Dataset.
Supporting Information for: Nonlinear optical response of a plasmonic nanoantenna to circularly polarized light: Rotation of multipolar charge density and near-field spin angular momentum inversion
Digital.CSIC. Repositorio Institucional del CSIC
oai:digital.csic.es:10261/342602
Digital.CSIC. Repositorio Institucional del CSIC
- Quijada, Marina
- Babaze, Antton
- Aizpurua, Javier
- Borisov, Andrei G.
Expression for the circularly polarized fundamental field convenient for an analysis of nonlinear effects; definition of the charge multipoles in cylindrical coordinates and induced potential of the nanowire; analysis of the induced nonlinear near field; definition of the linear multipolar polarizabilities; discussion on the time-to-frequency Fourier transform used to analyze the time-dependent results of the TDDFT and to obtain the frequency-resolved quantities; classical nonretarded calculations of the linear response; extended discussion of the symmetry constraints for the bulk contribution to nonlinear polarization; derivation of the selection rules based on the nonlinear density response formalism; results showing magnetization of the nanowire by a circularly polarized fundamental field pulse; and discussion of the Friedel oscillations of the ground-state electron density (PDF).
Time evolution of the charge density induced in the nanowire, δϱ(n)(r, t) = Re{δϱ(r, nΩ)e–inΩt }, at the fundamental frequency (n = 1) for circular polarization with SAM = 1 of the incoming field (MP4).
Time evolution of the charge density induced in the nanowire, δϱ(n)(r, t) = Re{δϱ(r, nΩ)e–inΩt }, at the n = 2 harmonic for circular polarization with SAM = 1 of the incoming field (MP4).
Time evolution of the charge density induced in the nanowire, δϱ(n)(r, t) = Re{δϱ(r, nΩ)e–inΩt }, at the n = 3 harmonic for circular polarization with SAM = 1 of the incoming field (MP4).
Time evolution of the charge density induced in the nanowire, δϱ(n)(r, t) = Re{δϱ(r, nΩ)e–inΩt }, at n = 4 harmonic for circular polarization with SAM = 1 of the incoming field (MP4).
Time evolution of the charge density induced in the nanowire, δϱ(n)(r, t) = Re{δϱ(r, nΩ)e–inΩt }, at the fundamental frequency (n = 1) for linear polarization of the incoming field (MP4).
Time evolution of the charge density induced in the nanowire, δϱ(n)(r, t) = Re{δϱ(r, nΩ)e–inΩt }, at the n = 2 harmonic for linear polarization of the incoming field (MP4).
Time evolution of the charge density induced in the nanowire, δϱ(n)(r, t) = Re{δϱ(r, nΩ)e–inΩt }, at the n = 3 harmonic for linear polarization of the incoming field (MP4).
Time evolution of the charge density induced in the nanowire, δϱ(n)(r, t) = Re{δϱ(r, nΩ)e–inΩt }, at the n = 4 harmonic for linear polarization of the incoming field (MP4)., Peer reviewed
DOI: http://hdl.handle.net/10261/342602
Digital.CSIC. Repositorio Institucional del CSIC
oai:digital.csic.es:10261/342602
HANDLE: http://hdl.handle.net/10261/342602
Digital.CSIC. Repositorio Institucional del CSIC
oai:digital.csic.es:10261/342602
Ver en: http://hdl.handle.net/10261/342602
Digital.CSIC. Repositorio Institucional del CSIC
oai:digital.csic.es:10261/342602
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Digital.CSIC. Repositorio Institucional del CSIC
oai:digital.csic.es:10261/342602
Dataset. 2023
SUPPORTING INFORMATION FOR: NONLINEAR OPTICAL RESPONSE OF A PLASMONIC NANOANTENNA TO CIRCULARLY POLARIZED LIGHT: ROTATION OF MULTIPOLAR CHARGE DENSITY AND NEAR-FIELD SPIN ANGULAR MOMENTUM INVERSION
Digital.CSIC. Repositorio Institucional del CSIC
- Quijada, Marina
- Babaze, Antton
- Aizpurua, Javier
- Borisov, Andrei G.
Expression for the circularly polarized fundamental field convenient for an analysis of nonlinear effects; definition of the charge multipoles in cylindrical coordinates and induced potential of the nanowire; analysis of the induced nonlinear near field; definition of the linear multipolar polarizabilities; discussion on the time-to-frequency Fourier transform used to analyze the time-dependent results of the TDDFT and to obtain the frequency-resolved quantities; classical nonretarded calculations of the linear response; extended discussion of the symmetry constraints for the bulk contribution to nonlinear polarization; derivation of the selection rules based on the nonlinear density response formalism; results showing magnetization of the nanowire by a circularly polarized fundamental field pulse; and discussion of the Friedel oscillations of the ground-state electron density (PDF).
Time evolution of the charge density induced in the nanowire, δϱ(n)(r, t) = Re{δϱ(r, nΩ)e–inΩt }, at the fundamental frequency (n = 1) for circular polarization with SAM = 1 of the incoming field (MP4).
Time evolution of the charge density induced in the nanowire, δϱ(n)(r, t) = Re{δϱ(r, nΩ)e–inΩt }, at the n = 2 harmonic for circular polarization with SAM = 1 of the incoming field (MP4).
Time evolution of the charge density induced in the nanowire, δϱ(n)(r, t) = Re{δϱ(r, nΩ)e–inΩt }, at the n = 3 harmonic for circular polarization with SAM = 1 of the incoming field (MP4).
Time evolution of the charge density induced in the nanowire, δϱ(n)(r, t) = Re{δϱ(r, nΩ)e–inΩt }, at n = 4 harmonic for circular polarization with SAM = 1 of the incoming field (MP4).
Time evolution of the charge density induced in the nanowire, δϱ(n)(r, t) = Re{δϱ(r, nΩ)e–inΩt }, at the fundamental frequency (n = 1) for linear polarization of the incoming field (MP4).
Time evolution of the charge density induced in the nanowire, δϱ(n)(r, t) = Re{δϱ(r, nΩ)e–inΩt }, at the n = 2 harmonic for linear polarization of the incoming field (MP4).
Time evolution of the charge density induced in the nanowire, δϱ(n)(r, t) = Re{δϱ(r, nΩ)e–inΩt }, at the n = 3 harmonic for linear polarization of the incoming field (MP4).
Time evolution of the charge density induced in the nanowire, δϱ(n)(r, t) = Re{δϱ(r, nΩ)e–inΩt }, at the n = 4 harmonic for linear polarization of the incoming field (MP4)., Peer reviewed
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