2481 - 2487 |
Massive thermostatting in isothermal density functional molecular dynamics simulations Windiks R, Delley B |
2488 - 2501 |
Quantum-classical approximation beyond Redfield theory Neufeld AA |
2502 - 2512 |
Molecular dynamics approach to vibrational energy relaxation: Quantum-classical versus purely classical nonequilibrium simulations Neufeld AA, Schwarzer D, Schroeder J, Troe J |
2513 - 2522 |
Thermal electron emission from the hot electronic subsystem of vibrationally cold C-60 Hansen K, Hoffmann K, Campbell EEB |
2523 - 2530 |
Conformations of indan and 2-indanol: A combined study by UV laser spectroscopy and quantum chemistry calculation Das A, Mahato KK, Panja SS, Chakraborty T |
2531 - 2537 |
The interaction of oxygen with small gold clusters Varganov SA, Olson RM, Gordon MS, Metiu H |
2538 - 2544 |
Crossed-beam scattering of F+CD4 -> DF+CD3(nu NK): The integral cross sections Zhou JG, Lin JJ, Shiu WC, Pu SC, Liu KP |
2545 - 2556 |
Ab initio derived analytical fits of the two lowest triplet potential energy surfaces and theoretical rate constants for the N(S-4) plus NO(X (2)Pi) system Gamallo P, Gonzalez M, Sayos R |
2557 - 2568 |
Laser-induced fluorescence, electronic absorption, infrared and Raman spectra, and ab initio calculations of 1,2-dihydronaphthalene: Investigation of the out-of-plane ring modes for the ground and S-1(pi,pi(*)) excited states Autrey D, Arp Z, Choo J, Laane J |
2569 - 2576 |
Instantaneous nonvertical electronic transitions with shaped femtosecond laser pulses: Is it possible? Henriksen NE, Moller KB |
2577 - 2589 |
Formation of ozone: Metastable states and anomalous isotope effect Babikov D, Kendrick BK, Walker RB, Pack RT, Fleurat-Lesard P, Schinke R |
2590 - 2595 |
First determination of the NO2 (A)over-tilde B-2(2) stretching frequencies by jet cooled intracavity laser absorption spectroscopy around 11,000 cm(-1) Jost R, Vergniory MG, Campargue A |
2596 - 2613 |
A realistic multi-sheeted potential energy surface for NO2((2)A') from the double many-body expansion method and a novel multiple energy-switching scheme Varandas AJC |
2614 - 2617 |
Fluorescence spectra of NH2 (X)over-tilde B-2(1)<-(A)over-tilde (2)A(1) Sigma bands: Experiment and theory Petrongolo C, Fan HY, Ionescu I, Kuffel D, Reid SA |
2618 - 2622 |
Examination of the correlation energy and second virial coefficients from accurate ab initio calculations of rare-gas dimers Giese TJ, Audette VM, York DM |
2623 - 2637 |
Perturbational ab initio calculations of relativistic contributions to nuclear magnetic resonance shielding tensors Manninen P, Lantto P, Vaara J, Ruud K |
2638 - 2657 |
Integral equation theories for orientionally ordered fluids Paci I, Cann NM |
2658 - 2662 |
Condensed-phase effects on absolute cross sections for dissociative electron attachment to CFCs and HCFCs adsorbed on Kr Lu QB, Sanche L |
2663 - 2668 |
Selectively observing the amplitude modulation under magic angle sample spinning Liu Y, Leu G, Singer S, Sen PN, Cory DG |
2669 - 2679 |
Electronic transport in disordered n-alkanes: From fluid methane to amorphous polyethylene Cubero D, Quirke N, Coker DF |
2680 - 2684 |
Experimental and theoretical characterization of a C2H2O2+ cation in solid argon Dong J, Miao L, Zhou MF |
2685 - 2690 |
Nuclear magnetic shielding and chirality. I. The shielding tensor of Xe interacting with Ne helices Sears DN, Jameson CJ, Harris RA |
2691 - 2693 |
Nuclear magnetic shielding and chirality. II. The shielding tensor of a naked spin in Ne helices Sears DN, Jameson CJ, Harris RA |
2694 - 2701 |
Nuclear magnetic shielding and chirality. III. The single electron on a helix model Sears DN, Jameson CJ, Harris RA |
2702 - 2708 |
Absolute hydration free energies of ions, ion-water clusters, and quasichemical theory Asthagiri D, Pratt LR, Ashbaugh HS |
2709 - 2715 |
Two-dimensional vibrational spectroscopy of the amide I band of crystalline acetanilide: Fermi resonance, conformational substates, or vibrational self-trapping? Edler J, Hamm P |
2716 - 2719 |
Equation of state for hard-spheres Miandehy M, Modarress H |
2720 - 2731 |
Phase diagrams classification of the systems with thermoreversible alternating association (the Flory approach) Thamm MV, Erukhimovich IY |
2732 - 2737 |
Spatial correlation in a Lotka-Volterra reaction diffusion mechanism Hansen JS, Toxvaerd S, Praestgaard EL |
2738 - 2746 |
Conformational distribution functions extracted from residual dipolar couplings: A hybrid model based on maximum entropy and molecular field theory Stevensson B, Sandstrom D, Maliniak A |
2747 - 2752 |
Intermolecular Fermi resonance Stride JA, Dallin PH, Jayasooriya UA |
2753 - 2760 |
Theoretical study of electronic and solvent reorganization associated with a charging process of organic compounds. I. Molecular and atomic level description of solvent reorganization Sato H, Kobori Y, Tero-Kubota S, Hirata F |
2761 - 2773 |
Modeling of ultrafast electron-transfer processes: Validity of multilevel Redfield theory Egorova D, Thoss M, Domcke W, Wang HB |
2774 - 2779 |
Temperature-programmed time of flight secondary ion mass spectrometry study of hydration of ammonia and formic acid adsorbed on the water-ice surface Souda R |
2780 - 2791 |
Kramers' turnover theory for diffusion of Na atoms on a Cu(001) surface measured by He scattering Guantes R, Vega JL, Miret-Artes S, Pollak E |
2792 - 2800 |
Molecular dynamics simulations of crystallization under confinement at triple point conditions Camara LG, Bresme F |
2801 - 2811 |
Knudsen self- and Fickian diffusion in rough nanoporous media Malek K, Coppens MO |
2812 - 2819 |
Dielectric permittivity and electric modulus in Bi2Ti4O11 Liu JJ, Duan CG, Yin WG, Mei WN, Smith RW, Hardy JR |
2820 - 2824 |
Adsorption structure of acetylene on Ge(001): A first-principles study Cho JH, Kleinman L |
2825 - 2839 |
Constant-number Monte Carlo simulation of aggregating and fragmenting particles Friesen WI, Dabros T |
2840 - 2848 |
Li ion transport in an intercalated polymer electrolyte Arun N, Vasudevan S, Ramanathan KV |
2849 - 2853 |
Dynamics of Li ions in an intercalated polymer electrolyte: A Li-7 nuclear magnetic resonance study Arun N, Vasudevan S, Ramanathan KV |
2854 - 2873 |
Eigenstates and transmission coefficients of finite-sized carbon nanotubes Compernolle S, Chibotaru L, Ceulemans A |
2874 - 2885 |
Self-assembled aggregates in the gravitational field: Growth and nematic order Baulin VA |
2886 - 2891 |
Conformation-assisted fluctuation of density and kinetics of nucleation in polymer melts Tan HG, Miao B, Yan DD |
2892 - 2902 |
Two-chamber lattice model for thermodiffusion in polymer solutions Luettmer-Strathmann J |
2903 - 2907 |
Towards an anisotropic bead-spring model for ribbonlike polymers: Monte Carlo simulations of liquid benzene Lorenz S, Walsh TR, Sutton AP |
2908 - 2914 |
The configurational phase transitions of flexible polymers in planar mixed flows near simple shear Woo NJ, Shaqfeh ESG |
2915 - 2922 |
Simulation of dense amorphous polymers by generating representative atomistic models Curco D, Aleman C |
2923 - 2934 |
Conformational dynamics of phenylene rings in poly(p-phenylene vinylene) as revealed by C-13 magic-angle-spinning exchange nuclear magnetic resonance experiments deAzevedo ER, Franco RWA, Marletta A, Faria RM, Bonagamba TJ |
2935 - 2937 |
Water's T-g-endotherm, sub-T-g peak of glasses and T-g of water Johari GP |