Dynamics of water and ions near DNA: comparison of simulation to time-resolved stokes-shift experiments.

Time-resolved Stokes-shift experiments measure the dynamics of biomolecules and of the perturbed solvent near them on subnanosecond time scales, but molecular dynamics simulations are needed to provide a clear interpretation of the results. Here we show that simulations using standard methods quantitatively reproduce the main features of TRSS experiments in DNA and provide a molecular assignment for the dynamics. The simulations reproduce the magnitude and unusual power-law dynamics of the Stokes shift seen in recent experiments [ Andreatta, D., et al. J. Am. Chem. Soc. 2005, 127, 7270 ]. A polarization model is introduced to eliminate cross-correlations between the different components contributing to the signal. Using this model, well-defined contributions of the DNA, water, and counterion to the experimental signal are extracted. Water is found to have the largest contribution and to be responsible for the power-law dynamics. The counterions have a smaller, but non-negligible, contribution with a time constant of 220 ps. The contribution to the signal of the DNA itself is minor and fits a 30 ps stretched exponential. Both time-averaged and dynamic distributions are calculated. They show a small subset of ions with a different coupling but no other evidence of substates or rate heterogeneity.

Ultrafast dynamics in DNA: "fraying" at the end of the helix.

The dynamics of the electric fields in the interior of DNA are measured by using oligonucleotides in which a native base pair is replaced by a dye molecule (coumarin 102) whose emission spectrum is sensitive to the local electric field. Time-resolved measurements of the emission spectrum have been extended to a six decade time range (40 fs to 40 ns) by combining results from time-correlated photon counting, fluorescence up-conversion, and transient absorption. Recent results showed that when the reporter is placed in the center of the oligonucleotide, the dynamics are very broadly distributed over this entire time range and do not show specific time constants associated with individual processes (Andreatta, D.; et al. J. Am. Chem. Soc. 2005, 127, 7270). This paper examines an oligonucleotide with the reporter near its end. The broadly distributed relaxation seen before remains with little attenuation. In addition, a new relaxation with a well-defined relaxation time of 5 ps appears. This process is assigned to the rapid component of "fraying" at the end of the helix.

Power-law solvation dynamics in DNA over six decades in time.

Time-resolved Stokes shifts in a dye-containing oligonucleotide have been observed over the entire time range from 40 fs to 40 ns. The dynamics fit to a power law with a small exponent of 0.15. Similar relaxation has been seen in proteins but has not been anticipated in DNA. Distinct relaxation components due to specific subcomponents of the system, bulk water, bound water, counterions, backbone, bases, and so on, are not found. The various subcomponents may be so strongly coupled that their motions cannot be treated separately.

Effect of lesions on the dynamics of DNA on the picosecond and nanosecond timescales using a polarity sensitive probe.

This paper explores the effects of structural modifications on the fast dynamics of DNA and the ability of time-resolved Stokes shift spectroscopy to measure those changes. The time-resolved Stokes shift of a synthetic coumarin base-pair replacement within an oligomer is measured between 40 ps and 40 ns. Comparisons are made between 17mers without modification, with a deleted base near the coumarin and with the coumarin placed near the end of the oligomer. The deletion of a next-to-nearest-neighbor base pair does not change the subnanosecond dynamics, but does cause an additional motion with a time constant of approximately 20 ns. A candidate for this motion is the flipping of the abasic sugar out of the helix and the concomitant intrusion of water into the interior of the helix. A nearby chain end causes little change in the dynamics after 1 ns but leads to a reduction in the amplitude of the dynamics between 40 ps and 1 ns. We suggest that at the chain end, where DNA on one side of the probe has been replaced by water, the charge- stabilizing dynamics have the same overall amplitude, but that much of the relaxation occurs before the start of the measurement time window.