457 - 460 |
Analytic continuation for quantum nonadiabatic rate constants Golosov AA, Reichman DR, Rabani E |
461 - 470 |
Connections between second-order Gorling-Levy and many-body perturbation approaches in density functional theory Ivanov S, Hirata S, Grabowski I, Bartlett RJ |
471 - 486 |
Relativistic effects on the nuclear magnetic shielding tensor Melo JI, de Azua MCR, Giribet CG, Aucar GA, Romero RH |
487 - 496 |
Valence basis sets for relativistic energy-consistent small-core actinide pseudopotentials Cao XY, Dolg M, Stoll H |
497 - 504 |
Molecular motors driven by laser pulses: Role of molecular chirality and photon helicity Hoki K, Yamaki M, Koseki S, Fujimura Y |
505 - 513 |
Analytical time-dependent Hartree-Fock evaluation of the dynamic zero-point vibrationally averaged (ZPVA) first hyperpolarizability Quinet O, Kirtman B, Champagne B |
514 - 521 |
A discrete solvent reaction field model within density functional theory Jensen L, van Duijnen PT, Snijders JG |
522 - 536 |
Linear response at the 4-component relativistic level: Application to the frequency-dependent dipole polarizabilities of the coinage metal dimers Saue T, Jensen HJA |
537 - 549 |
Counterpoise-corrected geometries and harmonic frequencies of N-body clusters: Application to (HF)(n) (n=3,4) Salvador P, Szczesniak MM |
550 - 556 |
Electronic and photophysical properties of C60Cl24 Coheur PF, Lievin J, Colin R, Razbirin B |
557 - 564 |
A computational study of chlorofluoro-methyl radicals Schwartz M, Peebles LR, Berry RJ, Marshall P |
565 - 568 |
Quantum mechanical and quasi-classical trajectory study of the C(D-1)+H-2 reaction dynamics Banares L, Aoiz FJ, Honvault P, Bussery-Honvault B, Launay JM |
569 - 581 |
Quantum reactive scattering in three dimensions using adiabatically adjusting principal axis hyperspherical coordinates: Periodic distributed approximating functional method for surface functions Zhang KM, Parker GA, Kouri DJ, Hoffman DK, Iyengar SS |
582 - 594 |
Analytical fittings for the global potential energy surface of the ground state of methylene Yu JSK, Chen SY, Yu CH |
595 - 599 |
Control of vibrational ionization branching through feedback-optimized tailored femtosecond laser pulses Hertz E, Nersisyan G, Papadogiannis NA, Charalambidis D |
600 - 609 |
Photodissociation of the ArHBr complex investigated with the multiconfiguration time-dependent Hartree approach Trin J, Monnerville M, Pouilly B, Meyer HD |
610 - 621 |
Theoretical investigation of the temperature dependence of the O+O-2 exchange reaction Fleurat-Lessard P, Grebenshchikov SY, Siebert R, Schinke R, Halberstadt N |
622 - 632 |
CF A(2)Sigma(+)-X (2)Pi and B-2 Delta-X (2)Pi study by broadband absorption spectroscopy in a plasma etch reactor: Determination of transition probabilities, CF X-2 Pi concentrations, and gas temperatures Luque J, Hudson EA, Booth JP |
633 - 642 |
Kinetic and mechanistic studies on the abstraction reactions of atomic O (P-3) with (CH3)(2)SiH2 and (CH3)(3)SiH Zhang QZ, Gu YS, Wang SK |
643 - 658 |
Tunneling dynamics of the NH chromophore in NHD2 during and after coherent infrared excitation Marquardt R, Quack M, Thanopulos I, Luckhaus D |
659 - 668 |
Intramolecular vibrational energy redistribution, mode specificity, and nonexponential unimolecular decay dynamics of vibrationally highly excited states of DCO ((X)over-tilde(2)A') Renth F, Temps F, Trollsch A |
669 - 679 |
Rigorous calculation of electric field effects on the free energy change of the electron transfer reaction Seki K, Traytak SD, Tachiya M |
680 - 689 |
Physical limit of stability in supercooled D2O and D2O+H2O mixtures Kiselev SB, Ely JF |
690 - 705 |
Modeling velocity autocorrelation functions of confined fluids: A memory function approach Krishnan SH, Ayappa KG |
706 - 710 |
Density inhomogeneities and electron mobility in supercritical xenon Holroyd RA, Itoh K, Nishikawa M |
711 - 718 |
Basis set and electron correlation effects on ab initio electronic and vibrational nonlinear optical properties of conjugated organic molecules Torrent-Sucarrat M, Sola M, Duran M, Luis JM, Kirtman B |
719 - 727 |
Relaxation of the structure of simple metal ion complexes in aqueous solutions at up to supercritical conditions Mayanovic RA, Jayanetti S, Anderson AJ, Bassett WA, Chou IM |
728 - 735 |
Calculation of the melting point of NaCl by molecular simulation Anwar J, Frenkel D, Noro MG |
736 - 745 |
The role of total pressure in gas-phase nucleation: A diffusion effect Suh SM, Girshick SL, Zachariah MR |
746 - 759 |
Exciton exciton annihilation dynamics in chromophore complexes. I. Multiexciton density matrix formulation Bruggemann B, May V |
760 - 767 |
Molecular beam study of CH4 oxidation on a Pt(111)-(2x2)-O surface Kondo T, Sasaki T, Yamamoto S |
768 - 783 |
A kinetic theory of homogeneous bubble nucleation Shen VK, Debenedetti PG |
784 - 791 |
Polymer crystallization on pre-patterned substrates Dorenbos G, Sommer JU, Reiter G |
792 - 806 |
Homogeneous bubble nucleation in liquids: The classical theory revisited Delale CF, Hruby J, Marsik F |
807 - 815 |
Inherent structures of crystalline pentacene Della Valle RG, Venuti E, Brillante A, Girlando A |
816 - 829 |
Wetting of nanopatterned surfaces: The striped surface Schneemilch M, Quirke N, Henderson JR |
830 - 842 |
Application of the fundamental measure density functional theory to the adsorption in cylindrical pores Figueroa-Gerstenmaier S, Blas FJ, Avalos JB, Vega LF |
843 - 871 |
Microcanonical unimolecular rate theory at surfaces. I. Dissociative chemisorption of methane on Pt(111) Bukoski A, Blumling D, Harrison I |
872 - 877 |
Nucleation of pores in amphiphile bilayers Talanquer V, Oxtoby DW |
878 - 882 |
What causes the carbon nanotubes collapse in a chemical vapor deposition process Qian WZ, Wei F, Liu T, Wang ZW, Li YD |
883 - 891 |
Collapse transition for isolated square-well chain molecules: The exact density of states for short chains Taylor MP |
892 - 896 |
On the relation between the compressibility and the static structure factor of a fluid with a state-dependent pair-potential Tejero CF, Baus M |
897 - 904 |
Effect of curvature and twist on the conformations of a fluctuating ribbon Kessler DA, Rabin Y |
905 - 913 |
Thin films of asymmetric triblock copolymers: A Monte Carlo study Szamel G, Muller M |
914 - 924 |
Role of intramolecular energy on polyolefin miscibility: Isotactic polypropylene/polyethylene blends Heine D, Wu DT, Curro JG, Grest GS |
925 - 936 |
Brownian dynamics simulations of polymer stretching and transport in a complex electroosmotic flow Panwar AS, Kumar S |
937 - 951 |
Collapse or swelling dynamics of homopolymer rings: Self-consistent Hartree approach Rostiashvili VG, Lee NK, Vilgis TA |
952 - 958 |
Statistics, pathways and dynamics of single molecule protein folding Wang J |
959 - 968 |
First-passage time distribution and non-Markovian diffusion dynamics of protein folding Lee CL, Stell G, Wang J |
969 - 980 |
On the charge overcompensation of quenched polyelectrolyte stars electrostatically adsorbed onto a quenched oppositely charged planar surface Leermakers FAM, van den Oever JMP, Zhulina EB |
981 - 994 |
The fundamental photophysics of conjugated oligomer herringbone aggregates Spano FC |
995 - 995 |
Solid-fluid equilibrium in molecular models of n-alkanes (vol 110, pg 664, 1999) Malanoski AP, Monson PA |
996 - 996 |
Fluorescence dynamics of phenylene substituted polyphenylenevinylene-trinitrofluorenone blend systems (vol 117, pg 1395, 2002) Im C, Lupton JM, Schouwink P, Heun S, Becker H, Baessler H |