物理学报
物理學報
물이학보
2013年
10期
250-255
,共6页
刘颖刚?%车伏龙%贾振安%傅海威%王宏亮%邵敏
劉穎剛?%車伏龍%賈振安%傅海威%王宏亮%邵敏
류영강?%차복룡%가진안%부해위%왕굉량%소민
微纳光纤%光纤布拉格光栅%折射率传感%数值模拟
微納光纖%光纖佈拉格光柵%摺射率傳感%數值模擬
미납광섬%광섬포랍격광책%절사솔전감%수치모의
micro/nanofiber%fiber Bragg grating%refractive index sensing%numerical simulation
利用光纤布拉格光栅方程和光纤基模有效折射率随纤芯半径和环境折射率的函数关系,建立了微纳光纤布拉格光栅(MNFBG)反射波长随环境折射率变化的数学模型,给出了波长灵敏度函数,并指出MNFBG反射波长的变化规律决定于有效折射率随纤芯半径和环境折射率变化的关系.详细探究了有效折射率及其灵敏度的变化规律,结果表明:有效折射率随纤芯半径和环境折射率的减小而非线性减小,其对环境折射率变化的灵敏度随环境折射率的增大而非线性增加,而且随纤芯半径减小,有效折射率的灵敏度、线性度以及线性响应范围均呈递增规律.通过对纤芯半径为0.5μm的MNFBG在1.20—1.30和1.33—1.43环境折射率范围内的波长响应关系拟合,分别获得了477.33 nm/RIU和856.30 nm/RIU的波长灵敏度以及99.58%和99.7%的高线性度,论证了分析结论以及折射率区间划分测量方案的正确性,为MNFBG折射率传感器的设计、优化以及应用提供了参考依据.
利用光纖佈拉格光柵方程和光纖基模有效摺射率隨纖芯半徑和環境摺射率的函數關繫,建立瞭微納光纖佈拉格光柵(MNFBG)反射波長隨環境摺射率變化的數學模型,給齣瞭波長靈敏度函數,併指齣MNFBG反射波長的變化規律決定于有效摺射率隨纖芯半徑和環境摺射率變化的關繫.詳細探究瞭有效摺射率及其靈敏度的變化規律,結果錶明:有效摺射率隨纖芯半徑和環境摺射率的減小而非線性減小,其對環境摺射率變化的靈敏度隨環境摺射率的增大而非線性增加,而且隨纖芯半徑減小,有效摺射率的靈敏度、線性度以及線性響應範圍均呈遞增規律.通過對纖芯半徑為0.5μm的MNFBG在1.20—1.30和1.33—1.43環境摺射率範圍內的波長響應關繫擬閤,分彆穫得瞭477.33 nm/RIU和856.30 nm/RIU的波長靈敏度以及99.58%和99.7%的高線性度,論證瞭分析結論以及摺射率區間劃分測量方案的正確性,為MNFBG摺射率傳感器的設計、優化以及應用提供瞭參攷依據.
이용광섬포랍격광책방정화광섬기모유효절사솔수섬심반경화배경절사솔적함수관계,건립료미납광섬포랍격광책(MNFBG)반사파장수배경절사솔변화적수학모형,급출료파장령민도함수,병지출MNFBG반사파장적변화규률결정우유효절사솔수섬심반경화배경절사솔변화적관계.상세탐구료유효절사솔급기령민도적변화규률,결과표명:유효절사솔수섬심반경화배경절사솔적감소이비선성감소,기대배경절사솔변화적령민도수배경절사솔적증대이비선성증가,이차수섬심반경감소,유효절사솔적령민도、선성도이급선성향응범위균정체증규률.통과대섬심반경위0.5μm적MNFBG재1.20—1.30화1.33—1.43배경절사솔범위내적파장향응관계의합,분별획득료477.33 nm/RIU화856.30 nm/RIU적파장령민도이급99.58%화99.7%적고선성도,론증료분석결론이급절사솔구간화분측량방안적정학성,위MNFBG절사솔전감기적설계、우화이급응용제공료삼고의거.
@@@@Using the fiber Bragg grating equation and the functional relation of the fundamental effective mode refractive index (RI), the mathematical model of the wavelength shift and the relational function of wavelength sensitivity are established, when the reflected wavelength of the micro/nanofiber Bragg grating (MNFBG) changes with ambient RI and the fiber radius. The theoretical relationship demonstrates that the variation of MNFBG reflected wavelengths is dependent on the change of effective RI with fiber radius and ambient RI. Meanwhile, we also study the variation of effective RI and its sensitivity in detail. The results show that the effective RI nonlinearly decreases with fiber-core radius and ambient refractive index decreasing, and its sensitivity increases as the ambient refractive index increases, and the sensitivity, linearity and the linear response range increase with the decrease of the fiber radius. For a fiber radius of 0.5 μm, by simulating the curves of the effective index versus ambient RI in the index ranges of 1.20–1.30 and 1.33–1.43 respectively, the values of wavelength sensitivity of 477.33 nm/RIU and 856.30 nm/RIU and the values of high linearity of 99.2%and 99.7%are obtained, which not only verifies the analysis conclusions and the measurement program for RI sensing with MNFBG, but also supplies references for the RI sensor design, optimization and the application.