Table 3.
Solvent | Simulation Time / ps b | R2 | Fast process | Slow process | Offset | |||
---|---|---|---|---|---|---|---|---|
Δ1 / ps−2 | τ1 / ps | Δ2 / ps−2 | τ2 / ps | Δ0 / ps−2 | ||||
n-Hexane | 1008 | 0.98 | 0.640 | 0.108 | 0.242 | 0.861 | 0.051 | |
Dibutyl ether | 1402 | 0.99 | 0.430 | 0.162 | 0.310 | 4.57 | 0.237 | |
Tetrahydrofuran | 1242 | 0.99 | 0.553 | 0.151 | 0.452 | 2.30 | 0.006 | |
Valeronitrile | 986.3 | 0.99 | 0.611 | 0.141 | 0.431 | 2.84 | -0.031 | |
Acetonitrile | 1895 | 0.99 | 0.898 | 0.112 | 0.167 | 1.11 | 0.020 | |
Dimethyl sulfoxide | 1361 | 0.99 | 0.696 | 0.104 | 0.317 | 1.99 | 0.022 | |
Water | 699.8 | 0.98 | 0.432 | 0.080 | 0.465 | 0.928 | 0.041 |
Autocorrelation functions were calculated for the field experienced by the vibration (|Fvib|), and then fit to the function: CFF (t) = Δ0 + Δ1 exp(−t/τ1)+ Δ2 exp(−t/τ2).
Data reflect results from the long (less stringent) simulations of acetophenone in a box filled with various solvents. Electric fields were sampled every 10 fs. Fits were carried out on the first 10 ps of the correlation function, after which the correlation function mostly oscillated around zero.