10355 - 10358 |
Spin-orbit coupling in O-2(v)+O-2 collisions: A new energy transfer mechanism Dayou F, Campos-Martinez J, Hernandez MI, Hernandez-Lamoneda R |
10359 - 10363 |
Basis set effects on frontier molecular orbital energies and energy gaps: A comparative study between plane waves and localized basis functions in molecular systems Matus MH, Garza J, Galvan M |
10364 - 10367 |
Size versus volume extensivity of a new class of density matrix functionals Cioslowski J, Pernal K |
10368 - 10378 |
Atomic dipole moments calculated using analytical molecular second-moment gradients Solheim H, Ruud K, Astrand PO |
10379 - 10384 |
An exact reformulation of the diagonalization step in electronic structure calculations as a set of second order nonlinear equations Liang WZ, Head-Gordon M |
10385 - 10394 |
Geminal model chemistry II. Perturbative corrections Rassolov VA, Xu F, Garashchuk S |
10395 - 10403 |
The effect of spin-orbit coupling on fast neutral chemical reaction O(P-3)+CH3 -> CH3O Yagi K, Takayanagi T, Taketsugu T, Hirao K |
10404 - 10413 |
A systematic ab initio study of the equilibrium geometry and vibrational wave numbers of bismuthine Breidung J, Thiel W, Figgen D, Stoll H |
10414 - 10422 |
Geometry and electronic structure of V-n(Bz)(m) complexes Kandalam AK, Rao BK, Jena P, Pandey R |
10423 - 10425 |
Diffusion quantum Monte Carlo for equilibrium structures and harmonic frequencies of ethane and ozone molecules Lu SI |
10426 - 10441 |
Near-infrared spectra and rovibrational dynamics on a four-dimensional ab initio potential energy surface of (HBr)(2) Castillo-Chara J, McIntosh AL, Wang Z, Lucchese RR, Bevan JW |
10442 - 10449 |
Fractional revivals in the rovibrational motion of I-2 Lohmuller T, Engel V, Beswick JA, Meier C |
10450 - 10454 |
Electric dipole polarizabilities of copper clusters Knickelbein MB |
10455 - 10469 |
Postnucleation droplet growth in supersaturated gas with arbitrary vapor concentration Pines V, Zlatkowski M, Chait A |
10470 - 10482 |
Isomer-selective detection of microsolvated oxonium and carbenium ions of protonated phenol: Infrared spectra of C6H7O+-L-n clusters (L=Ar/N-2, n <= 6) Solca N, Dopfer O |
10483 - 10500 |
Calculation of the rate constant for state-selected recombination of H+O-2(v) as a function of temperature and pressure Teitelbaum H, Caridade PJSB, Varandas AJC |
10501 - 10512 |
Spectroscopic properties of novel aromatic metal clusters: NaM4 (M=Al,Ga,In) and their cations and anions Zhao CY, Balasubramanian K |
10513 - 10519 |
Mass-analyzed threshold ionization spectroscopy of p-methylphenol and p-ethylphenol cations and the alkyl substitution effect Lin JL, Li CY, Tzeng WB |
10520 - 10529 |
Broadening and line mixing in the 20 (0)0 <- 01 (1)0, 11 (1)0 <- 00 (0)0 and 12 (2)0 <- 01 (1)0 Q branches of carbon dioxide: Experimental results and energy-corrected sudden modeling Predoi-Cross A, May AD, Vitcu A, Drummond JR, Hartmann JM, Boulet C |
10530 - 10542 |
Rotational state-dependent mixings between resonance states of vibrationally highly excited DCO ((X)over-tilde (2)A') Wei J, Trollsch A, Tesch C, Temps F |
10543 - 10553 |
Relative vibrational overtone intensity of cis-cis and trans-perp peroxynitrous acid Matthews J, Sinha A, Francisco JS |
10554 - 10560 |
Polar isomer of formic acid dimers formed in helium nanodroplets Madeja F, Havenith M, Nauta K, Miller RE, Chocholousova J, Hobza P |
10561 - 10578 |
Confirmation of the "long-lived" tetra-nitrogen (N-4) molecule using neutralization-reionization mass spectrometry and ab initio calculations Rennie EE, Mayer PM |
10579 - 10593 |
Jet-cooled laser spectroscopy of the cyclohexoxy radical Zu L, Liu JJ, Tarczay G, Dupre P, Miller TA |
10594 - 10604 |
Analysis of the vibronic fine structure in circularly polarized emission spectra from chiral molecular aggregates Spano FC, Zhao Z, Meskers SCJ |
10605 - 10617 |
Heat capacity effects associated with the hydrophobic hydration and interaction of simple solutes: A detailed structural and energetical analysis based on molecular dynamics simulations Paschek D |
10618 - 10623 |
Polymerization of nitrogen in sodium azide Eremets MI, Popov MY, Trojan IA, Denisov VN, Boehler R, Hemley RJ |
10624 - 10633 |
Centroid molecular dynamics approach to the transport properties of liquid para-hydrogen over the wide temperature range Yonetani Y, Kinugawa K |
10634 - 10639 |
Density functional theory of fluids in the isothermal-isobaric ensemble Gonzalez A, White JA, Roman FL, Velasco S |
10640 - 10646 |
Adam-Gibbs model for the supercooled dynamics in the ortho-terphenyl ortho-phenylphenol mixture Roland CM, Capaccioli S, Lucchesi M, Casalini R |
10647 - 10658 |
A semiclassical generalized quantum master equation for an arbitrary system-bath coupling Shi Q, Geva E |
10659 - 10665 |
Intermolecular double-quantum coherences in two-dimensional spectra of binary mixtures in solution. The role of diffusion Engelsberg M, Barros W, Hallwass F |
10666 - 10680 |
Landscapes and fragilities Ruocco G, Sciortino F, Zamponi F, De Michele C, Scopigno T |
10681 - 10690 |
Computer simulation study of the closure relations in hard sphere fluids Fantoni R, Pastore G |
10691 - 10698 |
A vibrational spectroscopic study of structure evolution of water dissolved in supercritical carbon dioxide under isobaric heating Oparin R, Tassaing T, Danten Y, Besnard M |
10699 - 10710 |
Bridging continuum and statistical thermodynamics via equations of state and the density of states Gospodinov ID, Escobedo FA |
10711 - 10727 |
Thermodynamic forces in highly curved fluid interfaces Lovett R, Baus M |
10728 - 10735 |
Density inhomogeneity and diffusion behavior of fluids in micropores by molecular-dynamics simulation Liu YC, Wang Q, Lu LH |
10736 - 10747 |
New theory of equation of state for surface monolayer Rusanov AI |
10748 - 10752 |
Wavelength dependence of the hyper Rayleigh scattering response from gold nanoparticles Russier-Antoine I, Jonin C, Nappa J, Benichou E, Brevet PF |
10753 - 10762 |
Simulation study of angle-resolved photoemission spectra and intramolecular energy-band dispersion of a poly(tetrafluoroethylene) oligomer film Yoshimura D, Ishii H, Ouchi Y, Miyamae T, Hasegawa S, Okudaira KK, Ueno N, Seki K |
10763 - 10767 |
Coarse-grained nonequilibrium approach to the molecular modeling of permeation through microporous membranes Tunca C, Ford DM |
10768 - 10779 |
Hamiltonian theory for vibrational line shapes of atoms adsorbed on surfaces Guantes R, Vega JL, Miret-Artes S, Pollak E |
10780 - 10785 |
Application of the exact exchange potential method for half metallic intermediate band alloy semiconductor Fernandez JJ, Tablero C, Wahnon P |
10786 - 10791 |
Imaging water on Ag(111): Field induced reorientation and contrast inversion Morgenstern K, Nieminen J |
10792 - 10798 |
Dipole-induced structure in aromatic-terminated self-assembled monolayers - A study by near edge x-ray absorption fine structure spectroscopy Luk YY, Abbott NL, Crain JN, Himpsel FJ |
10799 - 10806 |
Trends in the band structures of the group-I and -II oxides Mikajlo EA, Dorsett HE, Ford MJ |
10807 - 10814 |
Optical properties of passivated silicon nanoclusters: The role of synthesis Draeger EW, Grossman JC, Williamson AJ, Galli G |
10815 - 10827 |
Density-induced coupling effects on the dispersivity of a flexible chain particle Van Dyke M, Haber S |
10828 - 10836 |
Orientational and interaction induced dynamics in the isotropic phase of a liquid crystal: Polarization resolved ultrafast optical Kerr effect spectroscopy Hunt NT, Meech SR |
10837 - 10847 |
Prediction of membrane protein structures by replica-exchange Monte Carlo simulations: Case of two helices Kokubo H, Okamoto Y |
10848 - 10851 |
Nematic ordering in dilute solutions of rodlike polyelectrolytes Potemkin II, Khokhlov AR |
10852 - 10852 |
On the acceptance probability of replica-exchange Monte Carlo trials (vol 117, pg 6911, 2002) Kofke DA |
10853 - 10853 |
Investigating bonding in small silicon-carbon clusters: Exploration of the potential energy surfaces of Si3C4, Si4C3, and Si4C4 using ab initio molecular dynamics (vol 120, pg 4333, 2004) Bertolus M, Finocchi F, Millie P |