传感技术学报
傳感技術學報
전감기술학보
Journal of Transduction Technology
2014年
6期
743-746
,共4页
赵洪霞%程培红%鲍吉龙%王金霞
趙洪霞%程培紅%鮑吉龍%王金霞
조홍하%정배홍%포길룡%왕금하
光纤光栅%包层半径%填充厚度%填充材料折射率%环境折射率
光纖光柵%包層半徑%填充厚度%填充材料摺射率%環境摺射率
광섬광책%포층반경%전충후도%전충재료절사솔%배경절사솔
optical-fiber grating%cladding-radius%filled-thickness%filled materials refractive index%environment refractive index
基于长周期光纤光栅( LPFG)包层有效折射率与包层半径、折射率和环境折射率的良好相关性,提出一种LPFG的新颖结构。利用传输矩阵法和三包层光纤的色散方程对其建模,mathcad15计算软件进行数值仿真和模拟。得到新型结构LPFG谐振峰发生分裂,即一个透射峰分裂为两个;两个分裂峰谐振波长间距随着腐蚀段包层半径的减小或填充材料厚度的增大而增加,模式越高增加越快;同时分裂峰间距在填充材料折射率小于1.4和大于1.48时基本不变,而在1.4和1.48之间分裂峰间距变化显著,在1.44附近达到极值。此种结构LPFG设计上的特殊性即可弥补半腐蚀LPFG容易断的不足,又可通过填充敏感材料且利用分裂峰间距定标而提高气体或液体浓度传感灵敏度。
基于長週期光纖光柵( LPFG)包層有效摺射率與包層半徑、摺射率和環境摺射率的良好相關性,提齣一種LPFG的新穎結構。利用傳輸矩陣法和三包層光纖的色散方程對其建模,mathcad15計算軟件進行數值倣真和模擬。得到新型結構LPFG諧振峰髮生分裂,即一箇透射峰分裂為兩箇;兩箇分裂峰諧振波長間距隨著腐蝕段包層半徑的減小或填充材料厚度的增大而增加,模式越高增加越快;同時分裂峰間距在填充材料摺射率小于1.4和大于1.48時基本不變,而在1.4和1.48之間分裂峰間距變化顯著,在1.44附近達到極值。此種結構LPFG設計上的特殊性即可瀰補半腐蝕LPFG容易斷的不足,又可通過填充敏感材料且利用分裂峰間距定標而提高氣體或液體濃度傳感靈敏度。
기우장주기광섬광책( LPFG)포층유효절사솔여포층반경、절사솔화배경절사솔적량호상관성,제출일충LPFG적신영결구。이용전수구진법화삼포층광섬적색산방정대기건모,mathcad15계산연건진행수치방진화모의。득도신형결구LPFG해진봉발생분렬,즉일개투사봉분렬위량개;량개분렬봉해진파장간거수착부식단포층반경적감소혹전충재료후도적증대이증가,모식월고증가월쾌;동시분렬봉간거재전충재료절사솔소우1.4화대우1.48시기본불변,이재1.4화1.48지간분렬봉간거변화현저,재1.44부근체도겁치。차충결구LPFG설계상적특수성즉가미보반부식LPFG용역단적불족,우가통과전충민감재료차이용분렬봉간거정표이제고기체혹액체농도전감령민도。
A novel LPFG structure was proposed based on the excellent relation between effective refractive index of cladding,radius and refractive index of cladding and environment refractive index. A theoretical model was built using transmission matrix method and dispersion equation of three-layered fiber,and then numerical simulation was carried out by Mathcad15 software. The simulation results show that the resonance peak is divided into two peaks, and the gap between them is increased when decreasing the cladding radius of the etched section or increasing the thickness of the filling materials. The gap increase is more rapid for the higher order mode. Moreover, the gap between the divided peaks remains unchanged when the refractive index of the filling materials n is less than 1 . 4 and more than 1 . 48 . The gap change is remarkable when the refractive index is in the 1 . 4<n<1 . 48 range and it reaches the maximum at n=1 . 44 . The specific LPFG structure designed in this manuscript can not only compensate for the defect of easy-to-breaking for half-etched LPFG,but also increase the detection sensibility to gas and liquid by changing the filling materials and calibrating the gap between the divided peaks.