Abstract
A method to simulate nonadiabatic rate constants in condensed phases was developed. Such a method was based on a novel path integral representation of the imaginary time flux-flux correlation function. Thus, this representation does not have the standard alternating weight problem that plagues other imaginary time path integral approaches to multistate systems. This paper employs the maximum entropy (MaxEnt) formalism to accomplish the desired continuation.
Original language | English |
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Pages (from-to) | 457-460 |
Number of pages | 4 |
Journal | Journal of Chemical Physics |
Volume | 118 |
Issue number | 2 |
DOIs | |
State | Published - 8 Jan 2003 |