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CN1588141A - Photon crystal optical fiber - Google Patents

Photon crystal optical fiber Download PDF

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Publication number
CN1588141A
CN1588141A CNA2004100535417A CN200410053541A CN1588141A CN 1588141 A CN1588141 A CN 1588141A CN A2004100535417 A CNA2004100535417 A CN A2004100535417A CN 200410053541 A CN200410053541 A CN 200410053541A CN 1588141 A CN1588141 A CN 1588141A
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optical fiber
air holes
airport
cladding
background material
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CNA2004100535417A
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Chinese (zh)
Inventor
郭淑琴
黄肇明
方捻
王陆唐
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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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Priority to CNA2004100535417A priority Critical patent/CN1588141A/en
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Abstract

本发明涉及一种光子晶体光纤。它包含有纤芯和包层,其特征在于纤芯为光纤背景材料的中心实心区域;包层为包围纤芯的外围均布空气孔的区域,空气孔在光纤背景材料中呈周期性排列,即每相邻的三个空气孔构成一个正三角形;包层中靠近纤芯的若干圈空气孔在光纤背景材料中的正六边形排列围成的带状区域构成内包层,其余距纤芯较远的空气孔在光纤背景材料中的周期性排列围成的环形区域构成外包层;内包层中的空气孔小于外包层的空气孔。本发明提供的光纤可以在很宽波长范围内实现比较平坦的色散特性。本光纤适用于制作各种光器件和作为传输光纤使用。

The invention relates to a photonic crystal fiber. It contains a core and a cladding, which is characterized in that the core is the central solid area of the fiber background material; the cladding is an area surrounded by uniform air holes around the core, and the air holes are periodically arranged in the fiber background material. That is, every adjacent three air holes form an equilateral triangle; several rings of air holes in the cladding close to the core are arranged in a regular hexagonal shape in the fiber background material to form an inner cladding, and the rest are farther away from the core. The annular area surrounded by the periodic arrangement of distant air holes in the optical fiber background material constitutes the outer cladding; the air holes in the inner cladding are smaller than the air holes in the outer cladding. The optical fiber provided by the invention can realize relatively flat dispersion characteristics in a wide wavelength range. This optical fiber is suitable for making various optical devices and used as transmission optical fiber.

Description

光子晶体光纤Photonic crystal fiber

技术领域:Technical field:

本发明涉及一种光子晶体光纤,特别是一种在很宽波长范围内色散平坦的光子晶体光纤。The invention relates to a photon crystal fiber, in particular to a photon crystal fiber with flat dispersion in a wide wavelength range.

技术背景:technical background:

近十年来,光子晶体光纤因其具有许多优良的特性而受到全世界科学家们的热切关注。光子晶体光纤又称为多孔光纤或微结构光纤,其特点是包层的折射率受到波长量级周期性的调制,这种调制一般通过在硅玻璃中引入沿轴向伸长的空气孔实现,光纤芯由一个破坏了折射率调制周期性的缺陷构成。相对于包层的有效折射率,如果纤芯由低折射率材料(如空气)构成,这种光纤是通过带隙原理导光的,它要求包层中的空气孔严格排列。另一类光子晶体光纤的纤芯折射率较高,因此通过全内反射就可实现光的传导,这类光纤对包层中空气孔的周期性排列要求不是很精确,因此制作起来比较容易。In the past ten years, photonic crystal fiber has attracted the attention of scientists all over the world because of its many excellent properties. Photonic crystal fiber, also known as holey fiber or microstructure fiber, is characterized by the fact that the refractive index of the cladding is periodically modulated by the wavelength order. This modulation is generally achieved by introducing axially elongated air holes into silica glass. The fiber core consists of a defect that breaks the periodicity of the refractive index modulation. Relative to the effective refractive index of the cladding, if the core is made of a low refractive index material (such as air), this fiber guides light through the band gap principle, which requires strict arrangement of the air holes in the cladding. Another type of photonic crystal fiber has a higher core refractive index, so light transmission can be achieved through total internal reflection. This type of fiber does not require very precise periodic arrangement of air holes in the cladding, so it is easier to manufacture.

光子晶体光纤具有许多不同于传统光纤的优良特性,如:可在任意波长实现单模传输(无休止单模),通过改变空气孔和孔间距大小可灵活控制光纤的色散和模场面积,可以实现很弱或很强的非线性效应。此外,通过空气孔排布的非对称性可实现很高的双折射特性。但是改变空气孔和孔间距大小,只能在较狭小波长范围内使色散—波长曲线较平坦。Photonic crystal fibers have many excellent characteristics different from traditional fibers, such as: single-mode transmission (endless single-mode) can be achieved at any wavelength, and the dispersion and mode field area of the fiber can be flexibly controlled by changing the size of the air hole and the hole spacing. Implement very weak or strong nonlinear effects. In addition, high birefringence properties can be achieved through the asymmetry of the air hole arrangement. However, changing the size of the air hole and hole spacing can only make the dispersion-wavelength curve flatter in a narrow wavelength range.

光子晶体光纤的这些优良特性使其在光通信领域发挥发了极大作用,利用高色散光子晶体光纤可以进行色散补偿,利用强非线性或强双折射光子晶体光纤可制作各种光器件,尤其是制作技术的提高已经逐渐减小了光纤损耗,使其有可能作为传输光纤使用,因此为适应WDM系统中的要求非常有必要研制宽波长范围色散平坦的光子晶体光纤。These excellent characteristics of photonic crystal fiber make it play a great role in the field of optical communication. High dispersion photonic crystal fiber can be used for dispersion compensation, and strong nonlinear or strong birefringent photonic crystal fiber can be used to make various optical devices, especially It is the improvement of the production technology that has gradually reduced the loss of the fiber, making it possible to use it as a transmission fiber. Therefore, in order to meet the requirements of the WDM system, it is very necessary to develop a photonic crystal fiber with flat dispersion in a wide wavelength range.

发明内容:Invention content:

本发明的目的在于提供一种能够在很宽波长范围内实现色散平坦的光子晶体光纤。The object of the present invention is to provide a photonic crystal fiber capable of flattening dispersion in a wide wavelength range.

为达到上述目的,本发明采用下述技术方案:To achieve the above object, the present invention adopts the following technical solutions:

一种光子晶体光纤,包括纤芯和包层,其特征在于纤芯为光纤背景材料的中心实心区域;包层为包围纤芯的外围均布空气孔的区域,空气孔在光纤背景材料中呈周期性排列,即每相邻的三个空气孔构成一个正三角形;包层中靠近纤芯的若干圈空气孔在光纤背景材料中的正六边形排列围成的带状区域构成内包层,其余距纤芯较远的空气孔在光纤背景材料中的周期性排列围成的环形区域构成外包层;内包层中的空气孔小于外包层的空气孔。A photonic crystal fiber, comprising a core and a cladding, is characterized in that the core is the central solid region of the optical fiber background material; the cladding is the area surrounding the periphery of the core with air holes uniformly distributed, and the air holes appear in the fiber background material Periodically arranged, that is, every adjacent three air holes form an equilateral triangle; several rings of air holes in the cladding close to the fiber core are arranged in a regular hexagonal band in the fiber background material to form the inner cladding, and the rest The annular area surrounded by the periodic arrangement of the air holes farther from the fiber core in the fiber background material constitutes the outer cladding; the air holes in the inner cladding are smaller than the air holes in the outer cladding.

上述的内包层的空气孔排列的圈数为1-4圈。The air holes in the inner cladding layer are arranged in 1-4 turns.

上述的内包层空气孔直径(d1)与外包层空气孔直径(d2)之比(d1/d2)为0.1-0.9。The above-mentioned ratio (d 1 / d 2 ) of the inner cladding air hole diameter (d 1 ) to the outer cladding air hole diameter (d 2 ) is 0.1-0.9.

上述的内包层空气孔直径(d1)与外包层空气孔直径(d2)之比(d1/d2)为0.2-0.5。The above-mentioned ratio (d 1 / d 2 ) of the inner cladding air hole diameter (d 1 ) to the outer cladding air hole diameter (d 2 ) is 0.2-0.5.

上述的光纤背景材料为硅玻璃材料或聚合物材料。The above optical fiber background material is silica glass material or polymer material.

本发明与现在技术相比具有显而易见的实质性特点和优点:本发明中的内包层空气孔比外包层空气孔小,能实现很宽波长范围内的平坦色散。本发明提供的光纤适用于制作各种光器件和作为传输光纤使用。Compared with the current technology, the present invention has obvious substantive features and advantages: the inner cladding air holes in the present invention are smaller than the outer cladding air holes, and can realize flat dispersion in a wide wavelength range. The optical fiber provided by the invention is suitable for making various optical devices and used as transmission optical fiber.

附图说明:Description of drawings:

图1是本发明的一个实施例的横截面图中心部分即计算窗口区的结构示意图。FIG. 1 is a schematic structural diagram of the central part of the cross-sectional view of an embodiment of the present invention, that is, the calculation window area.

图2是图1示例的模场分布图。FIG. 2 is a mode field distribution diagram of the example in FIG. 1 .

图3是图1示例的色散曲线图。FIG. 3 is a graph of the dispersion curve of the example in FIG. 1 .

具体实施方式:Detailed ways:

本发明的一个优选实施例子是:参见图1、图2和图3,光纤纤芯有一个空气孔缺失(二氧化硅实心)形成导光区域,其外围由六个较小的空气孔1在背景硅玻璃3中围成内包层,其它较大的空气孔2在背景硅玻璃3中的周期性排列形成外包层。采用本技术领域公认的一种周期性排列,即如图1所示,每相邻的三个空气孔1或2构成一个正三角形,模场的分布如图2所示。外包层中空气孔直径d2为1.035微米,空气孔间距Λ为2.3微米,当内包层空气孔直径d1与外包层相同即1.035微米时,在1.0微米~2.0微米的波长范围内,光纤的色散在40~-30约70皮秒/纳米/公里的范围里变化,内包层空气孔直径d1逐渐减小时,会引起色散曲线的高端下降,低端上升,当内包层空气孔直径d1缩小到0.3微米时,在1000纳米的带宽内,色散曲线是几乎维持在10皮秒/纳米/公里的一条水平线,真正实现了宽波长范围内的色散平坦。但d1继续缩小到0.2微米时,色散曲线在1.0-2.0微米的波长范围内反而呈上升变化趋势。可见,减小内包层空气孔大小至一最佳值时(此例中最佳d1为0.3微米)可实现宽波段色散平坦。A preferred implementation example of the present invention is: referring to Fig. 1, Fig. 2 and Fig. 3, there is an air hole missing (silicon dioxide solid) in the fiber core to form a light guide area, and its periphery is surrounded by six smaller air holes 1 The background silica glass 3 forms an inner cladding, and the periodic arrangement of other larger air holes 2 in the background silica glass 3 forms an outer cladding. A periodic arrangement recognized in the technical field is adopted, that is, as shown in FIG. 1 , every three adjacent air holes 1 or 2 form an equilateral triangle, and the distribution of the mode field is shown in FIG. 2 . The air hole diameter d 2 in the outer cladding is 1.035 microns, and the air hole spacing Λ is 2.3 microns. When the air hole diameter d 1 of the inner cladding is the same as that of the outer cladding, that is, 1.035 microns, in the wavelength range of 1.0 microns to 2.0 microns, the optical fiber The dispersion changes in the range of 40 to -30, about 70 ps/nm/km. When the inner cladding air hole diameter d 1 gradually decreases, the high end of the dispersion curve will decrease and the low end will rise. When the inner cladding air hole diameter d 1 When narrowed down to 0.3 microns, within a bandwidth of 1000 nanometers, the dispersion curve is a horizontal line that is almost maintained at 10 ps/nm/km, truly achieving flat dispersion in a wide wavelength range. But when d 1 continues to shrink to 0.2 microns, the dispersion curve shows an upward trend in the wavelength range of 1.0-2.0 microns. It can be seen that reducing the size of the air holes in the inner cladding layer to an optimum value (in this example, the optimum d 1 is 0.3 μm) can achieve broadband dispersion flatness.

Claims (5)

1. a photonic crystal fiber comprises fibre core and covering, it is characterized in that fibre core is the center solid area of optical fiber background material; Covering is the zone of the peripheral uniform airport (1,2) of encirclement fibre core, and airport (1,2) is periodic arrangement in optical fiber background material (3), and promptly every adjacent three airports (1,2) constitute an equilateral triangle; Arrange the belt-like zone that surrounds near the regular hexagon of some circle airports (1) in optical fiber background material (3) of fibre core in the covering and constitute inner cladding, all the other constitute surrounding layer apart from the annular region that the periodic arrangement of fibre core airport far away (2) in optical fiber background material (3) surrounds; Airport in the inner cladding (1) is less than the airport (2) of surrounding layer.
2. photonic crystal fiber according to claim 1, the number of turns that it is characterized in that airport (1) arrangement of inner cladding is the 1-4 circle.
3. photonic crystal fiber according to claim 1 and 2 is characterized in that inner cladding airport (1) diameter (d 1) and surrounding layer airport (2) diameter (d 2) ratio (d 1/ d 2) be 0.1-0.9.
4. photonic crystal fiber according to claim 3 is characterized in that inner cladding airport (1) diameter (d 1) and surrounding layer airport (2) diameter (d 2) ratio (d 1/ d 2) be 0.2-0.5.
5. photonic crystal fiber according to claim 1 is characterized in that optical fiber background material (3) is silex glass material or polymeric material.
CNA2004100535417A 2004-08-06 2004-08-06 Photon crystal optical fiber Pending CN1588141A (en)

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Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN1294431C (en) * 2004-12-03 2007-01-10 浙江工业大学 Photon crystal fiber
CN1296735C (en) * 2004-12-29 2007-01-24 浙江工业大学 Dispersed flat photon crystal fiber
CN1299137C (en) * 2005-04-15 2007-02-07 清华大学 Large chromatic dispersion Bragg type photonic crystal fiber
CN1304860C (en) * 2005-04-15 2007-03-14 清华大学 A photonic crystal fiber with large mode field area and large dispersion
CN107632337A (en) * 2017-10-25 2018-01-26 中国地质大学(武汉) A kind of tellurate Group-velocity Matching photonic crystal fiber
CN108333670A (en) * 2018-05-04 2018-07-27 中国电子科技集团公司第四十六研究所 A kind of active microstructured optical fibers of aperiodicity coarse pitch single mode
CN109343171A (en) * 2018-11-29 2019-02-15 中国地质大学(武汉) A ZBLAN Fluoride Ultraflat Dispersion Compensation 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
CN114035264A (en) * 2021-11-18 2022-02-11 燕山大学 A kind of dispersion compensation microstructure fiber

Cited By (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN1294431C (en) * 2004-12-03 2007-01-10 浙江工业大学 Photon crystal fiber
CN1296735C (en) * 2004-12-29 2007-01-24 浙江工业大学 Dispersed flat photon crystal fiber
CN1299137C (en) * 2005-04-15 2007-02-07 清华大学 Large chromatic dispersion Bragg type photonic crystal fiber
CN1304860C (en) * 2005-04-15 2007-03-14 清华大学 A photonic crystal fiber with large mode field area and large dispersion
CN107632337A (en) * 2017-10-25 2018-01-26 中国地质大学(武汉) A kind of tellurate Group-velocity Matching photonic crystal fiber
CN108333670A (en) * 2018-05-04 2018-07-27 中国电子科技集团公司第四十六研究所 A kind of active microstructured optical fibers of aperiodicity coarse pitch single mode
CN109343171A (en) * 2018-11-29 2019-02-15 中国地质大学(武汉) A ZBLAN Fluoride Ultraflat Dispersion Compensation Photonic Crystal Fiber
CN109343171B (en) * 2018-11-29 2024-06-04 中国地质大学(武汉) ZBLAN fluoride ultra-flat dispersion compensation 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
CN114035264A (en) * 2021-11-18 2022-02-11 燕山大学 A kind of dispersion compensation microstructure fiber
CN114035264B (en) * 2021-11-18 2022-06-17 燕山大学 Dispersion compensation microstructure optical fiber

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