CN206020713U - Double-clad photon crystal optical fibre - Google Patents

Double-clad photon crystal optical fibre Download PDF

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CN206020713U
CN206020713U CN201621068731.0U CN201621068731U CN206020713U CN 206020713 U CN206020713 U CN 206020713U CN 201621068731 U CN201621068731 U CN 201621068731U CN 206020713 U CN206020713 U CN 206020713U
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air holes
cladding
fiber
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雷景丽
侯尚林
王娜
王道斌
李晓晓
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Lanzhou University of Technology
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Abstract

本实用新型公开双包层光子晶体光纤,包括纤芯、内包层和外包层,其中,光纤本体材料为折射率为n1=1.44的熔融石英,纤芯由一个缺失的空气孔构成,内包层由第一层、第二层的小空气孔构成,外包层由第三层、第四层空气孔构成,采用了上述方案后本实用新型PCF由双包层构成主要是因为双包层结构不仅使得耦合难度降低,而且具有独特的色散特性,便于调节,当d1=0.5μm时,可以使得所设计的光纤在λ=1.55μm处出现最低损耗,达7.39×10‑6dB/km,使得该PCF不仅可做色散补偿光纤,而且实现低损耗传输。

The utility model discloses a double-clad photonic crystal fiber, which includes a core, an inner cladding and an outer cladding, wherein the fiber body material is fused silica with a refractive index of n 1 =1.44, the fiber core is composed of a missing air hole, and the inner cladding It is composed of small air holes in the first layer and the second layer, and the outer cladding layer is composed of air holes in the third layer and the fourth layer. After adopting the above scheme, the utility model PCF is composed of double cladding mainly because the double cladding structure not only It reduces the difficulty of coupling, and has unique dispersion characteristics, which is easy to adjust. When d 1 =0.5μm, the designed fiber can have the lowest loss at λ=1.55μm, reaching 7.39× 10-6 dB/km, making The PCF can not only be used as dispersion compensating optical fiber, but also realize low-loss transmission.

Description

双包层光子晶体光纤Double-clad photonic crystal fiber

技术领域technical field

本实用新型涉及一种光子晶体光纤,特别指双包层光子晶体光纤。The utility model relates to a photonic crystal fiber, in particular to a double-clad photonic crystal fiber.

背景技术Background technique

光子晶体光纤(photonic crystal fiber,PCF)又称微结构或多孔光纤,由纤芯及其周围周期性排列着微小的空气孔而构成。通过改变空气孔的尺寸和填充率,可以灵活调节包层和纤芯的相对折射率,从而达到对光的约束效果,实现光的传导。根据导光机理的不同,光子晶体光纤又可分为全内反射型光子晶体光纤(Total Internal Reflection PCF,简称TIR-PCF)和光子带隙型光子晶体光纤(Photonic Band Gap PCF,简称PBG-PCF)。光子晶体光纤之所以被广泛应用于多领域中主要在于其独特的特性:无截止单模,可控的模式面积,较宽波长范围内可控的色散特性,和作为传输介质的高非线性特性等。虽然PCF基于一些独特优势被广泛应用于各领域,但其高损耗却制约着一些应用的进一步发展。Photonic crystal fiber (PCF), also known as microstructure or holey fiber, is composed of tiny air holes periodically arranged around the core and its surroundings. By changing the size and filling rate of the air holes, the relative refractive index of the cladding and the fiber core can be flexibly adjusted, so as to achieve the confinement effect on light and realize the transmission of light. According to the light guiding mechanism, photonic crystal fiber can be divided into total internal reflection photonic crystal fiber (Total Internal Reflection PCF, TIR-PCF for short) and photonic band gap photonic crystal fiber (Photonic Band Gap PCF, PBG-PCF for short). ). The reason why photonic crystal fibers are widely used in many fields is mainly due to their unique characteristics: no cut-off single mode, controllable mode area, controllable dispersion characteristics in a wide wavelength range, and high nonlinear characteristics as a transmission medium Wait. Although PCF is widely used in various fields based on some unique advantages, its high loss restricts the further development of some applications.

实用新型内容Utility model content

本实用新型的目的在于提供一种在λ=1.30~1.80μm波段时损耗较低的可做色散补偿光纤。The purpose of the utility model is to provide a dispersion compensation optical fiber with low loss in the band of λ=1.30-1.80 μm.

为达成上述目的,本实用新型双包层光子晶体光纤,包括纤芯、内包层和外包层,其中,光纤本体材料为折射率为n1=1.44的熔融石英,纤芯由一个缺失的空气孔构成,内包层由第一层、第二层的小空气孔构成,外包层由第三层、第四层空气孔构成,而外包层与内包层角度相差30°,内包层空气孔的直径d1为0.5~0.7μm,外包层空气孔的直径d2为1.4~1.6μm,第一、二层空气孔的节距Λ1为1.3~1.5μm,第二、三层空气孔的节距Λ2为1.7~1.8μm,第三、四层空气孔的节距Λ3为1.9~2.1μm。In order to achieve the above object, the utility model double-clad photonic crystal fiber includes a core, an inner cladding and an outer cladding, wherein the fiber body material is fused silica with a refractive index n 1 =1.44, and the core is formed by a missing air hole The inner cladding is composed of small air holes in the first and second layers, the outer cladding is composed of air holes in the third and fourth layers, and the angle difference between the outer cladding and the inner cladding is 30°, and the diameter of the air holes in the inner cladding is d 1 is 0.5-0.7 μm, the diameter d 2 of the outer cladding air holes is 1.4-1.6 μm, the pitch Λ of the first and second layers of air holes is 1.3-1.5 μm, the pitch of the second and third layers of air holes Λ 2 is 1.7-1.8 μm, and the pitch Λ 3 of the third and fourth layers of air holes is 1.9-2.1 μm.

所述的内包层空气孔的直径d1为0.5,外包层空气孔的直径d2为1.5μm,第一、二层空气孔的节距Λ1为1.5μm,第二、三层空气孔的节距Λ2为1.75μm,第三、四层空气孔的节距Λ3为2μm。The diameter d1 of the air hole in the inner cladding layer is 0.5, the diameter d2 of the air hole in the outer cladding layer is 1.5 μm, the pitch Λ1 of the first and second layers of air holes is 1.5 μm, and the diameter of the second and third layers of air holes is 1.5 μm. The pitch Λ 2 is 1.75 μm, and the pitch Λ 3 of the air holes in the third and fourth layers is 2 μm.

所述包层空气孔呈六边形设置。The cladding air holes are arranged in a hexagonal shape.

采用了上述方案后本实用新型PCF由双包层构成主要是因为双包层结构不仅使得耦合难度降低,而且具有独特的色散特性,便于调节,当d1=0.5μm时,可以使得所设计的光纤在λ=1.55μm处出现最低损耗,达7.39×10-6dB/km,使得该PCF不仅可做色散补偿光纤,而且实现低损耗传输。After adopting the above scheme, the utility model PCF is composed of double cladding mainly because the double cladding structure not only reduces the difficulty of coupling, but also has unique dispersion characteristics, which is easy to adjust. When d 1 =0.5μm, the designed The optical fiber has the lowest loss at λ=1.55μm, reaching 7.39×10 -6 dB/km, so that the PCF can not only be used as dispersion compensation optical fiber, but also realize low-loss transmission.

附图说明Description of drawings

图1为本实用新型结构截面示意图。Fig. 1 is a schematic cross-sectional view of the structure of the utility model.

具体实施方式detailed description

为详细说明本实用新型的技术内容、构造特征、所实现目的及效果,以下结合实施方式并配合附图详予说明。In order to describe the technical content, structural features, achieved goals and effects of the present utility model in detail, the following will be described in detail in conjunction with the embodiments and accompanying drawings.

请参阅图1,本实用新型双包层光子晶体光纤,包括纤芯、内包层和外包层,其中,光纤本体材料为折射率为n1=1.44的熔融石英,纤芯由一个缺失的空气孔构成,包层为四层呈六边形的空气孔,内包层由第一层、第二层的小空气孔构成,外包层由第三层、第四层空气孔构成,而外包层与内包层角度相差30°,内包层空气孔的直径d1为0.5~0.7μm,外包层空气孔的直径d2为1.4~1.6μm,第一、二层空气孔的节距Λ1为1.3~1.5μm,第二、三层空气孔的节距Λ2为1.7~1.8μm,第三、四层空气孔的节距Λ3为1.9~2.1μm。Please refer to Fig. 1, the double-clad photonic crystal fiber of the present invention comprises fiber core, inner cladding and outer cladding, and wherein, the material of optical fiber body is the fused silica of refractive index n 1 =1.44, and fiber core is made of a missing air hole The cladding is composed of four layers of hexagonal air holes, the inner cladding is composed of the first and second layers of small air holes, the outer cladding is composed of the third and fourth layers of air holes, and the outer cladding and the inner cladding The layer angles differ by 30°, the diameter d 1 of the air holes in the inner cladding is 0.5-0.7 μm, the diameter d 2 of the air holes in the outer cladding is 1.4-1.6 μm, and the pitch Λ 1 of the air holes in the first and second layers is 1.3-1.5 μm, the pitch Λ 2 of the second and third layers of air holes is 1.7-1.8 μm, and the pitch Λ 3 of the third and fourth layers of air holes is 1.9-2.1 μm.

采用全矢量有限元法(Finite Element Method,FEM),对光子晶体光纤的各个参数进行设置,计算出了光子晶体光纤基模的有效折射率neff,以此分析其在1.30~1.80μm宽带范围内的色散和损耗特性。Using the full vector finite element method (Finite Element Method, FEM), set the parameters of the photonic crystal fiber, calculate the effective refractive index n eff of the fundamental mode of the photonic crystal fiber, and analyze it in the broadband range of 1.30~1.80μm Dispersion and loss characteristics within.

光子晶体光纤的总色散为The total dispersion of photonic crystal fiber is

其中λ为传播波长,c为真空中的光速,neff(λ)为基模有效折射率,Dm(λ)为材料色散。Where λ is the propagation wavelength, c is the speed of light in vacuum, n eff (λ) is the effective refractive index of the fundamental mode, and D m (λ) is the material dispersion.

光纤的一个重要参量是光信号在光纤内传输时功率的损耗。若P0是入射光纤的功率,传输功率An important parameter of optical fiber is the power loss when the optical signal is transmitted in the optical fiber. If P 0 is the power of the incident fiber, the transmission power

pT=p0exp(-αL)p T =p 0 exp(-αL)

式中,α是衰减系数,通常称为光纤损耗,L是光纤的长度。In the formula, α is the attenuation coefficient, usually called fiber loss, and L is the length of the fiber.

光子晶体光纤损耗沿用了传统石英光纤损耗的定义,即光信号沿光纤传输时光功率的衰减。不同波长的衰减是不同的,连续对不同波长的损耗测量,叫做损耗谱测量。在实际中损耗通常可以使用衰减系数表达:The loss of photonic crystal fiber follows the definition of traditional silica fiber loss, that is, the attenuation of optical power when the optical signal is transmitted along the optical fiber. The attenuation of different wavelengths is different, and the continuous loss measurement of different wavelengths is called loss spectrum measurement. In practice the loss can usually be expressed using the attenuation coefficient:

所设计的新型双包层光子晶体光纤(double-cladding photonic crystalfiber,DC-PCF),由于模式光场主要分布在纤芯附近,因而离纤芯最近的一层空气孔对光纤的传输特性起主要作用。下面主要分析光纤包层中内包层空气孔直径d1、外包层空气孔直径d2和空气孔节距(Λ1、Λ2、Λ3)分别对于色散和损耗的影响。The new type of double-cladding photonic crystal fiber (DC-PCF) designed, because the mode light field is mainly distributed near the core, the layer of air holes closest to the core plays an important role in the transmission characteristics of the fiber. effect. The influence of inner cladding air hole diameter d 1 , outer cladding air hole diameter d 2 and air hole pitch (Λ 1 , Λ 2 , Λ 3 ) on dispersion and loss is mainly analyzed below.

本文基于六边形的空气孔排布,提出了一种新型双包层PCF结构。由于这种结构的PCF色散特性主要是由内芯和周围的空气孔结构决定的,因此,内包层结构与常规PCF相同时,可以实现相似的色散特性。而外包层的结构会影响限制损耗,所以通过优化外包层的结构来降低损耗。同时,由全内反射定理可知,包层的周期性结构对于高折射率芯导光几乎没有影响,且具有规则结构的PCF难以在宽波段获得平坦色散,故本文将最内包层空气孔的直径缩小以调节光纤的色散特性。In this paper, a novel double-clad PCF structure is proposed based on the hexagonal air hole arrangement. Since the PCF dispersion characteristics of this structure are mainly determined by the inner core and the surrounding air hole structure, similar dispersion characteristics can be achieved when the inner cladding structure is the same as that of conventional PCF. The structure of the outer cladding will affect the limit loss, so the loss is reduced by optimizing the structure of the outer cladding. At the same time, it can be seen from the total internal reflection theorem that the periodic structure of the cladding has little effect on the light guiding of the high refractive index core, and it is difficult for a PCF with a regular structure to obtain flat dispersion in a wide band, so this paper uses the diameter of the air hole in the innermost cladding Zoom out to tune the dispersion properties of the fiber.

通过合理设置PCF内、外包层空气孔的直径和空气孔节距,内包层空气孔的直径d1为0.5μm,外包层空气孔的直径d2为1.5μm,第一、二层空气孔的节距Λ1为1.5μm,第二、三层空气孔的节距Λ2为1.75μm,第三、四层空气孔的节距Λ3为2μm时,使得此PCF不仅可以实现宽带色散补偿而且具有低损耗的特性。数值结果显示,该PCF实现了色散在1.30~1.80μm的波段内呈宽带色散补偿效果,并使所设计的光纤在λ=1.55μm时,限制损耗达7.39×10-6dB/km。由此,本设计为基于宽带色散补偿光子晶体光纤的器件的选材和应用提供了参考,而此设计的低损特性可以增大光子晶体光纤的传输效率,为其实现实用化提供了一定的理论依据。By reasonably setting the diameter and air hole pitch of the air holes in the inner and outer cladding layers of the PCF, the diameter d 1 of the air holes in the inner cladding layer is 0.5 μm, the diameter d 2 of the air holes in the outer cladding layer is 1.5 μm, and the air holes in the first and second layers When the pitch Λ 1 is 1.5 μm, the pitch Λ 2 of the second and third layers of air holes is 1.75 μm, and the pitch Λ 3 of the third and fourth layers of air holes is 2 μm, this PCF can not only realize broadband dispersion compensation but also It has the characteristic of low loss. Numerical results show that the PCF achieves a broadband dispersion compensation effect in the 1.30-1.80μm band, and makes the designed optical fiber limit loss up to 7.39×10 -6 dB/km when λ=1.55μm. Therefore, this design provides a reference for the material selection and application of devices based on broadband dispersion compensation photonic crystal fiber, and the low loss characteristics of this design can increase the transmission efficiency of photonic crystal fiber, and provide a certain theory for its practical application in accordance with.

以上所述仅为本实用新型的实施例,并非因此限制本实用新型的专利范围,凡是利用本实用新型说明书及附图内容所作的等效形状或结构变换,或直接或间接运用在其他相关的技术领域,均同理包括在本实用新型的专利保护范围内。The above is only an embodiment of the present utility model, and does not limit the patent scope of the present utility model. Any equivalent shape or structural transformation made by using the description of the utility model and the contents of the accompanying drawings, or directly or indirectly used in other related Technical fields are all included in the scope of patent protection of the utility model in the same way.

Claims (3)

1.双包层光子晶体光纤,包括纤芯、内包层和外包层,其特征在于:光纤本体材料为折射率为n1=1.44的熔融石英,纤芯由一个缺失的空气孔构成,包层为四层呈六边形的空气孔,内包层由第一层、第二层的小空气孔构成,外包层由第三层、第四层空气孔构成,而外包层与内包层角度相差30°,内包层空气孔的直径d1为0.5~0.7μm,外包层空气孔的直径d2为1.4~1.6μm,第一、二层空气孔的节距Λ1为1.3~1.5μm,第二、三层空气孔的节距Λ2为1.7~1.8μm,第三、四层空气孔的节距Λ3为1.9~2.1μm。1. Double-clad photonic crystal fiber, comprising a core, an inner cladding and an outer cladding, characterized in that: the material of the fiber body is fused silica with a refractive index n 1 =1.44, the core is made of a missing air hole, and the cladding It is four layers of hexagonal air holes, the inner cladding is composed of the first and second layers of small air holes, the outer cladding is composed of the third and fourth layers of air holes, and the angle difference between the outer cladding and the inner cladding is 30° °, the diameter d 1 of the air holes in the inner cladding is 0.5-0.7 μm, the diameter d 2 of the air holes in the outer cladding is 1.4-1.6 μm, the pitch Λ 1 of the air holes in the first and second layers is 1.3-1.5 μm, the second 1. The pitch Λ2 of the third layer of air holes is 1.7-1.8 μm, and the pitch Λ3 of the third and fourth layers of air holes is 1.9-2.1 μm. 2.如权利要求1所述的双包层光子晶体光纤,其特征在于:所述的内包层空气孔的直径d1为0.5,外包层空气孔的直径d2为1.5μm,第一、二层空气孔的节距Λ1为1.5μm,第二、三层空气孔的节距Λ2为1.75μm,第三、四层空气孔的节距Λ3为2μm。2. double-clad photonic crystal fiber as claimed in claim 1, is characterized in that: the diameter d 1 of described inner cladding air hole is 0.5, and the diameter d 2 of outer cladding air hole is 1.5 μm, first, second The pitch Λ 1 of the air holes in the first layer is 1.5 μm, the pitch Λ 2 of the second and third layers of air holes is 1.75 μm, and the pitch Λ 3 of the third and fourth layers of air holes is 2 μm. 3.如权利要求1所述的双包层光子晶体光纤,其特征在于:所述包层空气孔呈六边形设置。3. The double-clad photonic crystal fiber according to claim 1, characterized in that: the air holes in the cladding are arranged in a hexagonal shape.
CN201621068731.0U 2016-09-21 2016-09-21 Double-clad photon crystal optical fibre Expired - Fee Related CN206020713U (en)

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Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN107526228A (en) * 2017-09-25 2017-12-29 兰州理工大学 A kind of method that photonic crystal fiber based on doping realizes fast optical transport
CN107783348A (en) * 2017-09-25 2018-03-09 兰州理工大学 A kind of method that fast optical transport is realized using special construction photonic crystal fiber
CN109581580A (en) * 2018-12-12 2019-04-05 桂林电子科技大学 A kind of fiber bragg grating device based on hollow-core photonic crystal fiber
CN112363269A (en) * 2020-12-11 2021-02-12 东北石油大学 High-birefringence low-limiting-loss photonic quasicrystal optical fiber

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN107526228A (en) * 2017-09-25 2017-12-29 兰州理工大学 A kind of method that photonic crystal fiber based on doping realizes fast optical transport
CN107783348A (en) * 2017-09-25 2018-03-09 兰州理工大学 A kind of method that fast optical transport is realized using special construction photonic crystal fiber
CN109581580A (en) * 2018-12-12 2019-04-05 桂林电子科技大学 A kind of fiber bragg grating device based on hollow-core photonic crystal fiber
CN112363269A (en) * 2020-12-11 2021-02-12 东北石油大学 High-birefringence low-limiting-loss photonic quasicrystal optical fiber

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