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Phonon-mediated path-interference in electronic energy transfer

Source: J. Chem. Phys. 136, 024112 (2012); http://dx.doi.org/10.1063/1.3675844

Published 13 January 2012

KEYWORDS and PACS
Keywords
PACS
  • 33.15.Mt
    Molecular rotation, vibration, and vibration-rotation constants
  • 33.20.Tp
    Vibrational analysis (molecular spectra)
  • 36.20.Ng
    Vibrational and rotational structure, infrared and Raman spectra of macromolecules
  • YEAR: 2011
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PUBLICATION DATA
ISSN:
1553-9628 (online)
Publisher:
AIP is a member of CrossRef AIP
Hoda Hossein-Nejad,1 Alexandra Olaya-Castro,2 and Gregory D. Scholes3
1Department of Physics, University of Toronto, 60 St. George St., Toronto, Ontario M5S 1A7, Canada
2Department of Physics and Astronomy, University College London, Gower Street, London WC1E 6BT, United Kingdom
3Lash Miller Chemical Laboratories, Institute for Optical Sciences and Centre for Quantum Information and Quantum Control, University of Toronto, 80 St. George St., Toronto, Ontario M5S 3H6, Canada

We present a formalism to quantify the contribution of path-interference in phonon-mediated electronic energy transfer. The transfer rate between two molecules is computed by considering the quantum mechanical amplitudes associated with pathways connecting the initial and final sites. This includes contributions from classical pathways, but also terms arising from interference of different pathways. We treat the vibrational modes coupled to the molecules as a non-Markovian harmonic oscillator bath, and investigate the correction to transfer rates due to the lowest-order interference contribution. We show that depending on the structure of the harmonic bath, the correction due to path-interference may have a dominant vibrational or electronic character, and can make a notable contribution to the transfer rate in the steady state. ©2012 American Institute of Physics
History: Received 2 November 2011; accepted 19 December 2011; published 13 January 2012
Digital Object Identifier: http://dx.doi.org/10.1063/1.3675844

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