789 - 791 |
Correlation effect in spectral line shape from the Doppler to the collision regime Lance B, Robert D |
792 - 795 |
Wavelength-resolved stimulated photon echoes: Direct observation of ultrafast intramolecular vibrational contributions to electronic dephasing Book LD, Scherer NF |
796 - 803 |
Nonequilibrium distribution function formalism for diffusion-influenced bimolecular reactions: Beyond the superposition approximation Sung J, Lee S |
804 - 815 |
Nonequilibrium distribution function theory of diffusion-influenced reversible energy-transfer reactions Sung JY, Chi JH, Lee S |
816 - 826 |
Learning to interpolate molecular potential energy surfaces with confidence: A Bayesian approach Bettens RPA, Collins MA |
827 - 832 |
Size-extensive calculations of static structure factors from the coupled cluster singles and doubles model Watanabe N, Ten-no S, Pal S, Iwata S, Udagawa Y |
833 - 841 |
A formal method for solving the stationary BBGKY hierarchy for a classical inhomogeneous fluid Paine GH |
842 - 848 |
Calculation of frequency-dependent second hyperpolarizabilities for electric field induced second harmonic generation in the second-order Moller-Plesset perturbation theory Kobayashi T, Sasagane K, Aiga F, Yamaguchi K |
849 - 858 |
Comparison of methods for calculating the properties of intramolecular hydrogen bonds. Excited state proton transfer Kar T, Scheiner S, Cuma M |
859 - 874 |
Geometric investigation of low-dimensional manifolds in systems approaching equilibrium Davis MJ, Skodje RT |
875 - 884 |
Finite field treatment of vibrational polarizabilities and hyperpolarizabilities: On the role of the Eckart conditions, their implementation, and their use in characterizing key vibrations Luis JM, Duran M, Andres JL, Champagne B, Kirtman B |
885 - 892 |
Accurate dipole moments from Hartree-Fock calculations by means of class IV charges Li JB, Xing JH, Cramer CJ, Truhlar DG |
893 - 910 |
Total energy partitioning within a one-electron formalism: A Hamilton population study of surface-CO interaction in the c(2 x 2)-CO/Ni(100) chemisorption system Glassey WV, Papoian GA, Hoffmann R |
911 - 915 |
Kinetic energy density dependent approximations to the exchange energy Ernzerhof M, Scuseria GE |
916 - 922 |
Transition probability due to a conical intersection: On the role of the initial conditions and of the geometric setup of the crossing surfaces Ferretti A, Lami A, Villani G |
923 - 930 |
The photodissociation of carbonyl cyanide CO(CN)(2) at 193 nm studied by photofragment translational energy spectroscopy Scheld HA, Furlan A, Huber JR |
931 - 937 |
Laser excitation and photoionization spectroscopy of the AO(+) and B1 states of indium monoiodide: Ground state dissociation energy and photodissociation yield of In(6s S-2(1/2)) King KK, Herring CM, Eden JG |
938 - 949 |
Competitive fragmentation and electron loss kinetics of photoactivated silver cluster anions: Dissociation energies of Ag-n(-) (n=7-11) Shi Y, Spasov VA, Ervin KM |
950 - 958 |
The electronic spectrum, molecular structure, and oscillatory fluorescence decay of jet-cooled germylidene (H2C = Ge-74), the simplest unsaturated germylene Hostutler DA, Smith TC, Li HY, Clouthier DJ |
959 - 968 |
The decay dynamics of photoexcited rare gas cluster ions Jones AB, Jukes PR, Stace AJ |
969 - 972 |
Thermodynamic investigation of the AlNC and AlCN isomers by Knudsen cell mass spectrometry Meloni G, Gingerich KA |
973 - 980 |
The He-LiH potential energy surface revisited. I. An interpolated rigid rotor surface Taylor BK, Hinde RJ |
981 - 987 |
Spectroscopic characterization of excited Ca(4s4d delta D-3(J))RG((3)Delta(1,2)) states (RG=Ar, Kr, Xe): No "heavy-atom" mixing of RG(nd delta) character into the wave functions Leung AWK, Kaup JG, Bellert D, McCaffrey JG, Breckenridge WH |
988 - 996 |
Quantum mechanical study on energy dependence of probabilities of nonreactive vibrational transitions, atom exchange reaction, and dissociation in a collinear He+H-2(+) collision Onda K, Sakimoto K |
997 - 1007 |
A three-dimensional potential energy surface for He+Cl-2 (B (3)Pi(0u+)): Ab initio calculations and a multiproperty fit Williams J, Rohrbacher A, Seong J, Marianayagam N, Janda KC, Burcl R, Szczesniak MM, Chalasinski G, Cybulski SM, Halberstadt N |
1008 - 1016 |
The vibrational energy pattern in acetylene. V. (C2H2)-C-13 Di Lonardo G, Fusina L, Venuti E, Johns JWC, El Idrissi MI, Lievin J, Herman M |
1017 - 1021 |
The relaxation from linear to triangular Ag-3 probed by femtosecond resonant two-photon ionization Leisner T, Vajda S, Wolf S, Woste L, Berry RS |
1022 - 1034 |
Measurement of the HD(v '=2,J '=3) product differential cross section for the H+D-2 exchange reaction at 1.55 +/- 0.05 eV using the photoloc technique Fernandez-Alonso F, Bean BD, Zare RN |
1035 - 1042 |
Differential cross sections for H+D-2 -> HD(v(')=1, J(')=1,5,8)+D at 1.7 eV Fernandez-Alonso F, Bean BD, Zare RN |
1043 - 1048 |
A comment on dielectric hole burning Wagner A, Kliem H |
1049 - 1059 |
A simple model of tracer-diffusion of nonspherical Brownian particles Guevara-Rodriguez FD, Medina-Noyola M |
1060 - 1067 |
Intermediate-time tracer-diffusion of nonspherical Brownian particles Guevara-Rodriguez FD, Medina-Noyola M |
1068 - 1075 |
Dynamic correlation effect in reversible diffusion-influenced reactions: Brownian dynamics simulation in three dimensions Kim H, Yang M, Shin KJ |
1076 - 1095 |
A first-principle computation of the thermodynamics of glasses Mezard M, Parisi G |
1096 - 1103 |
Simulation studies of liquid ammonia by classical ab initio, classical, and path-integral molecular dynamics Diraison M, Martyna GJ, Tuckerman ME |
1104 - 1108 |
Identifying physical clusters in bubble nucleation Kusaka I, Oxtoby DW |
1109 - 1116 |
A primitive model of a charged hard ellipsoidal fluid Rickayzen G |
1117 - 1125 |
Molecular dynamics simulation of formamide in water using density functional theory and classical potentials Chalmet S, Ruiz-Lopez MF |
1126 - 1136 |
Revisiting angular jump models of molecular reorientations in viscous liquids Diezemann G, Sillescu H |
1137 - 1157 |
Multidimensional solvation dynamical effects on quantum yields in model triad systems Okada A, Bandyopadhyay T |
1158 - 1168 |
Ultraviolet-laser induced desorption of NO from the Cr2O3(0001) surface: Involvement of a precursor state? Wilde M, Seiferth O, Al-Shamery K, Freund HJ |
1169 - 1174 |
Adsorption of fluoroform CHF3 on ice Ih(0001): Structure and vibrations Graham AP, Menzel A, Toennies JP |
1175 - 1184 |
Molecular processes of adsorption and desorption of alkanethiol monolayers on Au(111) Kondoh H, Kodama C, Sumida H, Nozoye H |
1185 - 1190 |
Femtosecond probing of exciton relaxation and transport dynamics in polybithiophene Bock AM, Schmid D, Kryschi C |
1191 - 1194 |
Energy transfer with migration. Generalization of the Yokota-Tanimoto model for any kind of multipole interaction Martin IR, Rodriguez VD, Rodriguez-Mendoza UR, Lavin V, Montoya E, Jaque D |
1195 - 1208 |
Discrete dipole approximation for ultraviolet-visible extinction spectra simulation of silver and gold colloids Felidj N, Aubard J, Levi G |
1209 - 1222 |
Diffusion mechanisms of normal alkanes in faujasite zeolites Clark LA, Ye GT, Gupta A, Hall LL, Snurr RQ |
1223 - 1230 |
Molecular dynamics simulations of simple dipolar liquids in spherical cavity: Effects of confinement on structural, dielectric, and dynamical properties Senapati S, Chandra A |
1231 - 1239 |
Motion of interlamellar hydrated sodium ions in layered Cd0.75PS3Na0.5(H2O)(2) Arun N, Jeevanandam P, Vasudevan S, Ramanathan KV |
1240 - 1254 |
Monolayer adsorption of nonrandom mixtures Hocker T, Aranovich GL, Donohue MD |
1255 - 1264 |
Electron dynamics in gold and gold-silver alloy nanoparticles: The influence of a nonequilibrium electron distribution and the size dependence of the electron-phonon relaxation Link S, Burda C, Wang ZL, El-Sayed MA |
1265 - 1272 |
Effect of the transient mobility in two-dimensional continuum deposition Belardinelli RE, Linares DH, Pereyra VD |
1273 - 1280 |
Molecular dynamics simulation of the rheological and dynamical properties of a model alkane fluid under confinement Cui ST, Cummings PT, Cochran HD |
1281 - 1287 |
Constant surface tension simulations of lipid bilayers: The sensitivity of surface areas and compressibilities Feller SE, Pastor RW |
1288 - 1292 |
A high resolution electron energy loss spectroscopy study of the Fermi resonance of CO2 adsorbed on a Ag(110)/CO3 layer Krenzer B, Constant L, Conrad H |
1293 - 1301 |
Vapor-liquid equilibria of vibrating square well chains Hu LG, Rangwalla H, Cui JY, Elliott JR |
1302 - 1308 |
Conformational properties of polymer chains in the theta region Rubio AM, Freire JJ, Yong CW, Clarke JHR |
1309 - 1324 |
Density functional study of intramolecular ferromagnetic interaction through m-phenylene coupling unit. III. Possibility of high-spin polymer Mitani M, Takano Y, Yoshioka Y, Yamaguchi K |
1325 - 1334 |
Molecular dynamics simulations of dielectric relaxation of concentrated polymer solutions Kaznessis YN, Hill DA, Maginn EJ |
1335 - 1336 |
Tunneling manifold of two noninteracting NH4 torsional oscillators in polycrystalline ammonium iodide Choi C, Peternelj J, Damyanovich A, Pintar MM |
1337 - 1338 |
Thermochemistry of ZnCl(g) Hildenbrand DL, Lau KH, Roos JW |
1339 - 1339 |
Finite-size scaling of helix-coil transitions in poly-alanine studied by multicanonical simulations (vol 110, pg 1267, 1999) Hansmann UHE, Okamoto Y |
1340 - 1340 |
Comparison of thermal and photochemical behavior of O-2 chemisorbed on Pt(335) (vol 110, pg 6939, 1999) Heyd DV, Scharff RJ, Yates JT |