Abstract
The time-dependent perturbation theory that we have used to treat resonance energy transfer and absorption of light assumes that we know that a system is in a given state (state 1), so the coefficient associated with this state (C1) is 1, while the coefficient for finding the system in a different state (C2) is zero. The resulting expression for the rate of transitions to state 2 (Eq. (2.58) or Eq. (7.8)) neglects the possibility of a return to state 1. It can continue to hold at later times only if the transition to state 2 is followed by a relaxation that takes the two states out of resonance.
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© 2009 Springer-Verlag Berlin Heidelberg
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(2009). Coherence and Dephasing. In: Modern Optical Spectroscopy. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-540-37542-5_10
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DOI: https://doi.org/10.1007/978-3-540-37542-5_10
Publisher Name: Springer, Berlin, Heidelberg
Print ISBN: 978-3-540-95895-6
Online ISBN: 978-3-540-37542-5
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