We study electronic image states around a metallic nanoring and show that the interplay between the attractive polarization force and a repulsive centrifugal force gives rise to Rydberg-like image states trapped several nanometers away from the surface. The nanoring is modeled as a perfectly conducting isolated torus whose classical electrostatic image potential is derived analytically. The image states are computed via a two-dimensional finite-difference scheme as solutions of the effective Schrödinger equation describing the outer electron subject to this image potential. These findings demonstrate not only the existence of detached image states around nanorings but allow us also to provide general criteria on the ring geometry, i.e., the aspect ratio of the torus, that need to be fulfilled in order to support such states.
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21 May 2017
Research Article|
May 19 2017
Highly excited electronic image states of metallic nanorings
Christian Fey;
Christian Fey
a)
1Zentrum für optische Quantentechnologien,
Universität Hamburg
, Luruper Chaussee 149, 22761 Hamburg, Germany
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Henrik Jabusch;
Henrik Jabusch
1Zentrum für optische Quantentechnologien,
Universität Hamburg
, Luruper Chaussee 149, 22761 Hamburg, Germany
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Johannes Knörzer;
Johannes Knörzer
b)
1Zentrum für optische Quantentechnologien,
Universität Hamburg
, Luruper Chaussee 149, 22761 Hamburg, Germany
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Peter Schmelcher
Peter Schmelcher
c)
1Zentrum für optische Quantentechnologien,
Universität Hamburg
, Luruper Chaussee 149, 22761 Hamburg, Germany
2The Hamburg Centre for Ultrafast Imaging,
Universität Hamburg
, Luruper Chaussee 149, 22761 Hamburg, Germany
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b)
Current address: Max-Planck-Institut für Quantenoptik, Hans-Kopfermann-Str. 1, 85748 Garching, Germany.
J. Chem. Phys. 146, 194704 (2017)
Article history
Received:
March 08 2017
Accepted:
April 28 2017
Citation
Christian Fey, Henrik Jabusch, Johannes Knörzer, Peter Schmelcher; Highly excited electronic image states of metallic nanorings. J. Chem. Phys. 21 May 2017; 146 (19): 194704. https://doi.org/10.1063/1.4983294
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