1063 - 1065 |
A diffusion Monte Carlo accurate interaction potential between H and PsH Mella M, Morosi G, Bressanini D |
1066 - 1069 |
Ab initio calculation of the zero-field splitting parameter D of benzene and naphthalene Bomfleur B, Sironi M, Raimondi M, Voitlander J |
1070 - 1081 |
Rovibrational Hamiltonians for general polyatomic molecules in spherical polar parametrization. I. Orthogonal representations Mladenovic M |
1082 - 1095 |
Rovibrational Hamiltonians for general polyatomic molecules in spherical polar parametrization. II. Nonorthogonal descriptions of internal molecular geometry Mladenovic M |
1096 - 1106 |
Quantized field description of rotor frequency-driven dipolar recoupling Boender GJ, Vega S, de Groot HJM |
1107 - 1112 |
On the divergent behavior of Moller-Plesset perturbation theory for the molecular electric dipole moment Larsen H, Halkier A, Olsen J, Jorgensen P |
1113 - 1121 |
Radial moments of the electron density: Gas phase results and the effects of solvation Worsnop SK, Boyd RJ, Elorza JM, Sarasola C, Ugalde JM |
1122 - 1124 |
Mapping of simulated localized fluctuations onto a macrosystem: Direct counting in the macrosystem to confirm statistical mechanical theory Bowles RK |
1125 - 1132 |
Gaussian-3 theory using scaled energies Curtiss LA, Raghavachari K, Redfern PC, Pople JA |
1133 - 1149 |
Molecular properties from combined QM/MM methods. I. Analytical second derivative and vibrational calculations Cui Q, Karplus M |
1150 - 1157 |
The Hartree product and the description of local and global quantities in atomic systems: A study within Kohn-Sham theory Garza J, Nichols JA, Dixon DA |
1158 - 1169 |
Vibronic structure of alkoxy radicals via photoelectron spectroscopy Ramond TM, Davico GE, Schwartz RL, Lineberger WC |
1170 - 1177 |
van der Waals isomers and ionic reactivity of the cluster system para-chlorofluorobenzene/methanol Riehn C, Buchhold K, Reimann B, Djafari S, Barth HD, Brutschy B, Tarakeshwar P, Kim KS |
1178 - 1191 |
Ab initio study of the gas-phase structure and electronic properties of M-CH3 (M=Li, Na) and M-CCH (M=Li, Na, K): A combined post-Hartree-Fock and density functional theory study Scalmani G, Bredas JL, Barone V |
1192 - 1203 |
Water-chain clusters: Vibronic spectra of 7-hydroxyquinoline center dot(H2O)(2) Bach A, Coussan S, Muller A, Leutwyler S |
1204 - 1211 |
Theoretical characterization of the excited-state structures and properties of phenol and its one-water complex Fang WH |
1212 - 1220 |
Six-dimensional calculation of the vibrational spectrum of the HFCO molecule Viel A, Leforestier C |
1221 - 1228 |
Statistical thermodynamics of bond torsional modes Chuang YY, Truhlar DG |
1229 - 1239 |
Molecular dichotomy within an intense high-frequency laser field Nguyen NA, Nguyen-Dang TT |
1240 - 1254 |
Global potential energy surfaces for the H-3(+) system. Analytical representation of the adiabatic ground-state 1 (1)A ' potential Aguado A, Roncero O, Tablero C, Sanz C, Paniagua M |
1255 - 1259 |
Time-dependent quantum mechanical study of photodissociation of molecular oxygen in the Schumann-Runge continuum Balakrishnan N, Jamieson MJ, Dalgarno A, Li Y, Buenker RJ |
1260 - 1270 |
The diffraction signatures of individual vibrational modes in polyatomic molecules Ryu S, Weber PM, Stratt RM |
1271 - 1278 |
Rotationally resolved pulsed-field ionization photoelectron bands for O-2(+)(A (2)Pi(u),v(+)=0-12) in the energy range of 17.0-18.2 eV Song Y, Evans M, Ng CY, Hsu CW, Jarvis GK |
1279 - 1286 |
The vibrational distribution of O-2(X (3)Sigma(-)(g)) produced in the photodissociation of ozone between 226 and 240 and at 266 nm Geiser JD, Dylewski SM, Mueller JA, Wilson RJ, Toumi R, Houston PL |
1287 - 1294 |
Rotational patches: Stark effect, dipole moment, and dynamics of water loosely bound to benzene Emilsson T, Gutowsky HS, de Oliveira G, Dykstra CE |
1295 - 1305 |
Structure and energetics of SinNm clusters: Growth pathways in a heterogenous cluster system Jungnickel G, Frauenheim T, Jackson KA |
1306 - 1315 |
Rotationally resolved pulsed field ionization photoelectron bands for O-2(+)(a (4)Pi(u), v(+)=0-18) in the energy range of 16.0-18.0 eV Song Y, Evans M, Ng CY, Hsu CW, Jarvis GK |
1316 - 1320 |
The strong field photoelectron spectroscopy of acetylene: Evidence for short-lived 4p gerade states via electric field-induced resonance-enhanced multiphoton ionization Moore NP, Levis RJ |
1321 - 1329 |
The microwave spectra and structures of Ar-AgX (X=F,Cl,Br) Evans CJ, Gerry MCL |
1330 - 1334 |
Reactions of C+(P-2(u)) with CO((1)Sigma(+)) from thermal energies to 30 eV Lu WY, Tosi P, Filippi M, Bassi D |
1335 - 1343 |
Experimental and theoretical study of line mixing in methane spectra. III. The Q branch of the Raman nu(1) band Pieroni D, Hartmann JM, Chaussard F, Michaut X, Gabard T, Saint-Loup R, Berger H, Champion JP |
1344 - 1352 |
Molecular calculations of excitation energies and (hyper)polarizabilities with a statistical average of orbital model exchange-correlation potentials Schipper PRT, Gritsenko OV, van Gisbergen SJA, Baerends EJ |
1353 - 1366 |
Anharmonic force field and vibrational frequencies of tetrafluoromethane (CF4) and tetrafluorosilane (SiF4) Wang XG, Sibert EL, Martin JML |
1367 - 1372 |
Three-dimensional picture of dynamical structure in liquid water Svishchev IM, Zassetsky AY |
1373 - 1382 |
A fast ab initio model for the calculation of excited electronic states of atoms and molecules in a weakly polarizable environment. I. Theory Kunz CF, Hess BA |
1383 - 1389 |
A fast ab initio model for the calculation of excited electronic states of atoms and molecules in a weakly polarizable environment. II. Application to the spectrum of cesium in liquid helium Kunz CF, Hess BA |
1390 - 1394 |
Mapping volume scale for overlapping clusters Reiss H, Bowles RK |
1395 - 1403 |
Calculation of the vibrational linewidth and line shape of Raman spectra using the relaxation function. I. Method and application to nitrogen Kooi ME, Smit F, Michels JPJ, Schouten JA |
1404 - 1412 |
Calculation of the vibrational linewidth and line shape of Raman spectra using the relaxation function. II. Application to the mixture neon-nitrogen with inhomogeneous broadening due to concentration fluctuations Kooi ME, Michels JPJ, Schouten JA |
1413 - 1424 |
Spin relaxation by dipolar coupling: From motional narrowing to the rigid limit Nevzorov AA, Freed JH |
1425 - 1443 |
Dipolar relaxation in a many-body system of spins of 1/2 Nevzorov AA, Freed JH |
1444 - 1448 |
Matrix isolation and spectroscopic characterization of a linear AlOSi radical Junker M, Friesen M, Schnockel H |
1449 - 1456 |
A simulation study of the decay of the pair correlation function in simple fluids Dijkstra M, Evans R |
1457 - 1461 |
On the identification of the vibrational spectrum of cyclic C-8 in solid Ar Wang SL, Rittby CML, Graham WRM |
1462 - 1473 |
Tumbling and spinning diffusions of acetonitrile in water and organic solvents Wakai C, Saito H, Matubayasi N, Nakahara M |
1474 - 1482 |
Ion pairing and dissociation at liquid/liquid interfaces: Molecular dynamics and continuum models Schweighofer K, Benjamin I |
1483 - 1488 |
Enhanced saturation coverages in adsorption-desorption processes Van Tassel PR, Viot P, Tarjus G, Ramsden JJ, Talbot J |
1489 - 1496 |
Studies of local structure of Cm3+ in borosilicate glass using laser and x-ray spectroscopic methods and computational modeling Liu GK, Zhorin VV, Antonio MR, Li ST, Williams CW, Soderholm L |
1497 - 1502 |
Tensor analysis of the second-order nonlinear optical susceptibility of chiral anisotropic thin films Kauranen M, Van Elshocht S, Verbiest T, Persoons A |
1503 - 1509 |
Dynamics of lithium ions in bismuthate glasses Pan A, Ghosh A |
1510 - 1521 |
Formalism, analytical model, and a priori Green's-function-based calculations of the current-voltage characteristics of molecular wires Hall LE, Reimers JR, Hush NS, Silverbrook K |
1522 - 1530 |
Collision-induced desorption of hydrocarbons physisorbed on Au(111) Libuda J, Scoles G |
1531 - 1540 |
Correlation effects in molecular diffusion in zeolites at infinite dilution Jousse F, Auerbach SM, Vercauteren DP |
1541 - 1546 |
Almost temperature independent charge carrier mobilities in liquid crystals Palenberg MA, Silbey RJ, Malagoli M, Bredas JL |
1547 - 1553 |
Globular state of random copolymers with arbitrary amphiphilicity Ganazzoli F |
1554 - 1559 |
Melt layer solidification of fatty acids in a rectangular cell Fukui K, Maeda K |
1560 - 1564 |
Calculation of helical twisting power for liquid crystal chiral dopants Cook MJ, Wilson MR |
1565 - 1573 |
Monte Carlo simulation of a grafted polymer chain confined in a tube Sotta P, Lesne A, Victor JM |
1574 - 1578 |
Microscopic density fluctuations and solvation in polymeric fluids Garde S, Khare R, Hummer G |
1579 - 1584 |
Generalized van der Waals density functional theory for nonuniform polymers Patra CN, Yethiraj A |
1585 - 1597 |
Theoretical study of polymeric mixtures with different sequence statistics. I. Ising class: Linear random copolymers with different statistical sequences and ternary blends of linear random copolymers with homopolymers Qi SY, Chakraborty AK |
1598 - 1605 |
Theoretical study of polymeric mixtures with different sequence statistics. II. Brazovskii class: Linear random copolymers with diblock copolymers Qi SY, Chakraborty AK |
1606 - 1615 |
Formation and equilibrium properties of living polymer brushes Milchev A, Wittmer JP, Landau DP |
1616 - 1617 |
Comment on "Calculation of ab initio dynamic hyperpolarizabilities of polymers" [J-Chem. Phys. 110, 2717 (1999)] Jacquemin D, Champagne B |
1618 - 1618 |
Response to "Comment on 'Calculation of ab initio dynamic hyperpolarizabilities of polymers' " [J-Chem. Phys. 112, 1616 (2000)] Gu FL, Ladik J |
1619 - 1619 |
Effects of local reactant concentration perturbations in oscillatory catalysis (vol 108, pg 5565, 1998) Lund CD, Surko CM, Maple MB, Yamamoto SY |
1620 - 1620 |
Ab initio calculations on the ground and excited states of BeOH and MgOH (vol 111, pg 10484, 1999) Theodorakopoulos G, Petsalakis ID, Hamilton IP |