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Reflection and Phase Matching in Plasmonic Gold Tapers.
Guo, Surong; Talebi, Nahid; Sigle, Wilfried; Vogelgesang, Ralf; Richter, Gunther; Esmann, Martin; Becker, Simon F; Lienau, Christoph; van Aken, Peter A.
Afiliação
  • Guo S; Max Planck Institute for Solid State Research , Heisenbergstraße 1, 70569 Stuttgart, Germany.
  • Talebi N; Max Planck Institute for Solid State Research , Heisenbergstraße 1, 70569 Stuttgart, Germany.
  • Sigle W; Max Planck Institute for Solid State Research , Heisenbergstraße 1, 70569 Stuttgart, Germany.
  • Vogelgesang R; Institute of Physics and Center of Interface Science, Carl von Ossietzky University of Oldenburg , 26129 Oldenburg, Germany.
  • Richter G; Max Planck Institute for Intelligent Systems , Heisenbergstr. 3, 70569 Stuttgart, Germany.
  • Esmann M; Institute of Physics and Center of Interface Science, Carl von Ossietzky University of Oldenburg , 26129 Oldenburg, Germany.
  • Becker SF; Institute of Physics and Center of Interface Science, Carl von Ossietzky University of Oldenburg , 26129 Oldenburg, Germany.
  • Lienau C; Institute of Physics and Center of Interface Science, Carl von Ossietzky University of Oldenburg , 26129 Oldenburg, Germany.
  • van Aken PA; Max Planck Institute for Solid State Research , Heisenbergstraße 1, 70569 Stuttgart, Germany.
Nano Lett ; 16(10): 6137-6144, 2016 10 12.
Article em En | MEDLINE | ID: mdl-27552231
ABSTRACT
We investigate different dynamic mechanisms, reflection and phase matching, of surface plasmons in a three-dimensional single-crystalline gold taper excited by relativistic electrons. Plasmonic modes of gold tapers with various opening angles from 5° to 47° are studied both experimentally and theoretically, by means of electron energy-loss spectroscopy and finite-difference time-domain numerical calculations, respectively. Distinct resonances along the taper shaft are observed in tapers independent of opening angles. We show that, despite their similarity, the origin of these resonances is different at different opening angles and results from a competition between two coexisting mechanisms. For gold tapers with large opening angles (above ∼20°), phase matching between the electron field and that of higher-order angular momentum modes of the taper is the dominant contribution to the electron energy-loss because of the increasing interaction length between electron and the taper near-field. In contrast, reflection from the taper apex dominates the EELS contrast in gold tapers with small opening angles (below ∼10°). For intermediate opening angles, a gradual transition of these two mechanisms was observed.
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Base de dados: MEDLINE Idioma: En Ano de publicação: 2016 Tipo de documento: Article
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Base de dados: MEDLINE Idioma: En Ano de publicação: 2016 Tipo de documento: Article