal becomes different polarization states;The optical axis of second birefringece crystal, second birefringece crystal is located at horizontal plane, Second birefringece crystal is made of birefringent material, and second birefringece crystal can make light beam deviation occur or without deviation Directly pass through;Second half-wave plate pair, second half-wave plate is to can have identical polarization state for two beams that pass through from left to right It is orthogonal light beam that light beam, which becomes two beam polarization states, and second half-wave plate to can be by the two beam polarization states passed through from right to left Orthogonal light beam becomes the identical light beam of two beam polarization states;Light beam can be reflected to change by right-angle prism, the right-angle prism The direction of darkening beam.
The optical element of reflection-type magneto-optic switch is set gradually from left to right are as follows: the input collimater, described The combination of first output collimater, the second output terminal collimator, the prism, first birefringece crystal are described First half-wave plate pair, the combination of the Farady rotator and magnetic element, second birefringece crystal, described the second half Wave plate pair, the right-angle prism.
Preferably, first birefringece crystal is calcite.
Preferably, when the Farady rotator applies saturation magnetic field by the magnetic element, pass through the faraday The polarization state of the light beam of gyrotropi crystal rotates 45 degree counterclockwise.
Preferably, it when the Farady rotator does not apply magnetic field by the magnetic element, is revolved by the faraday The polarization state of the light beam of luminescent crystal rotates clockwise 45 degree.
Preferably, the optical element that the light beam of the input collimater input passes through is successively are as follows: described first is birefringent Crystal, first half-wave plate pair, the combination of the Farady rotator and magnetic element, second birefringece crystal, Second half-wave plate pair, the right-angle prism, second half-wave plate pair, second birefringece crystal, the faraday The combination of gyrotropi crystal and magnetic element, first half-wave plate pair, first birefringece crystal, the prism, then from First output collimater projects.
Preferably, the optical element that the light beam of the input collimater input passes through is successively are as follows: described first is birefringent Crystal, first half-wave plate pair, the combination of the Farady rotator and magnetic element, second birefringece crystal, Second half-wave plate pair, the right-angle prism, second half-wave plate pair, second birefringece crystal, the faraday The combination of gyrotropi crystal and magnetic element, first half-wave plate pair, first birefringece crystal, the prism, then from The second output terminal collimator projects.
Detailed description of the invention
Fig. 1 a is the structural schematic diagram of magneto-optic shutter, and light beam is injected from input collimater at this time, from the first output end standard Straight device projects;Fig. 1 b is the structural schematic diagram of magneto-optic shutter, and light beam is injected from input collimater at this time, from second output terminal standard Straight device projects;
Fig. 2 is light beam by the polarization state variation diagram after each optical component of magneto-optic shutter, and light beam is from input terminal at this time Collimator is injected, and is projected from the first output collimater;
Fig. 3 is light beam by the polarization state variation diagram after each optical component of magneto-optic shutter, and light beam is from input terminal at this time Collimator is injected, and is projected from second output terminal collimator.
Specific embodiment
Embodiment one
A reflection-type magneto-optic switch is present embodiments provided, which does not include movable part, the light having had Performance and high switch speed are learned, and can be realized with a small size.Fig. 1 a shows the optical component of magneto-optic shutter Arrangement.Magneto-optic shutter includes three single optical fiber calibrators: input collimater 110, the first output collimater 109 and second are defeated Outlet collimator 111;One prism 101, it is preferable that prism 101 is rhombic prism;Two birefringece crystals: first is birefringent Crystal 102 and the second birefringece crystal 106;Two half-wave plates pair: the first half-wave plate to 103 and second half-wave plate to 107;One Farady rotator 105;One group of magnetic element 104 and a right-angle prism 108.Input collimater 110 is to be loaded with input The input collimater of light beam, the first output collimater 109 and second output terminal collimator 111 are be loaded with output beam defeated Outlet collimator.It is received by the first output collimater 109 or second output terminal collimator 111 and comes from input collimater 110 light beam realizes the function of magneto-optic shutter in the present embodiment.
Prism 101 is arranged on the first output collimater 109, input collimater 110, second output terminal collimator 111 right sides, prism 101 mainly receive output beam and change its direction, and light beam is incident on after deviation occurs in prism 101 In first output collimater 109 or second output terminal collimator 111.
First birefringece crystal 102 is arranged on the right side of prism 101, and the optical axis of the first birefringece crystal 102 is located at water Plane.First birefringece crystal 102 is made of birefringent material, when input collimater 110 input female light beam from left to right By when, female light beam is separated into the orthogonal polariton beam of two beams by the first birefringece crystal 102: one with refractive index no Ordinary light beamlet and an extraordinary ray beamlet with refractive index ne.Certainly, two beams separated obtained are orthogonal Polariton beam or same light beam can be merged into original female light beam after passing through from right to left.Preferably, first pair Refracting crystal 102 is calcite, and such selection can obtain in cost and difficulty of processing preferable in volume industrial production Balance.
The right side that first half-wave plate is arranged on the first birefringece crystal 102 to 103.First half-wave plate to 103 optical axis To determine direction, two beams refraction photon light beam, which has, after female light beam passes through the first birefringece crystal 102 from left to right mutually hangs down Straight polarization state, the photon light beam of two beams refraction later again from left to right by have determine first half-wave plate in direction to after 103, First half-wave plate makes this two beams beamlet polarization state having the same to 103;When the beamlet of two beams polarization state having the same From right to left by having the first half-wave plate for determining direction to after 103, the first half-wave plate has this two beams beamlet to 103 Orthogonal polarization state.
The combination of Farady rotator 105 and magnetic element 104 is arranged on the first half-wave plate to 103 right side.Method Draw gyrotropi crystal 105 that light polarization direction can be made to rotate, Beam rotation amount is the function of 105 thickness of Farady rotator. Usual Farady rotator is thicker, and the rotation being applied on light beam is bigger.Wherein magnetic element 104 is controllable magnetic element, Farady rotator 105 can be applied and add saturation magnetic field or the additional saturation magnetic field is made to disappear.
Second birefringece crystal 106 is arranged on the right side of Farady rotator 105, receives brilliant from Faraday The light beam of body 105 makes light beam that deviation or directly passing through without deviation occur.The optical axis of second birefringece crystal 106 is perpendicular to water Plane.In the present embodiment, such as Fig. 1 a, when magnetic element 104 applies magnetic field, light beam from left to right can be directly logical without deviation It crosses, deviation can occur for light beam from right to left;Such as Fig. 1 b, when magnetic element 104 does not apply magnetic field, light beam from left to right can be sent out Raw deviation, light beam from right to left can directly pass through without deviation.
The right side that second half-wave plate is arranged on the second birefringece crystal 106 to 107.Equally, the second half-wave plate is to 107 Optical axis is to determine direction, when the beamlet of two beams polarization state having the same is from left to right by having determine direction the second half For wave plate to after 107, the second half-wave plate makes this two beams beamlet have orthogonal polarization state to 107;When two beams have mutually The beamlet of vertical polarization state from right to left by have determine second half-wave plate in direction to after 107, the second half-wave plate pair 107 make this two beams beamlet polarization state having the same
Right-angle prism 108 is arranged on the second half-wave plate to 107 right side.By the second half-wave plate to 107 light beam quilt Right-angle prism 108 reflects.Right-angle prism 108 is arranged on properly relative to the second birefringece crystal 106 and entire magneto-optic shutter Position so that light beam can be reflected back toward the second birefringece crystal 106 and the first output collimater 109 or the second output Hold collimator 111.
The optical element of magneto-optic shutter is set gradually from left to right are as follows: input collimater 110, the first output collimater 109, the combination of second output terminal collimator 111, prism 101, the first birefringece crystal 102, the first half-wave plate is to 103, farad The combination of gyrotropi crystal 105 and magnetic element 104, the second birefringece crystal 106, the second half-wave plate is to 107, right-angle prism 108。
The combination of Farady rotator 105 and magnetic element 104 by magnetic element 104 whether apply saturation magnetic field come Change light beam to project from the first output collimater 109 or second output terminal collimator 111, to realize the function of magneto-optic shutter Energy.It is described in more detail below its principle.
Fig. 1 a and Fig. 2 describe magneto-optic shutter and light beam are input to the first output collimater from input collimater 100 The applicable cases of 109 outputs.Fig. 1 a illustrates the component of magneto-optic shutter and the light beam by these components, Fig. 2 are illustrated The polarization state of light beam after each component that light beam passes through magneto-optic shutter.
The light beam 112 projected from input collimater 110 is incident on the first birefringece crystal 102, the first birefringece crystal 102 optical axis is located at horizontal plane (i.e. in paper), the female light beam 112 projected by input terminal 110 can be decomposed into polarization direction Two orthogonal and spatially separated parallel beamlets.The polarization direction of first beamlet 113 (e light) is parallel to optical axis institute Plane (paper), the polarization direction of the second beamlet 114 (o light) is perpendicular to optical axis.Wherein the second beamlet 114 does not occur Deviation passes through the first birefringece crystal 102, and the first beamlet 113 then generates a sidesway.First beamlet 113 and second later Beamlet 114 makes the first beamlet 113 and the second beamlet 114 to 103 to 103, first half-wave plates by the first half-wave plate Polarization state direction is identical.Identical beamlet the first beamlet 113 of following two beams polarization state and the second beamlet 114 are incident on Farady rotator 105, at this time Farady rotator 105 outside magnetic element 104 plus saturation magnetic field under, the first sub-light The polarization state of beam 113 and the second beamlet 114 is relative to first beamlet 113 and the second sub-light in the first half-wave plate is to 103 The polarization state of beam 114 has rotated 45 degree counterclockwise by Faraday rotator 105.Two the first beamlets of beam beamlet, 113 He at this time The polarization state of second beamlet 114 is identical, and (optical axis of the second birefringece crystal 106 hangs down relative to the second birefringece crystal 106 Directly in horizontal plane) be o light (polarization direction is perpendicular to optical axis), two light beams do not occur deviation by the second birefringece crystal 106.Then two beam beamlet the first beamlets 113 and the second beamlet 114 by the second half-wave plate to after 107, the first sub-light The polarization state of beam 113 and the second beamlet 114 is orthogonal, is finally incident on right-angle prism 108 and is totally reflected.First beamlet Position exchanges after being reflected with the second beamlet, and again by the second half-wave plate to 107, at this time two beam beamlets first Beamlet 113 is identical with the polarization state of the second beamlet 114, and is e light (polarization for the second birefringece crystal 106 The plane being oriented parallel to where optical axis), the two-fold by second of deviation occurs for the first beamlet 113 and the second beamlet 114 Crystal 106 is penetrated, deflects into the first beamlet 113 and the second beamlet 114 from the extended line for being located at input collimater 110 On the extended line of the first output collimater 109.Then again by Farady rotator 105, since faraday is revolved The polarization state of the irreversibility of luminescent crystal 105, the first beamlet 113 and the second beamlet 114 continues to be rotated counterclockwise 45 degree. Then by the first half-wave plate to after 103, the polarization state of the first beamlet 113 and the second beamlet 114 is orthogonal, is incident on First birefringece crystal 102 synthesizes single beam, after transferring by prism 101, is incident on the first output collimator 109, finally quilt Guidance output.
Fig. 1 b and Fig. 3 describe magneto-optic shutter and light beam are input to second output terminal collimator from input collimater 110 The applicable cases of 111 outputs.
The female light beam 112 projected from input collimater 110 is incident on the first birefringece crystal 102, the first birefringent crystalline substance The optical axis of body 102 is located at horizontal plane (i.e. in paper), the female light beam 112 projected by input collimater 110 can be decomposed into Two orthogonal and spatially separated parallel beamlets of polarization direction.The polarization direction of first beamlet 113 (e light) is parallel In the plane (paper) where optical axis, the polarization direction of the second beamlet 114 (o light) is perpendicular to optical axis.Wherein the second beamlet 114 do not occur deviation by the first birefringece crystal 102, the first beamlet 113 then generates a sidesway.First beamlet later 113 and second beamlet 114 first beamlet 113 and the second son made to 103 to 103, first half-wave plates by the first half-wave plate The polarization state direction of light beam 114 is identical.Identical beamlet the first beamlet 113 of following two beams polarization state and the second beamlet 114 are incident on Farady rotator 105, and 105 externally-applied magnetic field of Farady rotator disappears at this time, 113 He of the first beamlet The polarization state of second beamlet 114 is relative to first beamlet 113 in the first half-wave plate is to 103 and the second beamlet 114 Polarization state has rotated clockwise 45 degree by Faraday rotator 105.Two the first beamlets of beam beamlet 113 and the second son at this time The polarization state of light beam 114 is identical, and (optical axis of the second birefringece crystal 106 is perpendicular to water relative to the second birefringece crystal 106 Plane) it is o light (polarization direction is parallel to paper), two light beams generation deviation passes through the second birefringece crystal 106, makes first Beamlet 113 and the second beamlet 114 are deflected into from the extended line for being located at input collimater 110 positioned at second output terminal standard On the extended line of straight device 111.Then two light beams by the second half-wave plate to after 107, the first beamlet 113 and the second beamlet 114 polarization state is orthogonal, is finally incident on right-angle prism 108 and is totally reflected, the first beamlet 113 and the second beamlet After 114 are reflected, position is exchanged, again by the second half-wave plate to 107, the first beamlet 113 and the second sub-light at this time 114 polarization state of beam is identical, and is o light for the second birefringece crystal 106, and deviation does not occur passes through the second birefringent crystalline substance Body 106.Then again by Farady rotator 105, due to the irreversibility of Farady rotator, the polarization of two light beams State continuation is rotated clockwise 45 degree.Then by the first half-wave plate to after 103, the polarization state of two light beams is orthogonal, incident Single beam is synthesized to the first birefringece crystal 102, after transferring by prism 101, is incident on second output terminal collimator 111, most After be guided to export.
In the present embodiment, due to the presence of faraday's crystal, magneto-optic shutter is irreversible.
The utility model is illustrated above by specific embodiment, but the utility model is not limited only to this, also Cover the various modifications that thought according to the present utility model is done in the range of the technical solution of the utility model.Above by The utility model is illustrated in specific embodiment, but the utility model is not limited only to this, also covers practical new according to this The various modifications that the thought of type is done in the range of the technical solution of the utility model.

Claims (6)

1. a kind of reflection-type magneto-optic switch, the reflection-type magneto-optic switch includes:
Female light beam is inputted the reflection-type magneto-optic and switched by input collimater, the input collimater;
First output collimater and second output terminal collimator, first output collimater and second output terminal collimator Light beam is exported into the reflection-type magneto-optic switch;
Prism, the prism can make light beam that deviation occur;
First birefringece crystal, the optical axis of first birefringece crystal are located at horizontal plane, and first birefringece crystal is by double Refractive material is constituted, and when female light beam is injected first birefringece crystal by the input collimater, described first is two-fold Penetrating crystal and female light beam is separated into two beam polarization states is orthogonal beamlet;
First half-wave plate pair, first half-wave plate to can by the two beam polarization states passed through from left to right be orthogonal light beam become The identical light beam of two beam polarization states;
The combination of Farady rotator and magnetic element, the magnetic element are controllable magnetic element, and the magnetic element can To apply saturation magnetic field on the Farady rotator or not apply magnetic field, the Farady rotator be applied it is full With can make the light beam for inputting the Farady rotator behind magnetic field when not being applied magnetic field with the Farady rotator Become different polarization states;
Second birefringece crystal, the optical axis of second birefringece crystal are located at horizontal plane, and second birefringece crystal is by double Refractive material is constituted, and second birefringece crystal can make light beam that deviation occur or directly pass through without deviation;
Second half-wave plate pair, light beam change of second half-wave plate to two beams passed through from left to right can be had to identical polarization state Be orthogonal light beam for two beam polarization states, second half-wave plate to can by the two beam polarization states passed through from right to left be it is orthogonal Light beam becomes the identical light beam of two beam polarization states;
Right-angle prism, the right-angle prism can reflect light beam to change the direction of light beam;
It is characterized in that, the optical element of the reflection-type magneto-optic switch is set gradually from left to right are as follows: the input terminal collimation The combination of device, first output collimater, the second output terminal collimator, the prism, the first birefringent crystalline substance Body, first half-wave plate pair, the combination of the Farady rotator and magnetic element, second birefringece crystal, institute State the second half-wave plate pair, the right-angle prism.
2. reflection-type magneto-optic switch as described in claim 1, which is characterized in that first birefringece crystal is side's solution Stone.
3. reflection-type magneto-optic switch as described in claim 1, which is characterized in that the Farady rotator is by the magnetic Property element apply saturation magnetic field when, rotate 45 degree counterclockwise by the polarization state of the light beam of the Farady rotator.
4. reflection-type magneto-optic switch as described in claim 1, which is characterized in that the Farady rotator is not described When magnetic element applies magnetic field, 45 degree are rotated clockwise by the polarization state of the light beam of the Farady rotator.
5. reflection-type magneto-optic switch as described in claim 1, which is characterized in that the light beam of the input collimater input The optical element of process is successively are as follows: first birefringece crystal, first half-wave plate pair, the Farady rotator and The combination of magnetic element, second birefringece crystal, second half-wave plate pair, the right-angle prism, second half-wave Piece pair, second birefringece crystal, the combination of the Farady rotator and magnetic element, first half-wave plate pair, Then first birefringece crystal, the prism are projected from first output collimater.
6. reflection-type magneto-optic switch as described in claim 1, which is characterized in that the light beam of the input collimater input The optical element of process is successively are as follows: first birefringece crystal, first half-wave plate pair, the Farady rotator and The combination of magnetic element, second birefringece crystal, second half-wave plate pair, the right-angle prism, second half-wave Piece pair, second birefringece crystal, the combination of the Farady rotator and magnetic element, first half-wave plate pair, Then first birefringece crystal, the prism are projected from the second output terminal collimator.
CN201821301718.4U 2018-08-10 2018-08-10 Reflection-type magneto-optic switch Active CN208432822U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201821301718.4U CN208432822U (en) 2018-08-10 2018-08-10 Reflection-type magneto-optic switch

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201821301718.4U CN208432822U (en) 2018-08-10 2018-08-10 Reflection-type magneto-optic switch

Publications (1)

Publication Number Publication Date
CN208432822U true CN208432822U (en) 2019-01-25

Family

ID=65097778

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201821301718.4U Active CN208432822U (en) 2018-08-10 2018-08-10 Reflection-type magneto-optic switch

Country Status (1)

Country Link
CN (1) CN208432822U (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN111347158A (en) * 2020-03-20 2020-06-30 华中科技大学 Compound welding set of semiconductor blue light laser and fiber laser

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN111347158A (en) * 2020-03-20 2020-06-30 华中科技大学 Compound welding set of semiconductor blue light laser and fiber laser

Similar Documents

Publication Publication Date Title
TWI810703B (en) Device for combining light beams which interact with adjacently arranged pixels of a light modulator
CN104635347B (en) A kind of faraday rotation mirror unrelated with wavelength and temperature
US6757101B2 (en) None-mechanical dual stage optical switches
WO1997022034A1 (en) Fibre optic circulator
US6757451B2 (en) Optical circulator
US6396629B1 (en) Multi-functional optical device utilizing multiple birefringent plates and a non-linear interferometer
CN103324008A (en) Projector
CN102929001B (en) Magneto-optic shutter
US9915833B2 (en) Faraday rotator mirror
CN208432822U (en) Reflection-type magneto-optic switch
CN103424896B (en) Optical path control device
US6504642B1 (en) Birefringent optical device
US6747797B2 (en) Loop optical circulator
US6795245B2 (en) Polarization independent magnetooptic switches
CN102183849A (en) High-speed and high-precision all-fiber polarization control device
CN203881971U (en) Solid-state high-speed 1x2 switch
CN102736275B (en) Reflection-type magneto-optical switch
US7224860B2 (en) Multi-port optical switches
US6735016B1 (en) Electro-optically controllable polarization insensitive optical device
JP3008964B2 (en) Light switch
CN1268967C (en) Miniature 2x2 magneto-optic switch
CN101672985B (en) Magneto-optic switch
CN202693929U (en) 2*2 high-speed mini-type all-solid magneto optical switch
CN208833951U (en) It is a kind of with photoswitch performance and adjustable two-way optical circulator
CN109844615B (en) Optical isolator

Legal Events

Date Code Title Description
GR01 Patent grant
GR01 Patent grant