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具有三个及四个零色散波长光子晶体光纤的仿真研究
引用本文:赵兴涛,郑义,刘晓旭,刘兆伦,李曙光,侯蓝田.具有三个及四个零色散波长光子晶体光纤的仿真研究[J].物理学报,2012,61(19):194210-194210.
作者姓名:赵兴涛  郑义  刘晓旭  刘兆伦  李曙光  侯蓝田
作者单位:1. 北京交通大学理学院激光研究所,北京100044 燕山大学,河北省测试计量技术及仪器重点实验室,亚稳材料科学与技术国家重点实验室,秦皇岛066004
2. 北京交通大学理学院激光研究所,北京,100044
3. 河北科技师范学院理化学院,秦皇岛,066004
4. 燕山大学,河北省测试计量技术及仪器重点实验室,亚稳材料科学与技术国家重点实验室,秦皇岛066004
基金项目:国家自然科学基金重点项目(批准号: 60637010)、国家重点基础研究发展计划(批准号: 2010CB327604)、国家自然科学基金(批准号: 60978028)、河北省自然科学基金(批准号: F2010001313, F2010001291)和秦皇岛市科学技术研究与发展计划(批准号: 201001A076)资助的课题.
摘    要:利用多极法对光子晶体光纤的色散特性进行了模拟, 通过设计合适的结构参数, 得到了具有3个零色散波长的单模光纤.对中心纤芯有1个微小空气孔光子晶体光纤的色散特性进行了分析, 设计出了具有4个零色散波长的色散曲线.分析了零色散波长随光纤结构的变化规律, 这些零色散波长的位置和间距可以在很大波长范围内灵活调节. 具有多个零色散波长的光纤可以得到色散值极低的超平坦色散曲线. 多个零色散波长光纤能产生丰富的相位匹配曲线, 可以有效地控制光孤子及超短脉冲的四波混频及共振散射产生的光谱特性.

关 键 词:光子晶体光纤  多极法  零色散波长  色散平坦
收稿时间:2011-12-16

Simulation of photonic crystal fiber with three and four zero-dispersion wavelengths
Zhao Xing-Tao,Zheng Yi,Liu Xiao-Xu,Liu Zhao-Lun,Li Shu-Guang,Hou Lan-Tian.Simulation of photonic crystal fiber with three and four zero-dispersion wavelengths[J].Acta Physica Sinica,2012,61(19):194210-194210.
Authors:Zhao Xing-Tao  Zheng Yi  Liu Xiao-Xu  Liu Zhao-Lun  Li Shu-Guang  Hou Lan-Tian
Institution:1. Laser Institute of Science College, Beijing Jiaotong University, Beijing 100044, China ;2. Measurement Technology and Instrumentation Key Lab of Hebei Province, State Key Lab of Metastable Materials Science and Technology, Yanshan University, Qinhuangdao 066004, China;3. College of Physics and Chemistry, Hebei Normal University of Science and Technology, Qinhuangdao 066004, China
Abstract:The dispersion characteristics of photonic crystal fibers are computed using the multipole method. Single-mode fiber with three zero-dispersion wavelengths is obtained by properly designing fiber structure parameters. The dispersion characteristics of photonic crystal fiber with a small air hole in the core are analyzed. Fibers with four zero-dispersion wavelengths are designed. The variation rules of zero-dispersion wavelength with fiber structure parameter are found. The locations and spacings of the zero-dispersion wavelengths can be adjusted flexibly in a large wavelength range. Closing to zero and flattened dispersion can be obtained in the fibers with multiple zero-dispersion wavelengths. The multiple zero-dispersion wavelengths can create a rich phase-matching topology, and enable better controlling the spectral locations of the four-wave-mixing and resonant-radiation bands emitted by solitons and short pulses.
Keywords:photonic crystal fiber  multipole method  zero dispersion wavelength  flattened dispersion
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