物理学报
物理學報
물이학보
2013年
3期
173-179
,共7页
刘超%裴丽?%李卓轩%宁提纲%高嵩%康泽新%孙将
劉超%裴麗?%李卓軒%寧提綱%高嵩%康澤新%孫將
류초%배려?%리탁헌%저제강%고숭%강택신%손장
声光调制%光纤布拉格光栅%傅里叶模式耦合理论%光谱特性
聲光調製%光纖佈拉格光柵%傅裏葉模式耦閤理論%光譜特性
성광조제%광섬포랍격광책%부리협모식우합이론%광보특성
acousto-optic modulation%fiber Bragg grating%Fourier mode coupling theory%spectral characteristics
将光纤光栅的傅里叶模式耦合理论应用于光纤布拉格光栅型全光纤声光调制器的理论分析中.与现有的分析方法相比,该模型算法简单、求解容易,能够快速有效地获得调制器的传输特性.基于该模型,理论分析了超声波频率及声致应变幅度对调制器特性的影响.仿真结果表明,该调制器反射谱的主反射峰与次反射峰的波长间隔与超声波频率成正比,反射峰的反射率随着声致应变幅度的改变而发生周期性的变化.另外,在同一声致应变幅度下,低频超声波调制的光栅反射中存在更多的次反射,光栅反射能量的周期性变化更加明显.实验中,使用频率为885.5 kHz的超声波对光纤布拉格光栅进行调制.实验结果与仿真结果相一致.
將光纖光柵的傅裏葉模式耦閤理論應用于光纖佈拉格光柵型全光纖聲光調製器的理論分析中.與現有的分析方法相比,該模型算法簡單、求解容易,能夠快速有效地穫得調製器的傳輸特性.基于該模型,理論分析瞭超聲波頻率及聲緻應變幅度對調製器特性的影響.倣真結果錶明,該調製器反射譜的主反射峰與次反射峰的波長間隔與超聲波頻率成正比,反射峰的反射率隨著聲緻應變幅度的改變而髮生週期性的變化.另外,在同一聲緻應變幅度下,低頻超聲波調製的光柵反射中存在更多的次反射,光柵反射能量的週期性變化更加明顯.實驗中,使用頻率為885.5 kHz的超聲波對光纖佈拉格光柵進行調製.實驗結果與倣真結果相一緻.
장광섬광책적부리협모식우합이론응용우광섬포랍격광책형전광섬성광조제기적이론분석중.여현유적분석방법상비,해모형산법간단、구해용역,능구쾌속유효지획득조제기적전수특성.기우해모형,이론분석료초성파빈솔급성치응변폭도대조제기특성적영향.방진결과표명,해조제기반사보적주반사봉여차반사봉적파장간격여초성파빈솔성정비,반사봉적반사솔수착성치응변폭도적개변이발생주기성적변화.령외,재동일성치응변폭도하,저빈초성파조제적광책반사중존재경다적차반사,광책반사능량적주기성변화경가명현.실험중,사용빈솔위885.5 kHz적초성파대광섬포랍격광책진행조제.실험결과여방진결과상일치.
The Fourier mode coupling theory is applied to the analysis of the fiber Bragg grating based all-fiber acousto-optic modulator for the first time. Compared with the existing analysis methods, the algorithm of this model is simple and easy, and transmission characteristics of the modulator can be acquired effectively and efficiently. Based on the theory, the performances of the modulator, related to ultrasonic frequency and amplitude of acoustically induced strain, are investigated. Simulation results show that in reflection spectra of the modulator, the wavelength interval between the primary relection peak and the secondary relection peak is proportional to ultrasonic frequency, and the reflectivity of the reflection peak varies periodically with intensity change of the amplitude of acoustically induced strain. In addition, with the same amplitude of acoustically induced strain, more secondary reflections exist in the low-frequency ultrasonic modulated fiber Bragg grating, and the periodic variation of the energy reflected by fiber Bragg graing is more obvious. In the experiment, the fiber Bragg graing is modulated by an ultrasonic wave with a frequency of 885.5 KHz. The experimental results accord well with the simulation results.