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Control of light scattering by nanoparticles with optically-induced magnetic responses

Control of light scattering by nanoparticles with optically-induced magnetic responses

作     者:刘伟 Andrey E. Miroshnichenko Yuri S. Kivshar 

作者机构:College of Optoelectronic Science and Engineering National University of Defence Technology Nonlinear Physics Center and Center for Ultrahigh-bandwidth Devices for Optical Systems CUDOS) Research School of Physics and EngineeringAustralian National University 

出 版 物:《Chinese Physics B》 (中国物理B(英文版))

年 卷 期:2014年第23卷第4期

页      面:41-51页

核心收录:

学科分类:070207[理学-光学] 07[理学] 070205[理学-凝聚态物理] 08[工学] 080501[工学-材料物理与化学] 0805[工学-材料科学与工程(可授工学、理学学位)] 0704[理学-天文学] 0803[工学-光学工程] 0702[理学-物理学] 

基  金:Project supported by the Australian Research Council Center of Excellence for Ultrahigh Bandwidth Devices for Optical Systems(Grant No.CE110001018) the Future Fellowship(Grant No.FT110100037) 

主  题:optically-induced magnetic response scattering control Mie resonance Fano resonance 

摘      要:Conventional approaches to control and shape the scattering pattems of light generated by different nanostructures are mostly based on engineering of their electric response due to the fact that most metallic nanostructures support only electric resonances in the optical frequency range. Recently, fuelled by the fast development in the fields of metamaterials and plasmonics, artificial optically-induced magnetic responses have been demonstrated for various nanostructures. This kind of response can be employed to provide an extra degree of freedom for the efficient control and shaping of the scattering patterns of nanoparticles and nanoantennas. Here we review the recent progress in this research direction of nanoparticle scattering shaping and control through the interference of both electric and optically-induced magnetic responses. We discuss the magnetic resonances supported by various structures in different spectral regimes, and then summarize the original results on the scattering shaping involving both electric and magnetic responses, based on the interference of both spectrally separated (with different resonant wavelengths) and overlapped dipoles (with the same resonant wavelength), and also other higher-order modes. Finally, we discuss the scattering control utilizing Fano resonances associated with the magnetic responses.

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