2017
DOI: 10.1103/physrevapplied.8.064010
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Enantiospecific Detection of Chiral Nanosamples Using Photoinduced Force

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Cited by 29 publications
(56 citation statements)
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“…16 Compared to s-SNOM in which the excitation is in near field and the detection is in the far field, in PiFM both the excitation and detection take place in near field which effectively suppresses the background scattering photons from the far field. 17,18 As a result, PiFM has been widely used for stimulated Raman spectroscopy, 19,20 nanoscale mapping of tightly focused electromagnetic beams 21,22 and propagating surface plasmon polaritons, 23 enantioselectivity of chiral nanostructures, 24,25…”
mentioning
confidence: 99%
“…16 Compared to s-SNOM in which the excitation is in near field and the detection is in the far field, in PiFM both the excitation and detection take place in near field which effectively suppresses the background scattering photons from the far field. 17,18 As a result, PiFM has been widely used for stimulated Raman spectroscopy, 19,20 nanoscale mapping of tightly focused electromagnetic beams 21,22 and propagating surface plasmon polaritons, 23 enantioselectivity of chiral nanostructures, 24,25…”
mentioning
confidence: 99%
“…See more details in the supplemental materials, and in Refs. 26,27 ). Moreover, we assume that every field is monochromatic and the time dependence exp( ) it   is assumed and suppressed, and the International System of Units (SI) is utilized throughout the paper.…”
Section: ) Objective and Operational Principlementioning
confidence: 99%
“…Note that this dipolar approximation has successfully been exploited to model photo-induced force microscopy in Refs. 23,26,27,33 to extract optical properties of samples. Here, we model the sample with its photo-induced electric and magnetic dipole moments p and m , respectively, given by [34][35][36] polarizabilities α em , and α me and is chosen following Ref.…”
Section: ) Introductionmentioning
confidence: 99%
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