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CN108732678B - Photonic crystal fiber - Google Patents

Photonic crystal fiber Download PDF

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Publication number
CN108732678B
CN108732678B CN201810537357.1A CN201810537357A CN108732678B CN 108732678 B CN108732678 B CN 108732678B CN 201810537357 A CN201810537357 A CN 201810537357A CN 108732678 B CN108732678 B CN 108732678B
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cladding
layer
core layer
photonic crystal
ring
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CN108732678A (en
Inventor
雷雨
许勋
贾宏志
庚志浩
刘星
刘刚
贾春华
沈志威
柴俊宇
王宁
涂建坤
孟丛
张坤
高聪
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University of Shanghai for Science and Technology
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University of Shanghai for Science and Technology
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    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/02Optical fibres with cladding with or without a coating
    • G02B6/02295Microstructured optical fibre
    • G02B6/02314Plurality of longitudinal structures extending along optical fibre axis, e.g. holes
    • G02B6/02342Plurality of longitudinal structures extending along optical fibre axis, e.g. holes characterised by cladding features, i.e. light confining region
    • G02B6/02361Longitudinal structures forming multiple layers around the core, e.g. arranged in multiple rings with each ring having longitudinal elements at substantially the same radial distance from the core, having rotational symmetry about the fibre axis
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B6/00Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
    • G02B6/02Optical fibres with cladding with or without a coating
    • G02B6/036Optical fibres with cladding with or without a coating core or cladding comprising multiple layers

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  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Optical Fibers, Optical Fiber Cores, And Optical Fiber Bundles (AREA)

Abstract

本发明公开了一种光子晶体光纤,其特征在于,包括:从内自外的芯层、包层以及涂覆层,光纤的横截面为圆形,芯层、包层以及涂覆层均同心,芯层位于光纤的最内层,芯层横截面的中心为圆形孔,包层内均匀设置多个半圆形的气孔,包层包括5个包层环,每个包层环由相同大小的半圆形的气孔依次连接形成,包层环内的半圆形的气孔的大小从内圈到外圈依次递增,涂覆层位于最外层,包层采用二氧化硅晶体材料制成,芯层采用二氧化硅晶体材料或者肖特玻璃(schott SF57)材料制成。本发明的电子晶体光纤可以传输多个轨道角动量模式,模式组的有效折射率差达到10‑3量级。

Figure 201810537357

The invention discloses a photonic crystal optical fiber, which is characterized by comprising: a core layer, a cladding layer and a coating layer from the inside to the outside, the cross section of the optical fiber is circular, and the core layer, the cladding layer and the coating layer are all concentric , the core layer is located in the innermost layer of the fiber, the center of the cross section of the core layer is a circular hole, and a plurality of semicircular air holes are evenly arranged in the cladding layer. The semicircular pores of different sizes are connected in turn to form. The size of the semicircular pores in the cladding ring increases sequentially from the inner ring to the outer ring. The coating layer is located in the outermost layer, and the cladding layer is made of silicon dioxide crystal material. , the core layer is made of silicon dioxide crystal material or Schott glass (schott SF57) material. The electronic crystal fiber of the present invention can transmit multiple orbital angular momentum modes, and the effective refractive index difference of the mode group reaches the order of 10-3 .

Figure 201810537357

Description

Photonic crystal fiber
Technical Field
The invention belongs to the field of communication, and particularly relates to a photonic crystal fiber.
Background
Orbital Angular momentum (Orbital Angular mometer) is another important parameter of photons in addition to the traditional wavelength, polarization, etc. parameters. With the continuous development of wavelength division multiplexing, time division multiplexing, code division multiplexing and other technologies in the field of optical communication, the transmission data volume of the traditional optical fiber is close to saturation, and OAM provides a brand new degree of freedom for the multiplexing of light beams.
In an OAM optical fiber communication system, an optical fiber supporting OAM mode transmission is a key device. Photonic Crystal Fibers (PCFs), which have attracted considerable attention in recent years, have a relatively complex refractive index profile in their cross-section, usually containing a different arrangement of air holes whose dimensions and wavelength are of approximately the same order and which extend over the entire length of the device, can be confined to the core region of the Fiber at low refractive index. The appearance of photonic crystal fibers shows a new mechanism for controlling photons, and the research field of light transmission is greatly expanded. With the recent gradual and deep research on Photonic Crystal Fibers (PCF) and the gradual maturity of the manufacturing technology of the PCF, the photonic crystal fibers and the optical soliton theory inject the bobby mechanism into the development of the optical communication technology.
For an optical fiber transmitting OAM modes, more modes mean more channels are packed on a single frequency, which significantly increases the amount of information transmitted. In addition, in order to support the stable transmission of OAM modes in the fiber, the fiber must have a high effective index difference to avoid mutual coupling and degeneracy between the individual vector eigenmodes in the fiber. Many specially structured fibers have been proposed to support OAM mode transmission, but the effective refractive index difference between modes in these fibers is always 10-4And in order of magnitude, no more significant improvement can be obtained. Since the difference in effective refractive index between the modes cannot be increased, when OAM mode transmission occurs, odd-even eigenmode walk, birefringence and polarization mode dispersion may occur, affecting the mode purity and causing coupling or crosstalk between the modes.
Disclosure of Invention
The present invention has been made to solve the above problems, and an object of the present invention is to provide a photonic crystal fiber capable of increasing the number of transfer orbital angular momentum modes and reducing confinement loss.
The present invention provides a photonic crystal fiber having the features comprising:
the optical fiber comprises a core layer, a cladding layer and a coating layer from inside to outside, wherein the cross section of the optical fiber is circular, the core layer, the cladding layer and the coating layer are all concentric, and the cladding layer comprises a plurality of cladding rings.
In addition, the photonic crystal fiber provided by the present invention may further have the following characteristics: the core cross-section has a circular hole in the center.
In addition, the photonic crystal fiber provided by the present invention may further have the following characteristics: the core layer is uniformly provided with four same round air holes which are distributed in a cross shape.
In addition, the photonic crystal fiber provided by the present invention may further have the following characteristics: the cladding comprises 5 cladding rings, and the cross section of each cladding ring is a circular ring.
In addition, the photonic crystal fiber provided by the present invention may further have the following characteristics: a plurality of air holes with the same shape and size are uniformly arranged in the cladding ring.
In addition, the photonic crystal fiber provided by the present invention may further have the following characteristics: the cross section of the air hole is semicircular, and the semicircular parts are adjacent in sequence.
In addition, the photonic crystal fiber provided by the present invention may further have the following characteristics: the semicircular openings of the air holes in the cladding ring face the core layer.
In addition, the photonic crystal fiber provided by the present invention may further have the following characteristics: the size of the air holes in the cladding ring increases gradually from the inner ring to the outer ring.
In addition, the photonic crystal fiber provided by the present invention may further have the following characteristics: the core refractive index is greater than the cladding refractive index.
In addition, the photonic crystal fiber provided by the present invention may further have the following characteristics: the cladding layer is made of silica crystal material, and the core layer is made of silica crystal material or Schottky SF57 (Schottky SF57) material.
Action and Effect of the invention
The photonic crystal fiber has the beneficial effects that: the optical fiber can transmit a plurality of orbital angular momentum modes, and the refractive index difference of the mode group reaches 10-3Magnitude.
Drawings
FIG. 1 is a schematic cross-sectional view of a photonic crystal fiber according to the present invention;
FIG. 2 is a PCF with silica material for both the core and cladding, EH mode for the highest order EH mode16,1E of (A)ZField intensity distribution diagram;
FIG. 3 shows a PCF with a core layer made of silica material and a cladding layer made of Schottky glass material, in the highest-order EH mode of the EH mode19,1E of (A)ZField intensity distribution diagram;
FIG. 4 shows the | -HE of PCF with both core and cladding made of silicaa+1,1‐EHa‐1,1| an effective refractive index difference Δ n of 2,3,4,7,9,11,13,15,17efffA graph of the relationship as a function of wavelength;
FIG. 5 is the | -HE of PCF with core layer made of silica material and cladding layer made of Schottky glass materiala+1,1‐EHa‐1,1| an effective refractive index difference Δ n of 2,3,4,7,9,11,13,15,17efffA graph of the relationship as a function of wavelength;
FIG. 6 is a schematic cross-sectional view of a photonic crystal fiber according to the present invention.
Detailed Description
In order to make the technical means, the creation features, the achievement purposes and the effects of the invention easy to understand, the following embodiments are specifically described with reference to the attached drawings.
< example one >
FIG. 1 is a schematic cross-sectional view of a photonic crystal fiber according to the present invention.
The photonic crystal fiber is in a strip line shape. The photonic crystal fiber cross-sectional structure is shown in fig. 1, and the photonic crystal fiber 100 includes a core layer 10, a cladding layer 20 and a coating layer 30 from the inside to the outside. And the core layer 10, the cladding layer 20, and the coating layer 30 are all concentric.
The core layer 10 is located at the inner ring of the cross-sectional structure of the photonic crystal fiber 100. The center of the core layer 10 is provided with a circular hole, the radius of the circular hole ranges from 4 to 10 μm, and the thickness of the core layer 10 ranges from 1 to 2 μm. In this embodiment, the radius of the central circular hole is 6.7 μm, and the thickness of the core layer 10 is 1.5 μm.
The cladding 20 is located between the core layer 10 and the coating layer 30, and includes five cladding rings, which are, in order from the inner circumference to the outer circumference of the cladding 20, a first cladding ring 21, a second cladding ring 22, a third cladding ring 23, a fourth cladding ring 24, and a fifth cladding ring 25.
The cladding ring 21 is uniformly provided with a plurality of semicircular air holes 211, the air holes 211 are adjacent to each other in sequence, the radius of each air hole 211 ranges from 0.3 μm to 0.9 μm, and in this embodiment, the radius of each semicircular air hole 211 ranges from 0.6 μm.
The cladding ring 22 is uniformly provided with a plurality of semicircular air holes 221, the air holes 221 are adjacent in sequence, the radius of each air hole 221 ranges from 0.4 μm to 1 μm, and in the embodiment, the radius of each semicircular air hole 221 ranges from 0.65 μm.
The cladding ring 23 is uniformly provided with a plurality of semicircular air holes 231, the air holes 231 are adjacent in sequence, the radius of the air holes 231 ranges from 0.5 μm to 1.1 μm, and in the embodiment, the radius of the semicircular air holes 231 ranges from 0.7 μm.
The cladding ring 24 is uniformly provided with a plurality of semicircular air holes 241, the air holes 241 are adjacent in sequence, the radius of the air holes 241 ranges from 0.6 μm to 1.2 μm, and in this embodiment, the radius of the semicircular air holes 241 ranges from 0.75 μm.
The cladding ring 25 is uniformly provided with a plurality of semicircular air holes 251, the air holes 251 are adjacent in sequence, the radius of the air holes 251 ranges from 0.7 μm to 1.3 μm, and in the embodiment, the radius of the semicircular air holes 251 ranges from 0.8 μm.
The size of the air holes in the cladding ring increases gradually from the inner ring to the outer ring. The spacing between the cladding layers was the same and was 0.1. mu.m. The number of semi-circular holes in each cladding ring is the same, and in this embodiment, the number of holes is 42. The semicircular openings of the air holes in the cladding ring face the core layer.
The coating layer 30 is located at an outer ring of the cross-sectional structure of the photonic crystal fiber 100.
In the present embodiment, the core layer 10 and the cladding layer 20 of the photonic crystal fiber 100 are both made of silica crystal material.
FIG. 2 shows the PCF in EH mode16,1E of (A)ZField intensity distribution graph.
Effective refractive index difference Δ neffFor HEs with the same topological charge number a and the same mode field intensity pattern concentric ring number ba+1,bDie and EHa‐1,bAbsolute value of difference between real parts of effective refractive indices of modes, i.e. | HEa+1,b‐EHa‐1,b| a. Proved by experiments, the effective refractive index difference delta neffGreater than 10‐4In time, the mold HE can be effectively preventeda+1,bAnd EHa‐1,bDegenerating into linear polarization mode LPa,bAnd to intermodal crosstalk between them, resulting in loss or error of data, which is detrimental to fiber transmission. The larger the difference in effective refractive index is, the better. (in HE)a+1,bAnd EHa‐1,bAnd LPa,bWherein a represents the number of topological charges, b represents the number of concentric rings)
The number of all concentric rings in the photonic crystal fiber of the present invention is 1,
FIG. 4 shows the optical fiber |. HEa+1,1‐EHa‐1,1| an effective refractive index difference Δ n of 2,3,4,7,9,11,13,15,17efffGraph of wavelength dependence.
As shown in FIG. 4, the abscissa is wavelength (μm) and the ordinate is | -HEa+1,1‐EHa‐1,1Value of | i.e. the difference in effective refractive index Δ neffIt can be seen that all | HE's are in the 1.3 μm to 1.7 μm banda+1,1‐EHa‐1,1-the values of ═ 2,3,4,7,9,11,13,15,17 are all greater than 10‐3Effectively prevent them from synthesizing LPa,1The mode coupling is generated, and the transmission of more modes is facilitated.
By optimally designing the parameters of the fiber structure, the supported eigenmodes include HEa+1,1Die and EHa‐1,1(a-2-18) in 17 mode groups, where each mode group contains 4 OAM modes, plus TM0,1And TE0,1Collectively, 70 patterns are formed.
< example two >
In the second embodiment, the silica material of the core layer of the optical fiber in the first embodiment is changed to the schottky glass material, and the other materials are not changed.
FIG. 3 shows the PCF in EH mode19,1E of (A)ZField intensity distribution graph.
Effective refractive index difference Δ neffFor HEs with the same topological charge number a and the same mode field intensity pattern concentric ring number ba+1,bDie and EHa‐1,bAbsolute value of difference between real parts of effective refractive indices of modes, i.e. | HEa+1,b‐EHa‐1,b| a. Proved by experiments, the effective refractive index difference delta neffGreater than 10‐4In time, the mold HE can be effectively preventeda+1,bAnd EHa‐1,bDegenerating into linear polarization mode LPa,bAnd to intermodal crosstalk between them, resulting in loss or error of data, which is detrimental to fiber transmission. The larger the difference in effective refractive index is, the better. (in HE)a+1,bAnd EHa‐1,bAnd LPa,bWherein a represents the number of topological charges, b represents the number of concentric rings)
The number of all concentric rings in the photonic crystal fiber of the present invention is 1,
FIG. 5 is |. HEa+1,1‐EHa‐1,1| an effective refractive index difference Δ n of 2,3,4,7,9,11,13,15,17efffGraph of wavelength dependence.
As shown in FIG. 5, the abscissa is wavelength (μm) and the ordinate is | -HEa+1,1‐EHa‐1,1Value of | i.e. the difference in effective refractive index Δ neffIt can be seen that all | HE's are in the 1.3 μm to 1.7 μm banda+1,1‐EHa‐1,1-the values of ═ 2,3,4,7,9,11,13,15,17 are all greater than 10‐3Effectively prevent them from synthesizing LPa,1The mode coupling is generated, and the transmission of more modes is facilitated.
By optimally designing the parameters of the fiber structure, the supported eigenmodes include HEa+1,1Die and EHa‐1,1(a-2-21) for 20 mode groups, each mode group containing 4 OAM modes, plus TM0,1And TE0,1Collectively, 82 patterns are formed.
< example three >
FIG. 6 is a schematic cross-sectional view of a photonic crystal fiber according to the present invention.
As shown in fig. 6, in the optical fiber of the third embodiment, a plurality of identical circular air holes are added to the core layer based on the optical fiber of the second embodiment, the radius of the circle is 0.5 μm, and the distance between the center of the circle and the inner ring of the core layer is the same as the distance between the center of the circle and the outer ring of the core layer. In this embodiment, the number of the circles is 4, the circles are distributed in a cross shape, and the arrangement of the four circular air holes is beneficial to a mode that the core layer transmits more.
Effects and effects of the embodiments
According to the photonic crystal fiber related in the embodiment, the beneficial effects are as follows: the optical fiber can transmit a plurality of orbital angular momentum modes, and the refractive index difference of the mode group reaches 10-3Magnitude.
The above embodiments are preferred examples of the present invention, and are not intended to limit the scope of the present invention.

Claims (6)

1. A photonic crystal fiber, comprising:
a core layer, a cladding layer and a coating layer from inside to outside,
the cross section of the optical fiber is circular, the core layer, the cladding layer and the coating layer are all concentric,
wherein the cladding comprises a plurality of cladding rings,
four identical circular air holes which are distributed in a cross shape are uniformly arranged in the core layer,
a plurality of air holes with the same shape and size are uniformly arranged in the cladding ring, the cross section of each air hole is semicircular, the semicircles are adjacent in sequence,
the size of the air holes in the cladding ring is increased progressively from the inner ring to the outer ring.
2. A photonic crystal fiber according to claim 1, wherein:
wherein the center of the cross section of the core layer has a circular hole.
3. A photonic crystal fiber according to claim 1, wherein:
wherein the cross section of the cladding ring is a circular ring.
4. A photonic crystal fiber according to claim 1, wherein:
wherein the semi-circular openings of the air holes in the cladding ring are all facing the core layer.
5. A photonic crystal fiber according to claim 1, wherein:
wherein the refractive index of the core layer is greater than the refractive index of the cladding layer.
6. A photonic crystal fiber according to claim 1, wherein:
the cladding layer is made of a silica crystal material, and the core layer is made of a silica crystal material or a Schottky glass material.
CN201810537357.1A 2018-05-30 2018-05-30 Photonic crystal fiber Expired - Fee Related CN108732678B (en)

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Publication number Priority date Publication date Assignee Title
CN109596573B (en) * 2018-12-18 2021-02-26 华北水利水电大学 Novel D-structure photonic crystal fiber sensor based on surface plasmon resonance
CN110146953B (en) * 2019-05-17 2020-11-17 西安理工大学 Photonic crystal fiber generating multiple orbital angular momentum modes and design method
CN112649915B (en) * 2020-12-25 2022-08-02 东北石油大学 Photonic crystal fiber supporting 114 OAM mode transmission

Citations (3)

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Publication number Priority date Publication date Assignee Title
CN101779149A (en) * 2007-07-02 2010-07-14 泰科电子瑞侃有限公司 The hole arranged photonic crystal fiber that is used for low-loss, tight fibre-optical bending application
CN106842414A (en) * 2017-03-08 2017-06-13 南京邮电大学 A kind of new photonic crystal fiber for transmitting multiple OAM patterns
CN107238890A (en) * 2017-07-05 2017-10-10 南京邮电大学 A kind of photonic crystal fiber for transmitting 22 photon angular momentum moulds

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20030190129A1 (en) * 2000-08-25 2003-10-09 Ian Bassett Optical waveguide fibre
US20060133753A1 (en) * 2004-12-22 2006-06-22 Nelson Brian K Hole assisted fiber device and fiber preform

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101779149A (en) * 2007-07-02 2010-07-14 泰科电子瑞侃有限公司 The hole arranged photonic crystal fiber that is used for low-loss, tight fibre-optical bending application
CN106842414A (en) * 2017-03-08 2017-06-13 南京邮电大学 A kind of new photonic crystal fiber for transmitting multiple OAM patterns
CN107238890A (en) * 2017-07-05 2017-10-10 南京邮电大学 A kind of photonic crystal fiber for transmitting 22 photon angular momentum moulds

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