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Polarized excitons in nanorings and the optical Aharonov-Bohm effect

A. O. Govorov, S. E. Ulloa, K. Karrai, and R. J. Warburton
Phys. Rev. B 66, 081309(R) – Published 30 August 2002
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Abstract

The quantum nature of matter lies in the wave function phases that accumulate while particles move along their trajectories. A prominent example is the Aharonov-Bohm phase, which has been studied in connection with the conductance of nanostructures. However, optical response in solids is determined by neutral excitations, for which no sensitivity to magnetic flux would be expected. We propose a mechanism for the topological phase of a neutral particle, a polarized exciton confined to a semiconductor quantum ring. We predict that this magnetic-field induced phase may strongly affect excitons in a system with cylindrical symmetry, resulting in switching between “bright” exciton ground states and novel “dark” states with nearly infinite lifetimes. Since excitons determine the optical response of semiconductors, the predicted phase can be used to tailor photon emission from quantum nanostructures.

  • Received 28 May 2002

DOI:https://doi.org/10.1103/PhysRevB.66.081309

©2002 American Physical Society

Authors & Affiliations

A. O. Govorov

  • Department of Physics and Astronomy, Nanoscale and Quantum Phenomena Institute, Ohio University, Athens, Ohio 45701-2979 and Institute of Semiconductor Physics, Russian Academy of Sciences, Siberian Branch, 630090 Novosibirsk, Russia

S. E. Ulloa

  • Department of Physics and Astronomy, Nanoscale and Quantum Phenomena Institute, Ohio University, Athens, Ohio 45701-2979

K. Karrai

  • Center for NanoScience, Ludwig-Maximilians-Universität Müchen, Geschwister-Scholl-Platz 1, 80539 München, Germany

R. J. Warburton

  • Department of Physics, Heriot-Watt University, Edinburgh, United Kingdom

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Vol. 66, Iss. 8 — 15 August 2002

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