2012
DOI: 10.1021/nn304855t
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Mirror-Image-Induced Magnetic Modes

Abstract: Reflection in a mirror changes the handedness of the real world, and right-handed objects turn left-handed and vice versa (M. Gardner, The Ambidextrous Universe, Penguin Books, 1964). Also, we learn from electromagnetism textbooks that a flat metallic mirror transforms an electric charge into a virtual opposite charge. Consequently, the mirror image of a magnet is another parallel virtual magnet as the mirror image changes both the charge sign and the curl handedness. Here we report the dramatic modification i… Show more

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Cited by 66 publications
(96 citation statements)
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References 38 publications
(63 reference statements)
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“…Here, we experimentally confirm this for the hybrid nanocavity by studying the RS from c‐Si NPs with different diameters placed on 60 nm Au film. For the wavelength of 632.8 nm used as a pump in Raman spectroscopy, NPs with diameters of 180 ± 10 and 250 ± 10 nm demonstrate in average 100‐fold enhancement for RS signal owing to the electric dipole (ED') and magnetic quadrupole (MQ') resonances modified by their mirror images (Figure c). It should be stressed that the obtained RS signal from the resonant c‐Si NPs on Au film is two order of magnitude higher than that of c‐Si NPs on glass at the same condition due to the greater values of both optical field enhancement and mode volume inside the NP, and also enhanced out‐coupling RS signal in backscattering geometry.…”
Section: Resultsmentioning
confidence: 99%
“…Here, we experimentally confirm this for the hybrid nanocavity by studying the RS from c‐Si NPs with different diameters placed on 60 nm Au film. For the wavelength of 632.8 nm used as a pump in Raman spectroscopy, NPs with diameters of 180 ± 10 and 250 ± 10 nm demonstrate in average 100‐fold enhancement for RS signal owing to the electric dipole (ED') and magnetic quadrupole (MQ') resonances modified by their mirror images (Figure c). It should be stressed that the obtained RS signal from the resonant c‐Si NPs on Au film is two order of magnitude higher than that of c‐Si NPs on glass at the same condition due to the greater values of both optical field enhancement and mode volume inside the NP, and also enhanced out‐coupling RS signal in backscattering geometry.…”
Section: Resultsmentioning
confidence: 99%
“…[ 43 ] Placing resonators on a metal substrate, however, gives a full 2π phase shift due to interference with image modes in the substrate. [ 44 ] Unlike metallic resonators, these dielectric resonators have negligible losses (imaginary part of refractive index ≈ 10 −3 ). As a result, the refl ection has a near unity amplitude at all wavelengths, an ideal characteristic for a refl ect array metasurface.…”
Section: Full Paper Full Paper Full Papermentioning
confidence: 99%
“…The solutions for this problem proposed earlier , albeit finding their applications for modelling the near‐field of low‐index nanoparticles on metallic substrates , involve laborious calculations. Thus, most of the analysis of the scattering of nanoparticles on substrates tends to be either qualitative or based on finite element methods . A promising analytical model was proposed recently in the work by Miroshnichenko et al.…”
Section: Introductionmentioning
confidence: 99%