2021
DOI: 10.1103/physrevb.103.235422
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Generalized electromagnetic theorems for nonlocal plasmonics

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Cited by 7 publications
(4 citation statements)
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“…It is worth noting however that classical consideration used here stops holding for the case of few nanometers and smaller particles where more detailed models of carrier behavior in the scatter need to be considered such as models taking into account non‐local effects. [ 84–86 ] Finally, one can observe how the backward‐forward scattering ratio behaves for the metals and dielectrics (see bottom of Figure 6). In all cases the forward‐backward scattering ratio Rbf${R_{bf}}$ starts with 0.5 which corresponds to the symmetric Rayleigh scattering.…”
Section: Mie Scatteringmentioning
confidence: 99%
“…It is worth noting however that classical consideration used here stops holding for the case of few nanometers and smaller particles where more detailed models of carrier behavior in the scatter need to be considered such as models taking into account non‐local effects. [ 84–86 ] Finally, one can observe how the backward‐forward scattering ratio behaves for the metals and dielectrics (see bottom of Figure 6). In all cases the forward‐backward scattering ratio Rbf${R_{bf}}$ starts with 0.5 which corresponds to the symmetric Rayleigh scattering.…”
Section: Mie Scatteringmentioning
confidence: 99%
“…The peaks in the electric field drastically increase the losses experienced by the gap plasmon, since the local absorption by the electron gas is proportional to E 1 • J * , where * denotes the complex conjugate [47]. This explains the larger imaginary part.…”
Section: A Lra With Spill-outmentioning
confidence: 99%
“…The peaks in the electric field drastically increase the losses experienced by the gap plasmon, since the local absorption by the electron gas is proportional to E 1 • J * , where * denotes the complex conjugate [43]. This explains the larger imaginary part.…”
Section: A Simplified Modelmentioning
confidence: 99%