2003
DOI: 10.1016/s0009-2614(03)00159-3
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Computer simulations of the solvation dynamics of Coumarin 153 in dimethylsulfoxide

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Cited by 21 publications
(25 citation statements)
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“…The important result for present purposes is that the equilibrium C g;G ( t ) was shown to be (surprisingly) a very good approximation for a significant fraction (∼2/3) of the nonequilibrium S ( t )’s decay for the modeled non-hydrogen-bonding polar solvent CH 3 Cl. Similar success of a Gaussian time dependence for S ( t ) was found by Maroncelli for acetonitrile (CH 3 CN) solvent, ,, and by other authors for other solvents. ,,, This success rather strongly supported the inertial perspective: the dominant effect is of the solvent molecules’ initial free streaming motion, changing their positions and thus the energy gap. However, as anticipated in ref .…”
Section: Theoretical Analysissupporting
confidence: 79%
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“…The important result for present purposes is that the equilibrium C g;G ( t ) was shown to be (surprisingly) a very good approximation for a significant fraction (∼2/3) of the nonequilibrium S ( t )’s decay for the modeled non-hydrogen-bonding polar solvent CH 3 Cl. Similar success of a Gaussian time dependence for S ( t ) was found by Maroncelli for acetonitrile (CH 3 CN) solvent, ,, and by other authors for other solvents. ,,, This success rather strongly supported the inertial perspective: the dominant effect is of the solvent molecules’ initial free streaming motion, changing their positions and thus the energy gap. However, as anticipated in ref .…”
Section: Theoretical Analysissupporting
confidence: 79%
“…It is important to stress for later reference that, accordingly, the Coulomb force figures neither in the initial distribution nor in the dynamics . The second approximation is that the equilibrium TCF’s short time dynamics can be approximated by a Gaussian in time, ,,,, characterized by a ground state frequency ω g . ,, Here, the second line involves the inertial Liouville operator p ·∇ r , while the last line is the evaluation for the present Coulomb potential energy case, and β is ( k B T ) −1 .…”
Section: Theoretical Analysismentioning
confidence: 99%
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“…As the computer simulation requires averaging over a large number of independent simulations and is therefore timeconsuming, only few studies focus solely on nonequilibrium simulation. [7][8][9][10] More often, nonequilibrium computational solvation dynamics is accompanied [11][12][13][14][15][16] or even replaced 4,[17][18][19][20][21][22][23][24][25] by equilibrium molecular dynamics simulation. Here, the nature of DUðtÞ is assumed to depend linearly on the perturbation, so that the nonequilibrium event can be described by the energy fluctuations present in the equilibrium state of the system.…”
Section: Introductionmentioning
confidence: 99%