级联声光器件与回音壁模式微腔实现非对称传输OACSTPCD
Asymmetric transmission of cascaded acousto-optic device and whispering gallery mode microcavity
本文提出利用级联声光效应器和耦合回音壁模式微球腔的方案来实现非对称传输效果,并进行理论和实验验证.实验中利用加热拉锥的方式制备了两段式光纤,可同时实现声光效应的激发和回音壁模式的耦合.利用光纤中声光效应将纤芯基模中的矢量模式转换到包层高阶模式,由于基模中不同矢量模式转换包层模式的矢量模式也不同,从而产生类似双折射效果,使输出的包层模式产生偏振变化.而后通过耦合回音壁模式微腔将包层模式转换回纤芯基模.由于回音壁模式的偏振选择效果,使得相反方向入射光能量具有不同的透射特性,其传输隔离度可达 17 dB.此外,对两个方向传输的透射率随偏振角度变化进行测试,测得声光效应带来的偏振变化约为 80°.本文的非对称传输方案继承了声光器件响应迅速、调谐性良好的优势,同时具有全光纤结构和无工作阈值的特点,在光开关、光隔离器等场景具有重要的应用潜力.
In this paper,an asymmetric transmission scheme is proposed by cascading an acousto-optic device and a coupled whispering gallery mode(WGM)microsphere cavity,and it is demonstrated theoretically and experimentally.With the acousto-optic interaction in a fiber,the vector modes of the fundamental core mode can be converted into the different vector modes of a cladding(linear polarization,LP)mode,and because of the optical path difference between the cladding vector modes,the polarization of the cladding mode will be changed.The cladding mode can be converted back into the core fundamental mode by coupling a WGM microcavity.By calculating the overlapping of the mode fields in the tapered fiber and the microcavity at the resonance wavelength,the coupling coefficients between different LP modes and WGM will be solved.And,the transmitivities and conversion coefficients of the two fiber modes can be obtained on condition that the polarization of the incident light does not coincide with the polarization orientation of the WGM.The transmission spectra of the coupled WGM microcavity are calculated by using Matlab program for eight states,including the states at different incident directions,different incident polarizations of input,whether the acoustic wave is on or off.The results show that the conversion coefficient from the cladding mode to the core mode is completely different from that of the contrary process when the acoustic wave is working.And the forward incident light and backward incident light have completely different transmission characteristics,thus resulting in the asymmetric transmission.The transmittances of forward incidence and reverse incidence at different polarizations are also studied,both of them change periodically with the polarization angle,and their phase difference is equal to the polarization change caused by acousto-optic interaction in the fiber.In the experiment,a two-stage tapered fiber is used to realize the acousto-optic interaction and the coupling of whispering gallery mode at the same time.By controlling the working states of the system,the same 8 states as in the calculation are studied experimentally.The results show that due to the polarization-selection effect of the WGM,the light energy incident from the opposite directions will show different transmission characteristics.While the forward transmittance reaches a maximum value of about 0.505,the reverse transmittance reaches a minimum value of about 0.010,and the transmission isolation reaches about 17 dB.The transmittances in two directions are measured at different incident polarization angles,the transmission isolation is analyzed,and the polarization change of cladding mode in the fiber is verified to be about 80°.The measured results coincide with the calculations from the developed theory well.Finally,the shortcomings and optimization method of the scheme are discussed.The asymmetric transmission scheme in this paper inherits the advantages of rapid response and good tuning of acousto-optic device,and has an all-fiber structure,which has important application potential in optical switch and isolator.
吕宇曦;王晨;段添期;赵彤;常朋发;王安帮
太原理工大学电子信息与光学工程学院,新型传感器与智能控制教育部(山西省)重点实验室,太原 030024太原理工大学电子信息与光学工程学院,新型传感器与智能控制教育部(山西省)重点实验室,太原 030024||广东工业大学信息工程学院,广东省信息光子技术重点实验室,广州 510006
非对称传输声光效应回音壁模式微腔模式转换
asymmetric transmissionacousto-optic effectwhispering gallery mode microcavitymode conversion
《物理学报》 2024 (001)
69-77 / 9
国家自然科学基金青年科学基金(批准号:62105233)、国家自然科学基金重点项目(批准号:62035009)、山西省自然科学基金(批准号:20210302124536,20210302123183)和应用光学国家重点实验开放课题(批准号:SKLAO2022001A09)资助的课题.Project supported by the Young Scientists Fund of the National Natural Science Foundation of China(Grant No.62105233),the Key Program of the National Natural Science Foundation of China(Grant No.62035009),the Natural Science Foundation of Shanxi Province,China(Grant Nos.20210302124536,20210302123183),and the Open Fund of State Key Laboratory of Applied Optics,China(Grant No.SKLAO2022001A09).
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