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作 者:代问问 陈凯[1] 褚奕祺 罗巧霞 王贤 高伟清[1] DAI Wenwen;CHEN Kai;CHU Yiqi;LUO Qiaoxia;WANG Xian;GAO Weiqing(School of Physics,Hefei University of Technology,Hefei 230601,China)
出 处:《合肥工业大学学报(自然科学版)》2024年第9期1262-1267,共6页Journal of Hefei University of Technology:Natural Science
基 金:国家自然科学基金资助项目(61875052;61905059;62105087;62105088);安徽省重点研发计划资助项目(202104a07020010);安徽省自然科学基金资助项目(1908085QF273;2108085QF282);中央高校基本科研业务费专项资金资助项目(JZ2020HGTB0065;JZ2021HGTA0145;JZ2021HGQA0255;JZ2021HGTA0148)
摘 要:针对2.0~25.0μm波段传输的限制损耗问题,文章采用数值模拟方法研究影响碲基硫系光子晶体光纤(photonic crystal fiber,PCF)限制损耗的主要因素。光纤纤芯和包层材料采用Ge 20 As 20 Se 15 Te 45玻璃,通过改变纤芯直径、空气孔直径和空气孔层数等参数进行2.0~25.0μm波段限制损耗的计算,结果表明,影响限制损耗的最大因素是纤芯直径,限制损耗随着纤芯直径和空气孔直径的增大而显著降低,随着空气孔层数的增加而降低;优化设计出一种低限制损耗的PCF,结果表明,当纤芯直径和节距为8.0μm、空气孔直径为7.2μm、包层空气孔层数为4时,该PCF在2.0~25.0μm波长范围的限制损耗低于1.4×10^(-6) dB/m,满足低损耗传输要求。文章研究结果对2.0~25.0μm波段光信号的传输具有一定的意义。In consideration of the confinement loss of transmission in the 2.0-25.0μm waveband,the main factors affecting the confinement loss of tellurium-based chalcogenide glass photonic crystal fiber(PCF)are investigated by numerical simulation.The core and cladding materials of PCF are Ge 20 As 20 Se 15 Te 45 glass.The confinement loss of PCF in 2.0-25.0μm waveband is calculated by changing the core diameter,air hole diameter and number of air hole layer.The results show that the greatest factor affecting the confinement loss is the core diameter,and the confinement loss decreases significantly with the increase of the core diameter,air hole diameter and number of air hole layer.A PCF with low confinement loss is designed by optimizing the parameters.It is shown that when the core diameter and pitch are 8.0μm,the diameter of air hole is 7.2μm,and the number of air hole layer in the cladding layer is 4,the calculated confinement loss is lower than 1.4×10^(-6) dB/m in the spectral range of 2.0-25.0μm,which meets the requirements of low loss transmission.The results are of significance for the transmission of optical signals in the spectral range of 2.0-25.0μm.
关 键 词:限制损耗 碲基硫系玻璃 光子晶体光纤(PCF) 中远红外波段
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