CN103969737B - Asymmetric birefringence vortex fiber and manufacturing method of asymmetric birefringence vortex fiber - Google Patents
Asymmetric birefringence vortex fiber and manufacturing method of asymmetric birefringence vortex fiber Download PDFInfo
- Publication number
- CN103969737B CN103969737B CN201310029915.0A CN201310029915A CN103969737B CN 103969737 B CN103969737 B CN 103969737B CN 201310029915 A CN201310029915 A CN 201310029915A CN 103969737 B CN103969737 B CN 103969737B
- Authority
- CN
- China
- Prior art keywords
- vortex
- optical fiber
- asymmetric
- double
- fiber
- 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 - Fee Related
Links
- 239000000835 fiber Substances 0.000 title claims abstract description 36
- 238000004519 manufacturing process Methods 0.000 title abstract 2
- 239000013307 optical fiber Substances 0.000 claims abstract description 75
- 230000005540 biological transmission Effects 0.000 claims abstract description 14
- 239000000463 material Substances 0.000 claims abstract description 13
- 230000003287 optical effect Effects 0.000 claims description 9
- 239000002019 doping agent Substances 0.000 claims description 7
- 230000009977 dual effect Effects 0.000 abstract 2
- 239000002245 particle Substances 0.000 abstract 1
- 230000010287 polarization Effects 0.000 description 10
- 238000002360 preparation method Methods 0.000 description 10
- 238000010586 diagram Methods 0.000 description 8
- 230000008878 coupling Effects 0.000 description 4
- 238000010168 coupling process Methods 0.000 description 4
- 238000005859 coupling reaction Methods 0.000 description 4
- 238000000034 method Methods 0.000 description 3
- 238000005516 engineering process Methods 0.000 description 2
- 238000010438 heat treatment Methods 0.000 description 2
- 238000012805 post-processing Methods 0.000 description 2
- 238000012552 review Methods 0.000 description 2
- 238000005491 wire drawing Methods 0.000 description 2
- 238000004891 communication Methods 0.000 description 1
- 230000007547 defect Effects 0.000 description 1
- 238000005315 distribution function Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000003780 insertion Methods 0.000 description 1
- 230000037431 insertion Effects 0.000 description 1
- 230000003993 interaction Effects 0.000 description 1
- 239000004531 microgranule Substances 0.000 description 1
- 238000012576 optical tweezer Methods 0.000 description 1
- 230000010363 phase shift Effects 0.000 description 1
Landscapes
- Optical Fibers, Optical Fiber Cores, And Optical Fiber Bundles (AREA)
Abstract
The invention discloses an asymmetric birefringence vortex fiber and a manufacturing method of the asymmetric birefringence vortex fiber. The asymmetric birefringence vortex fiber is formed by drawing an optical fiber perform with a single stress area or dual stress areas in a rotary mode, and therefore the asymmetric birefringence vortex fiber has a single spiral stress area or dual spiral stress areas; in addition, due to asymmetric distribution of the stress areas or different materials of the stress areas, spirally-distributed asymmetric stress birefringence is generated in a fiber core of the asymmetric birefringence vortex fiber, a radial phase difference of transmission light waves is accordingly formed, the light waves transmitted in the asymmetric birefringence vortex fiber can accordingly obtain the orbital annular momentum, vortex phase transmission is generated, and a similar vortex light transmission mode is achieved. The asymmetric birefringence vortex fiber overall has the advantages of being tiny in structure, flexible in operation, stable in system, high in interference resistant capacity and the like, and can be used for vortex beam generation, particle control, sensing application and the like.
Description
(1) technical field
The present invention relates to a kind of optical fiber and its technology of preparing, and in particular to a kind of asymmetric double refraction vortex optical fiber and its system
Preparation Method, belongs to technical field of optical fiber.
(2) background technology
One of vortex beams be noteworthy characterized by with orbital angular momentum (Physical Review A, 1992,45 (11)：
8185-8189), therefore it is widely studied in recent years, and has obtained in communication, optical tweezer, Atomic Manipulation and microtechnique greatly
Using.Generate vortex beams most common process be use spatial light modulator (Optics Express, 2008,16 (21)：
16984-16992), however spatial light modulator is typically bulky, it is expensive, and need to realize light in free space
Coupling, thus brings many inconvenience.
And the vortex photoproduction for being based on optical fiber grow up to be a useful person then on remote interaction and system compact have more advantage.Researchers make
With acoustics long-period gratings (Physical Review Letters, 2006,96 (4)：43604) or using in multimode fibre
In induced pressure (Applied Optics, 1998,37 (3)：469-472) realize vortex optical transmission mode.But in light
Mode Coupling can destroy orbital angular momentum pattern in fibre, so as to cause multipath interference.In most multimode fibres, TE/TM
Pattern and the HE for needing21Pattern coexists, and so they can generate linear polarization pattern (LP through Mode Coupling in outfan
Pattern), LP patterns are not the real eigen mode of optical fiber, and it can not carry orbital angular momentum.Therefore, document (Optics
Letters, 2012,37 (13)：2451-2453) report using micro-bend grating to slacken high-order LP11The generation of pattern, and then
Input pattern is converted into required HE21Pattern, ultimately generates highly purified vortex beams.
Preferably standard single-mode fiber has a good geometry circular symmetry, thus the basic mode HE for being transmitted11It is orthogonal mode
The double degenerate mode of formula.But in actual fiber, due to the presence of defect, this double degenerate is destroyed, so as to cause
Mode birefringence, in order to maintain this mode polarization, people to devise polarization maintaining optical fibre in standard single-mode fiber.Polarization maintaining optical fibre makesWithThe effective refractive index of pattern is different, propagation constant β of two orthogonal modesxWith βyDifference increases, two-mode coupling probability
Reduce, so if transmission light being linearly polarized on the parallel direction of one optical axis of optical fiber, then light will be always maintained at this
Plant polarization state to transmit in a fiber.
United States Patent (USP) (US20080101754) and European patent (EP1705503B1) propose a kind of fiber core refractive index only
With the gradient index fibre of azimuthal variation, this optical fiber can regard the space phase plate of longitudinal direction elongation as, using the optical fiber
Vortex beams can be generated.Although the vortex beams maker structure is extremely simple, it is extremely difficult to prepare this optical fiber,
Therefore the present invention is in polarization maintaining optical fibre technical foundation, it is proposed that a kind of Novel asymmetric birefringence vortex optical fiber, this vortex light
Fibre is prepared and is easier, and can produce class vortex beams.
(3) content of the invention
It is an object of the invention to provide it is a kind of generate vortex optical transmission mode asymmetric double refraction vortex optical fiber and
Its preparation method.
What the present invention was realized in：
One of vortex beams is noteworthy characterized by with orbital angular momentum, and in order to obtain orbital angular momentum, optical fiber must be taken
Band higher order pattern, for example, phase shift is two HE of ± pi/221The linear combination of pattern is capable of achieving orbital angular momentum pattern.By
There are single-screw or Double helix stressed zone, and two of Double helix stressed zone in the asymmetric double refraction vortex optical fiber of the present invention
The material adulterated in prestressing force rod is different, therefore the mal-distribution or the difference of stressed zone material of this stressed zone, results in
Asymmetric stress birefringence distribution in fibre core, and this is distributed in optical fiber longitudinal direction in the shape of a spiral, thus when light wave input
To after the optical fiber, can form that radial phase is poor, so that the light field wherein transmitted obtains orbital angular momentum, produce vortex phase and pass
It is defeated, realize class vortex optical transmission mode.
The asymmetric double refraction vortex optical fiber of the present invention is from the different of polarization maintaining optical fibre, in the present invention, due to stress
The mal-distribution in area or the difference of stressed zone material, are not in the linear polarization property of polarization maintaining optical fibre, but with spiral
The rotation of stressed zone, the polarization state that light wave is conducted in fibre core is also rotated with, and vortex optical transmission mode occurs.
Compared with prior art, advantages of the present invention is：
1st, the preparation of asymmetric double refraction vortex optical fiber is simple, can directly by the light with single-screw or Double helix stressed zone
Fine prefabricated rods rotation drawing is formed.
2nd, the refractive index Spiral distribution function and stressed zone dopant material of asymmetric double refraction vortex optical fiber is in preparation process
In be controllable, the final control being capable of achieving to generating class vortex beams feature.
3rd, asymmetric double refraction vortex optical fiber space pliability is fabulous, therefore can select in any suitable position and side
Upwards output class vortex beams, are easy in microgranule manipulation and the application for sensing.
(4) illustrate
Fig. 1 is the refraction vortex optical fiber schematic diagram of the asymmetric double with single-screw stressed zone；
Fig. 2 is the cross-sectional view that the asymmetric double with single-screw stressed zone reflects vortex optical fiber；
Fig. 3 is the peacekeeping (b) two of stress birfringence (a) three that the asymmetric double with single-screw stressed zone reflects vortex optical fiber
Dimension schematic diagram；
Fig. 4 is the light intensity transmission schematic diagram of the refraction vortex optical fiber of the asymmetric double with single-screw stressed zone；
Fig. 5 is that the asymmetric double with single-screw stressed zone reflects vortex optical fiber in Z=900 μm of (a), (b) Z=1000 μ
The PHASE DISTRIBUTION figure of m, Z=1100 μm of (c) and (d) Z=1200 μm of cross-section；
Fig. 6 is that the preform with single stress area prepares schematic diagram；
Fig. 7 is that the refraction vortex optical fiber of the asymmetric double with single-screw stressed zone prepares schematic diagram；
Fig. 8 is the refraction vortex optical fiber schematic diagram of the asymmetric double with Double helix stressed zone；
Fig. 9 is the cross-sectional view that the asymmetric double with Double helix stressed zone reflects vortex optical fiber；
Figure 10 is the peacekeeping (b) of stress birfringence (a) three that the asymmetric double with Double helix stressed zone reflects vortex optical fiber
Two-dimensional representation；
Figure 11 is the preform preparation method schematic diagram with double stressed zones；
Figure 12 is the preparation method schematic diagram that the asymmetric double with Double helix stressed zone reflects vortex optical fiber；
Figure 13 is the connection signal that the tail optical fiber with light source and the asymmetric double with single-screw stressed zone reflect vortex optical fiber
Figure.
Figure 14 is the connection signal that the tail optical fiber with light source and the asymmetric double with Double helix stressed zone reflect vortex optical fiber
Figure.
(5) specific embodiment
Illustrate below in conjunction with the accompanying drawings and the present invention is described in more detail：
With reference to Fig. 1-Fig. 5, what the first embodiment of the invention was realized in.
Describe how light wave is producing vortex after the asymmetric double refraction vortex optical fiber that one section of present invention is provided first
The ultimate principle of light field.One section of asymmetric double refraction vortex optical fiber is taken, the optical fiber includes covering 1, fibre core 2 and single-screw stressed zone
3.Due to the presence of single-screw stressed zone 3, stress analysis is carried out to the cross section of optic fibre shown in Fig. 2 and be can be obtained by such as Fig. 3 institutes
(in Fig. 3 (a), column fence area encompassed represents core region, and Z axis represent that stress is double for the stress birfringence distribution shown
Refraction size Ny-Nx, in Fig. 3 (b), gray scale size then represents stress birfringence size), it is this non-right due to existing in fibre core
The stress birfringence distribution of title, so when light source 4 is input into one end of the optical fiber, the optical fiber can generate class vortex optical transport
Pattern, the transmission of its light intensity as shown in figure 4, Z=900 μm, 1000 μm, 1100 μm and 1200 μm cross-section PHASE DISTRIBUTION such as
Shown in Fig. 5, it can be seen that, in the optical fiber, conduction light wave has vortex phase, and it is a species vortex beams.
Next provides the preparation method that asymmetric double reflects vortex optical fiber.This asymmetric double with single-screw stressed zone
The preparation process of refraction vortex optical fiber can be divided into following step (such as Fig. 6 and Fig. 7)：
Step 1：Such as Fig. 6, an eccentric orfice 7 is squeezed in the preform 6 containing core 5, then stressed zone prefabricated rods 8
In insertion eccentric orfice 7, the preform 9 with single stress area is thus obtained；
Step 2：Such as Fig. 7, preform 9 is positioned on wire-drawer-tower, in being total to for vertical distraction power 10 and twisting resistance 11
Torsion wire drawing is carried out under same-action, is prepared into the non-right of single-screw stressed zone after heating and corresponding post processing 12
Claim birefringence vortex optical fiber 13.
With reference to Fig. 8 and Fig. 9, the first embodiment, the asymmetric double refraction of second embodiment of the invention are different from
Vortex optical fiber has two stressed zones 14 and 15, forms Double helix stressed zone structure.For this with Double helix stressed zone
Asymmetric double reflects vortex optical fiber, and Figure 10 is given at the stress birfringence scattergram in fibre core, as can be seen from the figure its stress
Birefringent excursion is greater than the stress birfringence that the asymmetric double with single-screw stressed zone reflects vortex fiber core
Excursion (Fig. 3), thus the ability that this optical fiber produces vortex phase is more projected.
The preparation process of this refraction of the asymmetric double with Double helix stressed zone vortex optical fiber can be divided into following step
Suddenly (such as Figure 11 and Figure 12)：
Step 1：Such as Figure 11, two symmetrical eccentric orfices 7 are squeezed in containing core fibre prefabricated rods 6, then two doping
The different stressed zone prefabricated rods 16 and 17 of material are inserted respectively in two symmetrical eccentric orfices 7, thus obtain having double stressed zones
Preform 18；
Step 2：Such as Figure 12, preform 18 is positioned on wire-drawer-tower, in vertical distraction power 10 and twisting resistance 11
Torsion wire drawing is carried out under collective effect, is prepared into the non-of Double helix stressed zone after heating and corresponding post processing 12
Symmetrical birefringence vortex optical fiber 19.
Embodiment 1：
1st, prepared by optical fiber：Method for preparing optical fiber according to the first embodiment is prepared with the non-of single-screw stressed zone
Symmetrical birefringence vortex optical fiber 13；
2nd, light source couples：The refraction vortex of the asymmetric double with the single-screw stressed zone optical fiber 13 for preparing is cut
Cut, be then aligned, weld with the single-mode fiber 20 with light source tail optical fiber, as shown in figure 13；
3rd, vortex beams are generated：Will be in the refraction vortex light of the asymmetric double with single-screw stressed zone after input laser 21
Realize that vortex optical mode is transmitted in fine 13, and can be in optical fiber end output class vortex beams.
Embodiment 2：
1st, prepared by optical fiber：Method for preparing optical fiber according to second embodiment is prepared with the non-of Double helix stressed zone
Symmetrical birefringence vortex optical fiber 19；
2nd, light source couples：The refraction vortex of the asymmetric double with the Double helix stressed zone optical fiber 19 for preparing is cut
Cut, be then aligned, weld with the single-mode fiber 20 with light source tail optical fiber, as shown in figure 14；
3rd, vortex beams are generated：Will be in the refraction vortex light of the asymmetric double with Double helix stressed zone after input laser 21
Realize that vortex optical mode is transmitted in fine 19, and can be in optical fiber end output class vortex beams.
Claims (5)
1. a kind of asymmetric double reflects vortex optical fiber, it is characterized in that：Described asymmetric double refraction vortex optical fiber includes fibre core, bag
Layer and stressed zone, its fibre core be in cladding center position, stressed zone can be single stress area, alternatively double stressed zones, single stress area
It is only positioned between fibre core and covering outer wall, and double stressed zones are then symmetrically distributed in the both sides of fibre core, and two of double stressed zones
The dopant material of prestressing force rod is different, and whole stressed zone is distributed in the shape of a spiral around optical fiber central axis line, so as to be formed in a fiber
Single-screw or Double helix stressed zone, the mal-distribution of this stressed zone or the difference of stressed zone material, result in fibre core
The distribution of asymmetric stress birefringence, and this is distributed in optical fiber longitudinal direction in the shape of a spiral, thus after light wave is input to the optical fiber,
Radial phase can be formed poor, so as to obtain orbital angular momentum, produce vortex phase transmission, realize class vortex optical transmission mode.
2. asymmetric double according to claim 1 reflects vortex optical fiber, it is characterized in that：Described single stress area dopant material
It can be the dopant material in conventional Stress Profile for Polarization-Maintaining area.
3. asymmetric double according to claim 1 reflects vortex optical fiber, it is characterized in that：Described double stressed zone dopant materials
It is characterized in that：The coefficient of expansion of one stressed zone dopant material is more than covering；The coefficient of expansion of another stressed zone dopant material
Less than covering.
4. asymmetric double according to claim 1 reflects vortex optical fiber, it is characterized in that：Described single-screw or Double helix should
Pitch H in power area meets following relation：π (the β of H ＞ 21-β2)-1, wherein β1Represent the transmission of fibre core basic mode, β2Represent covering
The transmission of basic mode.
5. asymmetric double according to claim 1 reflects vortex optical fiber, it is characterized in that：Described single-screw or Double helix should
The period profile in power area is characterized in that：Constant cycle or variable period.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN201310029915.0A CN103969737B (en) | 2013-01-28 | 2013-01-28 | Asymmetric birefringence vortex fiber and manufacturing method of asymmetric birefringence vortex fiber |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| CN201310029915.0A CN103969737B (en) | 2013-01-28 | 2013-01-28 | Asymmetric birefringence vortex fiber and manufacturing method of asymmetric birefringence vortex fiber |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| CN103969737A CN103969737A (en) | 2014-08-06 |
| CN103969737B true CN103969737B (en) | 2017-04-12 |
Family
ID=51239452
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CN201310029915.0A Expired - Fee Related CN103969737B (en) | 2013-01-28 | 2013-01-28 | Asymmetric birefringence vortex fiber and manufacturing method of asymmetric birefringence vortex fiber |
Country Status (1)
| Country | Link |
|---|---|
| CN (1) | CN103969737B (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN110045459A (en) * | 2018-01-15 | 2019-07-23 | 上海交通大学 | The method of transmission rail angular momentum in the waveguide of photon integrated chip |
Families Citing this family (13)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN104503020A (en) * | 2014-12-19 | 2015-04-08 | 华中科技大学 | Longitudinal spiral mode transfer optical fiber |
| CN105182468B (en) * | 2015-09-23 | 2019-01-11 | 上海大学 | Leafy stressed zone circle single polarization fiber and preparation method thereof |
| CN105572794B (en) * | 2016-03-08 | 2019-03-05 | 哈尔滨工程大学 | A kind of triangle core rotational field optical fiber and preparation method thereof |
| CN105750181B (en) * | 2016-03-11 | 2017-12-19 | 南京大学 | A kind of device using acoustic metamaterial generation sound rotational field |
| US11347069B2 (en) | 2016-11-22 | 2022-05-31 | Lumentum Operations Llc | Rotary optical beam generator |
| US10429584B2 (en) * | 2016-11-22 | 2019-10-01 | Lumentum Operations Llc | Rotary optical beam generator |
| CN109752790B (en) * | 2017-11-03 | 2020-11-06 | 桂林电子科技大学 | Coaxial double-waveguide optical fiber capable of generating vortex rotation and annular field and preparation method thereof |
| CN109752789A (en) * | 2017-11-03 | 2019-05-14 | 桂林电子科技大学 | Particle light manipulation device based on the coaxial double wave guiding fiber of toroidal cores |
| US11536895B2 (en) | 2018-11-28 | 2022-12-27 | Shenzhen University | Method for manufacturing polarization-independent orbital angular momentum modulator |
| CN109799571B (en) * | 2018-12-12 | 2021-04-30 | 桂林电子科技大学 | Particle light control device based on annular core coaxial spiral waveguide fiber |
| CN109912193A (en) * | 2019-03-19 | 2019-06-21 | 中国电力科学研究院有限公司 | Photonic crystal fiber and preparation method thereof |
| CN112147739B (en) * | 2019-06-26 | 2022-11-29 | 上海康阔光智能技术有限公司 | Bending-resistant and torsion-resistant optical fiber for optical fiber gyroscope, and sensing optical fiber ring and optical fiber gyroscope using same |
| CN113376736B (en) * | 2021-06-18 | 2022-09-02 | 天津工业大学 | Vortex integrated multiplexing/demultiplexing optical fiber suitable for 6G communication |
Family Cites Families (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6766088B2 (en) * | 2000-05-01 | 2004-07-20 | Sumitomo Electric Industries, Ltd. | Optical fiber and method for making the same |
| JP3628299B2 (en) * | 2002-02-05 | 2005-03-09 | 三菱電線工業株式会社 | Double-clad fiber and method for producing double-clad fiber |
| JP5778939B2 (en) * | 2011-02-14 | 2015-09-16 | 株式会社フジクラ | Manufacturing method of optical fiber |
-
2013
- 2013-01-28 CN CN201310029915.0A patent/CN103969737B/en not_active Expired - Fee Related
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| CN110045459A (en) * | 2018-01-15 | 2019-07-23 | 上海交通大学 | The method of transmission rail angular momentum in the waveguide of photon integrated chip |
Also Published As
| Publication number | Publication date |
|---|---|
| CN103969737A (en) | 2014-08-06 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| CN103969737B (en) | Asymmetric birefringence vortex fiber and manufacturing method of asymmetric birefringence vortex fiber | |
| CN103969738B (en) | Based on inclined hole melting-embedding core vortex optical fiber of spiral and preparation method thereof | |
| CN103969739B (en) | Vortex optical fiber based on linear refractive index distribution and preparation method thereof | |
| Tan et al. | Photonic circuits written by femtosecond laser in glass: improved fabrication and recent progress in photonic devices | |
| US7289709B2 (en) | Photonic crystal fibres comprising stress elements | |
| AU2020100964A4 (en) | A vortex optical fiber with spiral eccentric hole structure surrounding the center-core and its preparation method | |
| DE69824525T2 (en) | Sheath-pumped fiber structures | |
| US8463094B2 (en) | Chiral fiber polarizer | |
| CN105572794B (en) | A kind of triangle core rotational field optical fiber and preparation method thereof | |
| CN109752790A (en) | A kind of producible vortex light and the coaxial double wave guiding fiber of toroidal field and preparation method thereof | |
| KR20010113696A (en) | Improvements in or relating to photonic crystal fibres | |
| Zhao et al. | Advances on mode-coupling theories, fabrication techniques, and applications of the helical long-period fiber gratings: A review | |
| WO2011061309A1 (en) | Birefringent micro-structured optical fiber for sensor application | |
| CN101788698B (en) | Quasi-rectangular multi-core polarization-preserving fiber and manufacturing method thereof | |
| CN107462948A (en) | Annular fiber with unsymmetrical grating and its in the aborning application of orbital angular momentum | |
| Lian et al. | OAM beams generation technology in optical fiber: A review | |
| CN106019475B (en) | A kind of less fundamental mode optical fibre device | |
| Alexeyev et al. | Generation of optical vortices in layered helical waveguides | |
| CN113281845A (en) | OAM photon lantern based on spiral tapered fiber bundle and manufacturing and application thereof | |
| CN102749304A (en) | High sensitivity photonic crystal fiber refractive index sensor and method for preparing same | |
| Wang et al. | Transmission and generation of orbital angular momentum modes in optical fibers | |
| CN100456061C (en) | Air conducting double-core photon band gap optical fiber | |
| CN101622560A (en) | Photonic band gap fiber | |
| CN109752796A (en) | Graded index rotational field optical fiber | |
| EP2502102A1 (en) | Birefringent micro-structured optical fiber for sensor application |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| C06 | Publication | ||
| PB01 | Publication | ||
| C10 | Entry into substantive examination | ||
| SE01 | Entry into force of request for substantive examination | ||
| GR01 | Patent grant | ||
| GR01 | Patent grant | ||
| TR01 | Transfer of patent right |
Effective date of registration: 20190719 Address after: 541004 the Guangxi Zhuang Autonomous Region golden Guilin Qixing District Road No. 1 Patentee after: GUILIN University OF ELECTRONIC TECHNOLOGY Address before: 214131 8th Floor, Building A1, National Sensing Information Center, No. 999 Gaolang East Road, Binhu District, Wuxi City, Jiangsu Province Patentee before: WUXI WANRUN PHOTON TECHNOLOGY CO.,LTD. |
|
| TR01 | Transfer of patent right | ||
| DD01 | Delivery of document by public notice |
Addressee: Yuan Libo Document name: Notice of Termination of Patent Rights |
|
| DD01 | Delivery of document by public notice | ||
| CF01 | Termination of patent right due to non-payment of annual fee |
Granted publication date: 20170412 |
|
| CF01 | Termination of patent right due to non-payment of annual fee |