2023
DOI: 10.1103/physrevresearch.5.023116
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Resonant helicity mixing of electromagnetic waves propagating through matter

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“…We also use (x ± i ŷ) = e ±iφ ( ρ ± i φ) (7) to compare with (1) and (2). Importantly, when we use the nanostructures excited by a vortex beam, such combinations do not appear for internal or scattered fields [36], while the resonant frequencies of magnetic and electric multipoles a generally different, except the helicity-preserving structures [40][41][42]. Thus, further we can just consider the total angular momentum projection of a beam m in , and the problem becomes almost fully analogous to the one considered in [32].…”
Section: Multipolar Content Of the Vortex Beamsmentioning
confidence: 99%
“…We also use (x ± i ŷ) = e ±iφ ( ρ ± i φ) (7) to compare with (1) and (2). Importantly, when we use the nanostructures excited by a vortex beam, such combinations do not appear for internal or scattered fields [36], while the resonant frequencies of magnetic and electric multipoles a generally different, except the helicity-preserving structures [40][41][42]. Thus, further we can just consider the total angular momentum projection of a beam m in , and the problem becomes almost fully analogous to the one considered in [32].…”
Section: Multipolar Content Of the Vortex Beamsmentioning
confidence: 99%