6519 - 6520 |
Tribute to Hans C. Andersen Chandler D, Weeks JD |
6521 - 6528 |
Autobiographical sketch of Hans C. Andersen Andersen HC |
6529 - 6535 |
Free energy of oxidation of metal aqua ions by an enforced change of coordination Blumberger J, Sprik M |
6536 - 6543 |
Vibrational echoes: Dephasing, rephasing, and the stability of classical trajectories Noid WG, Ezra GS, Loring RF |
6544 - 6554 |
Hydrogen bond networks: Structure and evolution after hydrogen bond breaking Asbury JB, Steinel T, Fayer MD |
6555 - 6563 |
Understanding the limitations of the virial in the simulation of nanosystems: A puzzle that stimulated the search for understanding Reiss H, Reguera D |
6564 - 6570 |
Asymmetry in the shapes of folded and denatured states of proteins Dima RI, Thirumalai D |
6571 - 6581 |
Describing protein folding kinetics by molecular dynamics simulations. 1. Theory Swope WC, Pitera JW, Suits F |
6582 - 6594 |
Describing protein folding kinetics by molecular dynamics simulations. 2. Example applications to alanine dipeptide and beta-hairpin peptide Swope WC, Pitera JW, Suits F, Pitman M, Eleftheriou M, Fitch BG, Germain RS, Rayshubski A, Ward TJC, Zhestkov Y, Zhou R |
6595 - 6602 |
On the calculation of diffusion coefficients in confined fluids and interfaces with an application to the liquid-vapor interface of water Liu P, Harder E, Berne BJ |
6603 - 6610 |
Hydrogen bonding structure and dynamics of water at the dimyristoylphosphatidylcholine lipid bilayer surface from a molecular dynamics simulation Lopez CF, Nielsen SO, Klein ML, Moore PB |
6611 - 6615 |
Geometrical picture of dynamical facilitation Whitelam S, Garrahan JP |
6616 - 6623 |
Molecular dynamics of excited state intramolecular proton transfer: 2-(2'-hydroxyphenyl)-4-methyloxazole in gas phase, solution, and protein environments Vendrell O, Moreno M, Lluch JM, Hammes-Schiffer S |
6624 - 6633 |
Dynamical arrest in superionic crystals and supercooled liquids Gray-Weale A, Madden PA |
6634 - 6642 |
The energy landscape of a fluorite-structured superionic conductor Gray-Weale A, Madden PA |
6643 - 6654 |
First-shell solvation of ion pairs: Correction of systematic errors in implicit solvent models Yu ZY, Jacobson MP, Josovitz J, Rapp CS, Friesner RA |
6655 - 6662 |
Dynamic heterogeneities in supercooled water Giovambattista N, Mazza MG, Buldyrev SV, Starr FW, Stanley HE |
6663 - 6666 |
Forces between two colloidal particles in a nematic solvent Al-Barwani MS, Sutcliffe GS, Allen MP |
6667 - 6672 |
Equilibrium time correlation functions from irreversible transformations in trajectory space Geissler PL, Dellago C |
6673 - 6686 |
The relaxation dynamics of a supercooled liquid confined by rough walls Scheidler P, Kob W, Binder K |
6687 - 6696 |
Liquid-state theory of structure, thermodynamics, and phase separation in suspensions of rod polymers and hard spheres Chen YL, Schweizer KS |
6697 - 6706 |
An integral equation approach to effective interactions between polymers in solution Krakoviack V, Rotenberg B, Hansen JP |
6707 - 6718 |
Free energy and structure of dislocation cores in two-dimensional crystals Bladon PB, Frenkel A |
6719 - 6722 |
Nonergodicity for a van der waals glass model Kawasaki K |
6723 - 6732 |
Electronic decoherence induced by intramolecular vibrational motions in a betaine dye molecule Hwang H, Rossky PJ |
6733 - 6744 |
Self-consistent field theory of polyelectrolyte systems Wang Q, Taniguchi T, Fredrickson GH |
6745 - 6749 |
Model study of coherent-control of the femtosecond primary event of vision Flores SC, Batista VS |
6750 - 6759 |
Fluid critical points from simulations: The Bruce-Wilding method and Yang-Yang anomalies Kim YC, Fisher ME |
6760 - 6766 |
A multigrid algorithm for sampling imaginary-time paths in quantum Monte Carlo simulations Mak CH |
6767 - 6771 |
Brownian motion of a rough sphere and the Stokes-Einstein Law Schmidt JR, Skinner JL |
6772 - 6777 |
Inherent-structure view of self-diffusion in liquids Shell MS, Debenedetti PG, Stillinger FH |
6778 - 6781 |
Micelle formation and the hydrophobic effect Maibaum L, Dinner AR, Chandler D |
6782 - 6795 |
A case study in the molecular interpretation of optical Kerr effect spectra: Instantaneous-normal-mode analysis of the OKE spectrum of liquid benzene Ryu S, Stratt RM |
6796 - 6808 |
East model: Basis set expansion, mode coupling, and irreducible memory kernels Wu JL, Cao JS |
6809 - 6815 |
Phase transitions of confined lattice homopolymers Hehmeyer OJ, Arya G, Panagiotopoulos AZ |
6816 - 6825 |
Phase space features and statistical aspects of forward-backward semiclassical dynamics Wright NJ, Makri N |
6826 - 6831 |
Importance of excluded volume on the solvation of urea in water Mountain RD, Thirumalai D |
6832 - 6837 |
Numerical investigation of the entropy crisis in model glass formers Brumer Y, Reichman DR |
6838 - 6843 |
Measuring the force ejecting DNA from phage Evilevitch A, Castelnovo M, Knobler CM, Gelbart WM |
6844 - 6849 |
Optimal allocation of replicas to processors in parallel tempering simulations Earl DJ, Deem MW |
6850 - 6855 |
Organization of coordination polyhedra in an amorphous binary alloy Fernandez JR, Harrowell P |
6856 - 6865 |
Instantaneous normal modes and cooperative dynamics in a quasi-two-dimensional system of particles Zangi R, Rice SA |
6866 - 6869 |
On the equivalence of atomic and molecular pressure Akkermans RLC, Ciccotti G |
6870 - 6876 |
Modified statistical treatment of kinetic energy in the Thomas-Fermi model Chai JD, Weeks JA |
6877 - 6882 |
Reformulation of Weeks-Chandler-Andersen perturbation theory directly in terms of a hard-sphere reference system Ben-Amotz D, Stell G |
6883 - 6892 |
Combining the semiclassical initial value representation with centroid dynamics Ka BJ, Voth GA |
6893 - 6900 |
Spontaneous relaxation in generalized oscillator models with glassy dynamics Ritort F |