2000
DOI: 10.1002/1097-461x(2000)80:4/5<1043::aid-qua53>3.0.co;2-e
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Application of the density matrix method to spectroscopy and dynamics of photosynthetic reaction centers

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Cited by 7 publications
(1 citation statement)
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“…The density matrix was propagated with time at 80 K by Runge–Kutta integration of the stochastic Liouville equation, including terms for coherence transfer and vibrational relaxations. ,, The time constant for thermal equilibration of the two lowest levels of each vibrational mode was taken to be 2.0 ps. Time constants for pure dephasing due to vibrational and electronic inhomogeneity were set at 100 ps (too long for this process to affect the results).…”
Section: Methodsmentioning
confidence: 99%
“…The density matrix was propagated with time at 80 K by Runge–Kutta integration of the stochastic Liouville equation, including terms for coherence transfer and vibrational relaxations. ,, The time constant for thermal equilibration of the two lowest levels of each vibrational mode was taken to be 2.0 ps. Time constants for pure dephasing due to vibrational and electronic inhomogeneity were set at 100 ps (too long for this process to affect the results).…”
Section: Methodsmentioning
confidence: 99%