CN106908895B - An all-solid-state broadband dispersion-compensated index-guided microstructured fiber - Google Patents
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- 239000000835 fiber Substances 0.000 title claims description 35
- 239000006185 dispersion Substances 0.000 claims abstract description 55
- 239000013307 optical fiber Substances 0.000 claims abstract description 37
- 238000005253 cladding Methods 0.000 claims abstract description 34
- 239000000463 material Substances 0.000 claims abstract description 19
- 239000010453 quartz Substances 0.000 claims abstract description 18
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N silicon dioxide Inorganic materials O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 claims abstract description 18
- 235000012239 silicon dioxide Nutrition 0.000 abstract description 16
- 230000005540 biological transmission Effects 0.000 abstract description 10
- 238000004891 communication Methods 0.000 abstract description 9
- 239000007787 solid Substances 0.000 description 8
- 238000000034 method Methods 0.000 description 5
- 238000010586 diagram Methods 0.000 description 4
- 230000008878 coupling Effects 0.000 description 3
- 238000010168 coupling process Methods 0.000 description 3
- 238000005859 coupling reaction Methods 0.000 description 3
- 230000008569 process Effects 0.000 description 3
- 230000008859 change Effects 0.000 description 2
- 238000005516 engineering process Methods 0.000 description 1
- 229910052732 germanium Inorganic materials 0.000 description 1
- GNPVGFCGXDBREM-UHFFFAOYSA-N germanium atom Chemical compound [Ge] GNPVGFCGXDBREM-UHFFFAOYSA-N 0.000 description 1
- 230000007246 mechanism Effects 0.000 description 1
- 230000005405 multipole Effects 0.000 description 1
- 239000004038 photonic crystal Substances 0.000 description 1
- 239000007962 solid dispersion Substances 0.000 description 1
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- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/02—Optical fibres with cladding with or without a coating
- G02B6/02295—Microstructured optical fibre
- G02B6/02314—Plurality of longitudinal structures extending along optical fibre axis, e.g. holes
- G02B6/02319—Plurality of longitudinal structures extending along optical fibre axis, e.g. holes characterised by core or core-cladding interface features
- G02B6/02323—Core having lower refractive index than cladding, e.g. photonic band gap guiding
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- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/02—Optical fibres with cladding with or without a coating
- G02B6/036—Optical fibres with cladding with or without a coating core or cladding comprising multiple layers
- G02B6/03616—Optical fibres characterised both by the number of different refractive index layers around the central core segment, i.e. around the innermost high index core layer, and their relative refractive index difference
- G02B6/03622—Optical fibres characterised both by the number of different refractive index layers around the central core segment, i.e. around the innermost high index core layer, and their relative refractive index difference having 2 layers only
- G02B6/03627—Optical fibres characterised both by the number of different refractive index layers around the central core segment, i.e. around the innermost high index core layer, and their relative refractive index difference having 2 layers only arranged - +
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Abstract
一种全固态宽带色散补偿折射率引导型微结构光纤,它包括内、外层纤芯圆柱、包层圆柱和基底材料,其中基底材料为纯石英,内层纤芯圆柱为掺锗的纯石英棒,外层纤芯圆柱为一层按正六边形紧密排列的掺氟或硼的纯石英棒;包层圆柱为按正六边形紧密排列的掺氟或硼的纯石英棒;内层纤芯圆柱的折射率大于基底材料折射率,基底材料折射率大于外层纤芯圆柱折射率,外层纤芯圆柱折射率大于包层圆柱折射率;包层圆柱的直径相同,且大于外层纤芯圆柱直径,内层纤芯圆柱直径大于外层芯圆柱直径;所有圆柱的柱间距相等。本发明易制备、易与传统光纤耦合,能对高速密集波分复用光纤通信传输过程中的累积色散进行宽带色散补偿、为光纤通信系统提供有效传输介质。
An all-solid-state broadband dispersion-compensated refractive index-guided microstructure optical fiber comprises inner and outer core cylinders, cladding cylinders and a base material, wherein the base material is pure silica, and the inner core cylinder is germanium-doped pure silica Rod, the outer core cylinder is a layer of fluorine- or boron-doped pure quartz rods closely arranged in a regular hexagon; the cladding cylinder is a fluorine- or boron-doped pure quartz rod closely arranged in a regular hexagon; the inner core The refractive index of the cylinder is greater than the refractive index of the base material, the refractive index of the base material is greater than the refractive index of the outer core cylinder, the refractive index of the outer core cylinder is greater than the refractive index of the cladding cylinder; the diameter of the cladding cylinder is the same and larger than that of the outer core Cylinder diameter, the inner core cylinder diameter is larger than the outer core cylinder diameter; the column spacing of all cylinders is equal. The invention is easy to prepare and easy to couple with the traditional optical fiber, can perform broadband dispersion compensation for the accumulated dispersion in the high-speed dense wavelength division multiplexing optical fiber communication transmission process, and provide an effective transmission medium for the optical fiber communication system.
Description
技术领域technical field
本发明属于光纤技术领域,特别涉及一种微结构光纤。The invention belongs to the technical field of optical fibers, and particularly relates to a microstructure optical fiber.
背景技术Background technique
在现代光纤通信系统中,尤其是高速密集波分复用光纤通信系统中,传输过程中的累积色散成为对该类系统的主要限制。因此,对高速密集波分复用光纤通信系统进行宽带色散补偿成为一个研究热点。In modern optical fiber communication systems, especially high-speed dense wavelength-division multiplexing optical fiber communication systems, the accumulated dispersion during transmission becomes the main limitation for such systems. Therefore, broadband dispersion compensation for high-speed dense wavelength division multiplexing optical fiber communication systems has become a research hotspot.
随着人们对微结构光纤(又叫光子晶体光纤)的理论研究和制备技术的不断了解,人们发现通过调整光纤微结构设计,可以极大地调节光纤的色散特性,例如光纤的色散平坦特性、色散补偿特性等。With the continuous understanding of the theoretical research and preparation technology of microstructured fibers (also known as photonic crystal fibers), it has been found that by adjusting the microstructure design of the fiber, the dispersion properties of the fiber can be greatly adjusted, such as the dispersion flatness of the fiber, dispersion compensation characteristics, etc.
目前有关色散补偿微结构光纤的研究,主要集中在空芯、全固带隙型和空气孔-石英结构折射率引导型微结构光纤方面。但是带隙型光纤限制了导光窗口,不适于做传输介质;空气孔-石英结构的微结构光纤存在不易与传统光纤耦合、拉制过程中由于温度过高,包层中的空气孔很容易出现塌陷或形变等缺点。At present, the research on dispersion-compensated microstructured fibers mainly focuses on hollow-core, all-solid bandgap and air-hole-quartz structure index-guided microstructured fibers. However, the bandgap optical fiber limits the light guide window and is not suitable as a transmission medium; the microstructure optical fiber with air hole-quartz structure is not easy to couple with the traditional optical fiber, and the air hole in the cladding is easy to be caused by the high temperature during the drawing process. Disadvantages such as collapse or deformation occur.
由于全固折射率引导型微结构光纤采用不同折射率的介质柱代替空气孔构成,在适合做传输介质的同时具有易与传统光纤耦合、易制备等优点,能有效解决上述空芯、全固带隙型和空气孔-石英结构折射率引导型微结构光纤所存在问题。目前已有部分研究人员对全固折射率引导型微结构光纤展开研究,但他们主要对其色散平坦特性、大模面积特性等进行研究。该类光纤能有效的在光纤通信中传输信号,但都不具备色散补偿特性,无法对光纤通信传输过程中的累积色散进行补偿。Since the all-solid index-guided microstructure fiber is composed of medium columns with different refractive indices instead of air holes, it is suitable for transmission media and has the advantages of easy coupling with traditional optical fibers and easy preparation, which can effectively solve the above-mentioned hollow, all-solid Problems with bandgap and air hole-quartz structure index-guided microstructured fibers. At present, some researchers have carried out research on the all-solid index-guided microstructured fiber, but they mainly study its dispersion flattening characteristics and large mode area characteristics. This type of optical fiber can effectively transmit signals in optical fiber communication, but does not have dispersion compensation characteristics, and cannot compensate for the accumulated dispersion in the transmission process of optical fiber communication.
目前未见研究人员对全固折射率引导型微结构光纤的色散补偿特性展开研究,仅发现两篇与全固色散补偿微结构光纤密切相关的报道。一是Gautam Prabhakar等设计一种局部全固色散补偿折射率引导型微结构光纤,该光纤虽然具有单点色散补偿特性或宽带色散补偿特性,但该光纤仍然含有两层圆形空气孔,存在不易与传统光纤耦合、拉制过程中由于温度过高,包层中的空气孔很容易出现塌陷或形变等缺点。二是贺冯良等设计一种全固色散补偿带隙型微结构光纤,该光纤虽然具有多零色散点特性和负色散补偿特性,但该光纤为带隙型光纤,限制了导光窗口,不适于做传输介质。At present, no researchers have studied the dispersion compensation characteristics of all-solid index-guided microstructured fibers, and only two reports have been found that are closely related to all-solid dispersion-compensated microstructured fibers. First, Gautam Prabhakar et al. designed a local all-solid dispersion-compensated refractive index-guided microstructure fiber. Although the fiber has single-point dispersion compensation characteristics or broadband dispersion compensation characteristics, the fiber still contains two layers of circular air holes. Coupling with traditional optical fibers, the air holes in the cladding are prone to collapse or deformation due to excessive temperature during the drawing process. Second, He Fengliang et al. designed an all-solid dispersion compensation bandgap microstructure fiber. Although the fiber has the characteristics of multiple zero dispersion points and negative dispersion compensation, the fiber is a bandgap fiber, which limits the light guide window and is not suitable for as a transmission medium.
发明内容SUMMARY OF THE INVENTION
本发明目的在于提供一种易制备、易与传统光纤耦合、能对高速密集波分复用光纤通信传输过程中的累积色散进行宽带色散补偿并且能为光纤通信系统提供有效传输介质的全固态宽带色散补偿折射率引导型微结构光纤。The purpose of the present invention is to provide an all-solid-state broadband that is easy to prepare, easy to couple with traditional optical fibers, can perform broadband dispersion compensation for the accumulated dispersion in the transmission process of high-speed dense wavelength division multiplexing optical fiber communication, and can provide an effective transmission medium for optical fiber communication systems. Dispersion-compensated index-guided microstructured fibers.
本发明包括内、外层纤芯圆柱、包层圆柱以及基底材料,其中基底材料为纯石英,内层纤芯圆柱为掺锗的纯石英棒,外层纤芯圆柱为一层按照正六边形紧密排列的掺氟或硼的纯石英棒;包层圆柱为按照正六边形紧密排列的掺氟或硼的纯石英棒;内层纤芯圆柱的折射率大于基底材料折射率,基底材料折射率大于外层纤芯圆柱折射率,外层纤芯圆柱折射率大于包层圆柱折射率;所有包层圆柱的直径相同,并且大于外层纤芯圆柱直径,内层纤芯圆柱直径大于外层芯圆柱直径;所有圆柱的柱间距相等。The invention includes inner and outer layer core cylinders, cladding cylinders and base material, wherein the base material is pure quartz, the inner core cylinder is pure quartz rod doped with germanium, and the outer core cylinder is a layer according to a regular hexagon. Closely arranged fluorine- or boron-doped pure silica rods; cladding cylinders are fluorine- or boron-doped pure silica rods closely arranged according to regular hexagons; the refractive index of the inner core cylinder is greater than that of the base material, and the refractive index of the base material is The refractive index of the outer core cylinder is greater than that of the outer core cylinder, and the refractive index of the outer core cylinder is greater than the refractive index of the cladding cylinder; the diameters of all cladding cylinders are the same and larger than the diameter of the outer core cylinder, and the inner core cylinder diameter is greater than that of the outer core Cylinder diameter; all cylinders are equally spaced.
所述基底材料折射率为1.45;The base material has a refractive index of 1.45;
所述内层纤芯圆柱的折射率为1.45~1.485;The refractive index of the inner core cylinder is 1.45-1.485;
所述外层纤芯圆柱的折射率为1.44~1.45;The refractive index of the outer core cylinder is 1.44-1.45;
所述包层圆柱的折射率为1.425~1.44;The refractive index of the cladding cylinder is 1.425-1.44;
所述内层纤芯圆柱直径为1.2~2.0μm;The diameter of the inner layer core cylinder is 1.2-2.0 μm;
所述外层纤芯圆柱直径为0.43~0.59μm;The diameter of the outer core cylinder is 0.43-0.59 μm;
所述包层圆柱直径为0.8~1.8μm;The diameter of the cladding cylinder is 0.8-1.8 μm;
所述所有圆柱的柱间距均为1.8~2.4μm。The column spacing of all the columns is 1.8-2.4 μm.
所述包层总层数为6层,在内层纤芯和外层纤芯之间有三层,外层纤芯之外有三层。The total number of the cladding layers is 6 layers, there are three layers between the inner layer core and the outer layer core, and there are three layers outside the outer layer core.
本发明与现有技术相比具有以下优点:Compared with the prior art, the present invention has the following advantages:
1、光纤是双层芯结构,利用内层芯和外层芯模式之间的耦合机理,获得较大负色散值。1. The optical fiber is a double-layer core structure, and a large negative dispersion value is obtained by using the coupling mechanism between the inner core and the outer core mode.
2、通过设计合适的内外层芯圆柱的折射率和直径、包层圆柱的折射率和直径以及柱间距,可以获得宽带色散补偿特性。2. By designing appropriate refractive index and diameter of inner and outer core cylinders, refractive index and diameter of cladding cylinders, and column spacing, broadband dispersion compensation characteristics can be obtained.
3、全固结构降低了成纤工艺复杂度,易于制备,易于与传统光纤耦合。3. The all-solid structure reduces the complexity of the fiber-forming process, is easy to prepare, and is easy to couple with traditional optical fibers.
4、折射率引导型微结构光纤不限制导光窗口,能作为有效的传输介质。4. The refractive index-guided microstructure fiber does not limit the light guide window and can be used as an effective transmission medium.
附图说明Description of drawings
图1是本发明的结构截面示意图。FIG. 1 is a schematic cross-sectional view of the structure of the present invention.
图2是本发明实施例1的折射率分布图。FIG. 2 is a refractive index distribution diagram of Example 1 of the present invention.
图3是本发明实施例1的基模有效折射率随波长的变换及不同波长下基模的模场分布图。3 is a graph showing the change of the effective refractive index of the fundamental mode with wavelength and the mode field distribution diagram of the fundamental mode at different wavelengths according to Embodiment 1 of the present invention.
图4是本发明实施例1的色散值与波长的关系图。FIG. 4 is a graph showing the relationship between dispersion value and wavelength in Example 1 of the present invention.
图5是本发明实施例1的卡帕值与波长的关系图。5 is a graph showing the relationship between the kappa value and the wavelength in Example 1 of the present invention.
图6是本发明实施例1的残余色散曲线图。FIG. 6 is a residual dispersion curve diagram of Example 1 of the present invention.
图中:1-内层纤芯圆柱、2-外层纤芯圆柱、3-包层圆柱、4-基底材料、5-圆柱之间的柱间距、6-内层纤芯圆柱的折射率、7-外层纤芯圆柱的折射率、8-包层圆柱折射率。In the figure: 1-inner core cylinder, 2-outer core cylinder, 3-cladding cylinder, 4-base material, 5-column spacing between cylinders, 6-refractive index of inner core cylinder, 7- The refractive index of the outer core cylinder, 8- The refractive index of the cladding cylinder.
具体实施方式Detailed ways
实施例1Example 1
在图1所示的全固态宽带色散补偿折射率引导型微结构光纤示意图中,基底材料4为纯石英,内层纤芯圆柱1为掺锗的纯石英棒,外层纤芯圆柱2为一层按照正六边形紧密排列的掺氟的纯石英棒;包层圆柱3为按照正六边形紧密排列的掺氟的纯石英棒;所有包层圆柱的直径相同,均为1.64μm,外层纤芯圆柱直径为0.51μm,内层纤芯圆柱直径为1.6μm,所有圆柱的柱间距相等,均为2.1μm;包层总层数为6层,在内层纤芯和外层纤芯之间有三层,外层芯之外有三层;如图2所示,基底材料折射率n0为1.45,内层纤芯圆柱的折射率n1为1.48,外层纤芯圆柱折射率n2为1.445,包层圆柱折射率n3为1.43。In the schematic diagram of the all-solid-state broadband dispersion-compensated refractive index-guided microstructure fiber shown in FIG. 1 , the base material 4 is pure silica, the inner core cylinder 1 is a germanium-doped pure silica rod, and the
内层纤芯和外层纤芯的圆柱折射率均大于包层圆柱的折射率,形成基于全内反射导光的微结构光纤,通过合理设计内、外层纤芯圆柱的折射率和直径、包层圆柱的折射率和直径以及柱间距,可以灵活的调节色散特性。采用多极法进行理论计算,得到本发明所述光纤基模有效折射率随波长的变换及不同波长下基模的模场分布。如图3所示。从图中可以看出,在某一波长处,折射率产生突变,该波长就称为相位匹配波长λp。当波长小于相位匹配波长时,基模在内层芯中传播,此时内层芯基模有效折射率大于外层芯高阶模有效折射率;当波长等于相位匹配波长时,内层芯基模和外层芯高阶模的有效折射率相等,从而二者发生耦合,即内层芯基模转换到外层芯中传播,外层芯高阶模转换到内层芯中传播。当波长大于相位匹配波长时,内层芯基模能量逐渐向外层芯耦合,此时外层芯基模有效折射率大于内芯层高阶模有效折射率。The cylindrical refractive index of the inner core and the outer core are both greater than the refractive index of the cladding cylinder, forming a microstructure fiber based on total internal reflection light guide. The refractive index and diameter of the cladding cylinder, as well as the column spacing, can flexibly adjust the dispersion characteristics. The multipole method is used for theoretical calculation to obtain the effective refractive index change of the fundamental mode of the optical fiber according to the present invention with wavelength and the mode field distribution of the fundamental mode at different wavelengths. As shown in Figure 3. It can be seen from the figure that at a certain wavelength, the refractive index changes abruptly, and this wavelength is called the phase matching wavelength λ p . When the wavelength is less than the phase matching wavelength, the fundamental mode propagates in the inner core, and the effective refractive index of the inner core fundamental mode is greater than the effective refractive index of the outer core high-order mode; when the wavelength is equal to the phase matching wavelength, the inner core fundamental mode and The effective refractive indices of the high-order modes of the outer core are equal, so that the two are coupled, that is, the fundamental mode of the inner core is converted into the outer core to propagate, and the higher-order modes of the outer core are converted to propagate in the inner core. When the wavelength is greater than the phase matching wavelength, the energy of the fundamental mode of the inner core is gradually coupled to the outer core, and the effective refractive index of the fundamental mode of the outer core is greater than the effective refractive index of the high-order mode of the inner core.
由于光纤的色散随波长发生变化,为了适应宽带色散补偿的需要,必须考虑对色散和色散斜率同时进行补偿,为了同时考虑色散和色散斜率的因素,人们定义了一个新的参数卡帕(K),其表达式为K=D/Dslope。它表示器件对光纤色散和色散斜率的同时补偿能力。如果要达到理想的宽带色散补偿,一般要求色散补偿光纤的卡帕值与被补偿光纤接近或相等。Since the dispersion of optical fiber varies with wavelength, in order to meet the needs of broadband dispersion compensation, it is necessary to consider the compensation of dispersion and dispersion slope at the same time. In order to consider the factors of dispersion and dispersion slope at the same time, a new parameter kappa (K) is defined. , whose expression is K=D/D slope . It represents the device's ability to simultaneously compensate for fiber dispersion and dispersion slope. In order to achieve ideal broadband dispersion compensation, it is generally required that the kappa value of the dispersion compensating fiber is close to or equal to that of the fiber being compensated.
图4和图5所示,从图中可以看出,在相位匹配波长处,色散值发生突变。且在相位匹配波长前,色散值具有负色散值以及负色散斜率,满足宽带色散补偿的需要。在1500nm~1600nm范围内,色散值在-220ps/nm·km~-163ps/nm·km内变化,本发明所述光纤的卡帕值和标准单模光纤的卡帕值非常接近,且在1538nm和1578nm处两卡帕值相等,具有良好的宽带色散补偿特性。As shown in Figure 4 and Figure 5, it can be seen from the figures that at the phase matching wavelength, the dispersion value changes abruptly. And before the phase matching wavelength, the dispersion value has a negative dispersion value and a negative dispersion slope, which meets the needs of broadband dispersion compensation. In the range of 1500nm~1600nm, the dispersion value varies within -220ps/nm·km~-163ps/nm·km, the Kappa value of the optical fiber of the present invention is very close to that of the standard single-mode fiber, and at 1538nm It is equal to the two kappa values at 1578nm, and has good broadband dispersion compensation characteristics.
如图6表示,从图中可以看出,在1500nm~1600nm范围内,本发明所述光纤补偿10.69倍的标准单模光纤之后,残余色散近零平坦,进一步表明本发明所述光纤具有良好的宽带色散补偿特性。As shown in Figure 6, it can be seen from the figure that in the range of 1500nm to 1600nm, after the optical fiber of the present invention compensates 10.69 times the standard single-mode fiber, the residual dispersion is nearly zero and flat, which further shows that the optical fiber of the present invention has good Broadband dispersion compensation characteristics.
实施例2Example 2
基底材料为纯石英,内层纤芯圆柱为掺锗的纯石英棒,外层纤芯圆柱为一层按照正六边形紧密排列的掺硼的纯石英棒;包层圆柱为按照正六边形紧密排列的掺硼的纯石英棒;所有包层圆柱的直径相同,均为1.0μm,外层纤芯圆柱直径为0.43μm,内层纤芯圆柱直径为2.0μm,所有圆柱的柱间距相等,均为1.8μm;包层总层数为6层,在内层纤芯和外层纤芯之间有三层,外层芯之外有三层;基底材料折射率n0为1.45,内层纤芯圆柱的折射率n1为1.46,外层纤芯圆柱折射率n2为1.44,包层圆柱折射率n3为1.425。The base material is pure quartz, the inner core cylinder is a germanium-doped pure quartz rod, the outer core cylinder is a layer of boron-doped pure quartz rods closely arranged in a regular hexagon; the cladding cylinder is a regular hexagonal close Arranged boron-doped pure quartz rods; all cladding cylinders have the same diameter, 1.0 μm, the outer core cylinder diameter is 0.43 μm, the inner core cylinder diameter is 2.0 μm, and the column spacing of all cylinders is equal, all is 1.8μm; the total number of cladding layers is 6, there are three layers between the inner core and the outer core, and there are three layers outside the outer core; the refractive index n 0 of the base material is 1.45, and the inner core is cylindrical The refractive index n1 is 1.46, the outer core cylindrical refractive index n2 is 1.44, and the cladding cylindrical refractive index n3 is 1.425.
以上所述的实施例仅仅是对本发明的优选实施方式进行描述,并非对本发明的范围进行限定,在不脱离本发明设计精神的前提下,本领域普通技术人员对本发明的技术方案做出的各种变形和改进,均应落入本发明权利要求书确定的保护范围内。The above-mentioned embodiments are only to describe the preferred embodiments of the present invention, and do not limit the scope of the present invention. On the premise of not departing from the design spirit of the present invention, those of ordinary skill in the art can Such deformations and improvements shall fall within the protection scope determined by the claims of the present invention.
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