4495 - 4497 |
Quantum calculations of the effect of bend excitation in methane on the HCl rotational distribution in the reaction CH4+Cl -> CH3+HCl Skokov S, Bowman JM |
4498 - 4500 |
Experimental evidence of polarization effects on exchangeable cations trapped in zeolites Giuntini JC, Maurin G, Devautour S, Henn F, Zanchetta JV |
4501 - 4504 |
Electric dipole polarizability of one excess-electron alkali-halide cluster Rayane D, Antoine R, Dugourd P, Broyer M |
4505 - 4514 |
Fast simulation of dynamic two-dimensional nuclear magnetic resonance spectra for systems with many spins or exchange sites Dumont RS, Assalone R |
4515 - 4523 |
On the classical limit for electronic structure and dynamics in the orbital approximation Remacle F, Levine RD |
4524 - 4532 |
A molecular based derivation of the nucleation theorem Bowles RK, McGraw R, Schaaf P, Senger B, Voegel JC, Reiss H |
4533 - 4548 |
An approximate short time Laplace transform inversion method Plimak L, Pollak E |
4549 - 4557 |
Brueckner based generalized coupled cluster theory: Implicit inclusion of higher excitation effects Nooijen M, Lotrich V |
4558 - 4564 |
Multidimensional reactive rate calculations in dissipative chaotic systems Hershkovitz E, Wiesenfeld L |
4565 - 4571 |
Rigorous solutions of diatomic molecule oscillator with empirical potential function in phase space Li QS, Lu J |
4572 - 4580 |
The direct production of CO(v=1-9) in the reaction of O(P-3) with the ethyl radical Reid JP, Marcy TP, Kuehn S, Leone SR |
4581 - 4587 |
The state-to-state predissociation dynamics of OC-HF upon HF stretch excitation Oudejans L, Miller RE |
4588 - 4597 |
Renner-Teller induced photodissociation of HCO in the first absorption band: Determination of linewidths for the (A)over-tilde(2)A '' K=0,1 states by filter-diagonalization Weiss J, Schinke R, Mandelshtam VA |
4598 - 4612 |
An accurate global ab initio potential energy surface for the X(1)A ' electronic state of HOBr Peterson KA |
4613 - 4619 |
Temperature effect on the deactivation of electronically excited potassium by hydrogen molecule Hsiao YC, Liu DK, Fung HS, Lin KC |
4620 - 4628 |
Theoretical simulations of the (HeBr2B)-Br-79, v=8 <- X, v ''=0 excitation spectrum: Spectroscopic manifestation of a linear isomer? Hernandez MI, Gonzalez-Lezana T, Delgado-Barrio G, Villarreal P, Buchachenko AA |
4629 - 4635 |
Anharmonic treatment of the lowest-energy conformers of glycine: A theoretical study Bludsky O, Chocholousova J, Vacek J, Huisken F, Hobza P |
4636 - 4646 |
Finite size effects and rotational relaxation in superfluid helium nanodroplets: Microwave-infrared double-resonance spectroscopy of cyanoacetylene Callegari C, Reinhard I, Lehmann KK, Scoles G, Nauta K, Miller RE |
4647 - 4653 |
Fragmentation of small sodium clusters Rytkonen A, Manninen M |
4654 - 4661 |
Electronic states of the copper, silver, and gold silicides and their ions Turski P, Barysz M |
4662 - 4667 |
Metastable states of negative carbon clusters: C-n(-), n=2-6 Naaman A, Bhushan KG, Pedersen HB, Altstein N, Heber O, Rappaport ML, Moalem R, Zajfman D |
4668 - 4673 |
The solvation of Na+ in water: First-principles simulations White JA, Schwegler E, Galli G, Gygi F |
4674 - 4682 |
Ultrafast Raman-induced Kerr-effect of water: Single molecule versus collective motions Winkler K, Lindner J, Bursing H, Vohringer P |
4683 - 4700 |
Temperature dependence of hydrophobic interactions: A mean force perspective, effects of water density, and nonadditivity of thermodynamic signatures Shimizu S, Chan HS |
4701 - 4706 |
Glass transition in chlorobenzene-decalin under pressure Koplinger J, Kasper G, Hunklinger S |
4707 - 4712 |
The best structural data of liquid ammonia based on the pair approximation: First-principles Monte Carlo simulation Hannongbua S |
4713 - 4721 |
The structure of deuterated methane-hydrate Gutt C, Asmussen B, Press W, Johnson MR, Handa YP, Tse JS |
4722 - 4731 |
Validating a polarizable model for the glass-forming liquid Ca0.4K0.6(NO3)(1.4) by ab initio calculations Ribeiro MCC, Almeida LCJ |
4732 - 4739 |
Molecular dynamics of a dense fluid of polydisperse hard spheres Sear RP |
4740 - 4750 |
Microscopic structure of Cl- coordination shell in NiCl2 methanol solution: A neutron diffraction study Adya AK, Kalugin ON |
4751 - 4762 |
X-ray scattering study and molecular simulation of glass forming liquids: Propylene carbonate and salol Eckstein E, Qian J, Hentschke R, Thurn-Albrecht T, Steffen W, Fischer EW |
4763 - 4766 |
Carbon rings and cages in the growth of single-walled carbon nanotubes Kiang CH |
4767 - 4773 |
Variance reduced Brownian simulation of a bead-spring chain under steady shear flow considering hydrodynamic interaction effects Kroger M, Alba-Perez A, Laso M, Ottinger HC |
4774 - 4784 |
Ligand-binding distributions in biopolymers Poland D |
4785 - 4793 |
Correlating the NMR self-diffusion and relaxation measurements with ionic conductivity in polymer electrolytes composed of cross-linked poly(ethylene oxide-propylene oxide) doped with LiN(SO2CF3)(2) Hayamizu K, Aihara Y, Price WS |
4794 - 4798 |
Correspondence of potentials of mean force in proteins and in liquids Shan YB, Zhou HX |
4799 - 4807 |
Effective interactions, structure, and isothermal compressibility of colloidal suspensions Dijkstra M, van Roij R, Evans R |
4808 - 4813 |
Hosted particle positions and dipole moments of protein-filled reverse micelles Chen PL, Tsao HK, Lu CYD |
4814 - 4826 |
Association behavior of binary polymer mixtures under elongational flow Dormidontova EE, ten Brinke G |
4827 - 4829 |
Designability of a protein chain in an off-lattice heteropolymer model Liang HJ |