3709 - 3712 |
Formation and growth of ice particles in stationary ultrasonic fields Bauerecker S, Neidhart B |
3713 - 3720 |
Implications of parity conservation for superpositions of chiral states Maierle CS, Harris RA |
3721 - 3729 |
Variational reaction path algorithm Fast PL, Truhlar DG |
3730 - 3741 |
Extracting accurate bound-state spectra from approximate wave packet propagation using the filter-diagonalization method Beck MH, Meyer HD |
3742 - 3759 |
A multitechnique maximum entropy approach to the determination of the orientation and conformation of flexible molecules in solution Berardi R, Spinozzi F, Zannoni C |
3760 - 3771 |
Why semilocal functionals work : Accuracy of the on-top pair density and importance of system averaging Burke K, Perdew JP, Ernzerhof M |
3772 - 3779 |
Product representation of potential energy surfaces. II Jackle A, Meyer HD |
3780 - 3791 |
Systematic design and evaluation of multiple-pulse experiments in nuclear magnetic resonance spectroscopy using a semi-continuous Baker-Campbell-Hausdorff expansion Hohwy M, Nielsen NC |
3792 - 3804 |
Hyperquantization algorithm. I. Theory for triatomic systems Aquilanti V, Cavalli S, De Fazio D |
3805 - 3818 |
Hyperquantization algorithm. II. Implementation for the F+H-2 reaction dynamics including open-shell and spin-orbit interactions Aquilanti V, Cavalli S, De Fazio D, Volpi A, Aguilar A, Gimenez X, Lucas JM |
3819 - 3823 |
The (2)Pi <- X (2)Pi electronic spectra of C8H and C10H in the gas phase Linnartz H, Motylewski T, Maier JP |
3824 - 3830 |
Highly predissociative levels of CH B (2)Sigma(-) state detected with two-color resonant four-wave mixing spectroscopy Kumar A, Hsiao CC, Hung WC, Lee YP |
3831 - 3840 |
Anomalously slow intramolecular vibrational redistribution in the acetylene (X)over-tilde (1)Sigma(+)(g) state above 10 000 cm(-)1 of internal energy Jacobson MP, O'Brien JP, Field RW |
3841 - 3849 |
Intramolecular interaction in the OH+-He and OH+-Ne open-shell ionic complexes : Infrared predissociation spectra of the nu(1) and nu(1)+nu(b) vibrations Roth D, Nizkorodov SA, Maier JP, Dopfer O |
3850 - 3855 |
Vibrational states in the electronic ground state of the OH+-He and OH+-Ne complexes Meuwly M, Maier JP, Rosmus P |
3856 - 3867 |
A comparative high-resolution study of predissociation linewidths in the Schumann-Runge bands of O-2 Dooley PM, Lewis BR, Gibson ST, Baldwin KGH, Cosby PC, Price JL, Copeland RA, Slanger TG, Thorne AP, Murray JE, Yoshino K |
3868 - 3874 |
A direct comparison of vibrational deactivation of hexafluorobenzene excited by infrared multiple photon absorption and internal conversion Gascooke JR, Alwahabi ZT, King KD, Lawrance WD |
3875 - 3881 |
Theoretical studies of the structures and vibrational frequencies of actinide compounds using relativistic effective core potentials with Hartree-Fock and density functional methods : UF6, NpF6, and PuF6 Hay PJ, Martin RL |
3882 - 3897 |
A combined experimental and theoretical study of rotational energy transfer in collisions between NO(X (2)Pi(1/2), v=3,J) and He, Ar and N-2 at temperatures down to 7 K James PL, Sims IR, Smith IWM, Alexander MH, Yang MB |
3898 - 3910 |
Scattering of aligned molecules. The potential energy surfaces for the Kr-O-2 and Xe-O-2 systems Aquilanti V, Ascenzi D, Cappelletti D, de Castro M, Pirani F |
3911 - 3918 |
The internal axis system of molecules with one large amplitude internal motion Szalay V, Ortigoso J |
3919 - 3927 |
Ab initio study of energy, structure and dynamics of the water-carbon dioxide complex Sadlej J, Makarewicz J, Chalasinski G |
3928 - 3934 |
Zero-order B-1(1)(n,O,O) vibrational levels of sulfur dioxide Hegazi E, Al-Adel F, Dastageer A, Hamdan A |
3935 - 3943 |
The chemistry of the superheavy elements. II. The stability of high oxidation states in group 11 elements : Relativistic coupled cluster calculations for the di-, tetra- and hexafluoro metallates of Cu, Ag, Au, and element 111 Seth M, Cooke F, Schwerdtfeger P, Heully JL, Pelissier M |
3944 - 3953 |
Mass-resolved two-photon and photoelectron spectra of Xe-2 in the Xe(4f) region above the first molecular ionization limit Hu XK, Mao DM, Shi YJ, Dimov SS, Lipson RH |
3954 - 3958 |
Transition energies of lanthanum, actinium, and eka-actinium (element 121) Ishikawa Y |
3959 - 3970 |
Electron and anion mobility in low density hydrogen cyanide gas. I. Dipole-bound electron ground states Klahn T, Krebs P |
3971 - 3982 |
Photodissociation dynamics of (C6H6)(3)(+) : Role of the extra benzene molecule weakly bound to the dimer core Ohashi K, Nishi N |
3983 - 3988 |
Resolving vibrational and structural contributions to isothermal compressibility Stillinger FH, Debenedetti PG, Sastry S |
3989 - 3993 |
Microscopic derivation of the Hubbard-Onsager-Zwanzig expression of limiting ionic conductivity Bagchi B |
3994 - 3998 |
Low-frequency Raman scattering of liquid CCl4, CHCl3, and acetone Amo Y, Tominaga Y |
3999 - 4008 |
Effect of an external electric field on diffusion-controlled bulk electron-ion recombination in high-mobility systems Wojcik M, Tachiya M |
4009 - 4014 |
Heat capacity anomaly near the critical point of aniline-cyclohexane Rebillot PF, Jacobs DT |
4015 - 4027 |
Vapor-liquid equilibria and heat effects of hydrogen fluoride from molecular simulation Visco DP, Kofke DA |
4028 - 4034 |
The generator coordinate method for a reaction coordinate coupled to a harmonic oscillator bath Cruz FFDS, Ruzzi M, Schmidt ACK |
4035 - 4046 |
Nuclear magnetic resonance-paramagnetic relaxation enhancements : Influence of spatial quantization of the electron spin when the zero-field splitting energy is larger than the Zeeman energy Abernathy SM, Miller JC, Lohr LL, Sharp RR |
4047 - 4051 |
Band-gap closure of H-2-He mixtures under pressure Chacham H, Reis SP, Koiller B |
4052 - 4062 |
Reaction of S-2 and H2S with Sn/Pt(111) surface alloys : Effects of metal-metal bonding on reactivity towards sulfur Rodriguez JA, Chaturvedi S, Jirsak T, Hrbek J |
4063 - 4070 |
Validity of Tolman's equation : How large should a droplet be? Koga K, Zeng XC, Shchekin AK |
4071 - 4077 |
The role of sticking and reaction probabilities in hot-atom mediated abstraction reactions of D on metal surfaces by gaseous H atoms Kammler T, Wehner S, Kuppers J |
4078 - 4089 |
Dynamic properties of dioctanoyl peroxide guest molecules constrained within the urea tunnel structure : A combined incoherent quasielastic neutron scattering and solid state H-2 nuclear magnetic resonance investigation Girard P, Aliev AE, Guillaume F, Harris KDM, Hollingsworth MD, Dianoux AJ, Jonsen P |
4090 - 4099 |
Dynamic nuclear polarization of diamond. I. Solid state and thermal mixing effects Reynhardt EC, High GL |
4100 - 4107 |
Dynamic nuclear polarization of diamond. II. Nuclear orientation via electron spin-locking Reynhardt EC, High GL |
4108 - 4118 |
Liquid-crystalline behavior of rod-coil diblock copolymers Matsen MW, Barrett C |
4119 - 4125 |
Linking rates of folding in lattice models of proteins with underlying thermodynamic characteristics Klimov DK, Thirumalai D |
4126 - 4127 |
Chemistry of PO-, PO2-, and PO3- in the gas phase Morris RA, Viggiano AA |
4128 - 4128 |
Harmonic inversion of time signals and its applications (vol 107, pg 6756, 1997) Mandelshtam VA, Taylor HS |
4129 - 4129 |
Electron and anion mobility in low density hydrogen cyanide gas. I. Dipole-bound electron ground states (vol 109, pg 531, 1998) Klahn T, Krebs P |