999 - 1002 |
Time-resolved photoelectron imaging of the photodissociation of I-2(-) Davis AV, Wester R, Bragg AE, Neumark DM |
1003 - 1006 |
Oxygen adsorption on graphite and nanotubes Giannozzi P, Car R, Scoles G |
1007 - 1014 |
A Lorentzian function based spectral filter for calculating the energy of excited bound states in quantum mechanics Vijay A |
1015 - 1026 |
Quasirelativistic theory for the magnetic shielding constant. I. Formulation of Douglas-Kroll-Hess transformation for the magnetic field and its application to atomic systems Fukuda R, Hada M, Nakatsuji H |
1027 - 1035 |
Quasirelativistic theory for magnetic shielding constants. II. Gauge-including atomic orbitals and applications to molecules Fukuda R, Hada M, Nakatsuji H |
1036 - 1043 |
Angular momentum in solid-harmonic-Gaussian integral evaluation Dunlap BI |
1044 - 1053 |
Application of time-dependent current-density-functional theory to nonlocal exchange-correlation effects in polymers van Faassen M, de Boeij PL, van Leeuwen R, Berger JA, Snijders JG |
1054 - 1058 |
Usefulness of the Colle-Salvetti model for the treatment of the nondynamic correlation Sancho-Garcia JC, Moscardo F |
1059 - 1067 |
A general method for implementing vibrationally adiabatic mixed quantum-classical simulations Thompson WH |
1068 - 1073 |
Local hybrid functionals Jaramillo J, Scuseria GE, Ernzerhof M |
1074 - 1084 |
Self-guided enhanced sampling methods for thermodynamic averages Andricioaei I, Dinner AR, Karplus M |
1085 - 1088 |
Efficient thermal rate constant calculation for rare event systems Corcelli SA, Rahman JA, Tully JC |
1089 - 1100 |
Ab initio molecular dynamics with a continuum solvation model Senn HM, Margl PM, Schmid R, Ziegler T, Blochl PE |
1101 - 1109 |
On the optimization of Gaussian basis sets Petersson GA, Zhong SJ, Montgomery JA, Frisch MJ |
1110 - 1118 |
Method for the ab initio calculation of intermolecular potentials of ionic clusters: Test on Rg-CO+, Rg=He, Ne, Ar Lotrich VF, van der Avoird A |
1119 - 1127 |
Many-body effects in nonadiabatic molecular theory for simultaneous determination of nuclear and electronic wave functions: Ab initio NOMO/MBPT and CC methods Nakai H, Sodeyama K |
1128 - 1136 |
Equation-of-motion coupled cluster method with full inclusion of the connected triple excitations for ionized states: IP-EOM-CCSDT Musial M, Kucharski SA, Bartlett RJ |
1137 - 1145 |
Core shell excitation of 2-propenal (acrolein) at the O 1s and C 1s edges: An experimental and ab initio study Duflot D, Flament JP, Walker IC, Heinesch J, Hubin-Franskin MJ |
1146 - 1157 |
Understanding highly excited states via parametric variations Semparithi A, Charulatha V, Keshavamurthy S |
1158 - 1161 |
Infrared emission spectra of BeH and BeD Shayesteh A, Tereszchuk K, Bernath PF, Colin R |
1162 - 1174 |
The dynamics of the H+D2O -> OD+HD reaction at 2.5 eV: Experiment and theory Brouard M, Burak I, Minayev D, O'Keeffe P, Vallance C, Aoiz FJ, Banares L, Castillo JF, Zhang DH, Collins MA |
1175 - 1183 |
Velocity map imaging of the photodissociation of CF3I: Vibrational energy dependence of the recoil anisotropy Aguirre F, Pratt ST |
1184 - 1188 |
Quantum dynamics study of the isotopic effect on capture reactions: HD, D-2+CH3 Wang DY |
1189 - 1195 |
Ab initio transition state theory calculation of the rate constant for the hydrogen abstraction reaction H2O2+H -> H-2+HO2 Tarchouna Y, Bahri M, Jaidane N, Ben Lakhdar Z, Flament JP |
1196 - 1205 |
Intermolecular vibrations of the hydrogen bonded OH-CO reactant complex Marshall MD, Pond BV, Lester MI |
1206 - 1213 |
Broadband absorption and ab initio results on the CF C-2 Sigma(+)-X-2 Pi system Luque J, Hudson EA, Booth JP, Petsalakis ID |
1214 - 1220 |
Gas-phase detection of the FCO2 radical by millimeter wave and high resolution infrared spectroscopy assisted by ab initio calculations Zelinger Z, Drean P, Walters A, Moreno JRA, Bogey M, Pernice H, von Ahsen S, Willner H, Breidung J, Thiel W, Burger H |
1221 - 1229 |
Infrared cavity ringdown spectroscopy of acid-water clusters: HCl-H2O, DCl-D2O, and DCl-(D2O)(2) Huneycutt AJ, Stickland RJ, Hellberg F, Saykally RJ |
1230 - 1241 |
Study of the benzene center dot N-2 intermolecular potential-energy surface Lee S, Romascan J, Felker PM, Pedersen TB, Fernandez B, Koch H |
1242 - 1252 |
Laser fluorescence excitation spectroscopy of the GeAr van der Waals complex Tao C, Dagdigian PJ |
1253 - 1265 |
Experimental studies of peptide bonds: Identification of the C-7(eq) conformation of the alanine dipeptide analog N-acetyl-alanine N-methylamide from torsion-rotation interactions Lavrich RJ, Plusquellic DF, Suenram RD, Fraser GT, Walker ARH, Tubergen MJ |
1266 - 1271 |
The permanent electric dipole moments of the (B)over-tilde(2)Sigma(+) and (X)over-tilde(2)Sigma(+) states of lanthanum imide, LaNH Steimle TC, Bousquet RR, Merer AJ, Rixon SJ |
1272 - 1281 |
Binding energy, structure, and vibrational spectra of (HCl)(2-6) and (HF)(2-10) clusters by density functional theory Guedes RC, do Couto PC, Cabral BJC |
1282 - 1291 |
Time-resolved photoelectron spectra as probe of excited state dynamics: A full quantum study of the Na2F cluster Heitz MC, Durand G, Spiegelman F, Meier C |
1292 - 1300 |
Calculation of frequency-dependent polarizabilities using the approximate coupled-cluster triples model CC3 Hald K, Pawlowski F, Jorgensen P, Hattig C |
1301 - 1311 |
Influence of hydrodynamic interaction on the diffusion-controlled reaction kinetics of molecules with highly anisotropic reactivity Shushin AI |
1312 - 1326 |
Isomerization and intermolecular solute-solvent interactions of ethyl isocyanate: Ultrafast infrared vibrational echoes and linear vibrational spectroscopy Levinger NE, Davis PH, Behera PK, Myers DJ, Stromberg C, Fayer MD |
1327 - 1332 |
Structure of an inhomogeneous fluid mixture: A new weighted density-functional theory within a perturbative approach Choudhury N, Ghosh SK |
1333 - 1340 |
Ion-water interaction potentials in the semimicroscopic model Dorman VL, Jordan PC |
1341 - 1346 |
Density fluctuation of a van der Waals fluid in supercritical state Nishikawa K, Kusano K, Arai AA, Morita T |
1347 - 1355 |
Ab initio simulation of the two-dimensional vibrational spectrum of dicarbonylacetylacetonato rhodium(I) Moran AM, Dreyer J, Mukamel S |
1356 - 1363 |
Dielectric hole burning in the high frequency wing of supercooled glycerol Duvvuri K, Richert R |
1364 - 1377 |
Photolysis of the OC center dot center dot center dot HONO complex in low temperature matrices: Infrared detection and ab initio calculations of nitrosoformic acid, HOC(O)NO Mielke Z, Olbert-Majkut A, Tokhadze KG |
1378 - 1391 |
Electronic structure of para aminophenoxyl radical in water Tripathi GNR |
1392 - 1399 |
A general expression for the condensation coefficient based on transition state theory and molecular dynamics simulation Nagayama G, Tsuruta T |
1400 - 1403 |
Melting of nanostructured Sn probed by in-situ x-ray diffraction Depero LE, Bontempi E, Sangaletti L, Pagliara S |
1404 - 1416 |
Interacting chain model for poly(ethylene glycol) from first principles - stretching of a single molecule using the transfer matrix approach Livadaru L, Netz RR, Kreuzer HJ |
1417 - 1422 |
Computer simulation of anisotropic diffusion in monolayer films in mica slit pores Su Z, Cushman JH, Curry JE |
1423 - 1432 |
Theoretical calculations of the electroabsorption spectra of perylenetetracarboxylic dianhydride Mazur G, Petelenz P, Slawik M |
1433 - 1439 |
Model for chemical effects in non-steady-state radiation enhanced diffusion of Ti in MgO Lu M, Lupu C, Rabalais JW |
1440 - 1452 |
Derivation of expressions for the spontaneous curvature, mean and Gaussian bending constants of thermodynamically open surfactant monolayers and bilayers Bergstrom M |
1453 - 1465 |
Fluid phase transitions at chemically heterogeneous, nonplanar solid substrates: Surface versus confinement effects Sacquin S, Schoen M, Fuchs AH |
1466 - 1478 |
Inhomogeneous suspensions of rigid rods in flow Dhont JKG, Briels WJ |
1479 - 1486 |
Surface-induced dissociations and reactions of acetonitrile monomer, dimer and trimer ions Mair C, Herman Z, Fedor J, Lezius M, Mark TD |
1487 - 1498 |
Molecular dynamics study of cristobalite silica using a charge transfer three-body potential: Phase transformation and structural disorder Huang LP, Kieffer J |
1499 - 1506 |
High pressure reactivity of solid furan probed by infrared and Raman spectroscopy Ceppatelli M, Santoro M, Bini R, Schettino V |
1507 - 1513 |
Interaction of a spherical particle with linear chains Klos J, Pakula T |
1514 - 1520 |
Quenching of an excitation moving on a flexible polymer Park PJ, Lee S |
1521 - 1532 |
Detailed atomistic Monte Carlo simulation of grafted polymer melts: II. Orientational order and nuclear magnetic resonance spectra Daoulas KC, Mavrantzas VG, Photinos DJ |
1533 - 1540 |
Efficient generation of low-energy folded states of a model protein Gordon HL, Kwan WK, Gong C, Larrass S, Rothstein SM |
1541 - 1549 |
Fluid demixing in colloid-polymer mixtures: Influence of polymer interactions Schmidt M, Denton AR, Brader JM |
1550 - 1556 |
Photophysics of thiophene based polymers in solution: The role of nonradiative decay processes de Melo JS, Burrows HD, Svensson M, Andersson MR, Monkman AP |
1557 - 1570 |
Generating strange magnetic and dielectric interactions: Classical molecules and particle foams Martin JE, Anderson RA, Williamson RL |
1571 - 1572 |
Comment on "Classical polarizable force fields parametrized from ab initio calculations" [J. Chem. Phys. 117, 1416 (2002)] Chelli R, Procacci P |
1573 - 1574 |
Transition strengths and potential curves for the valence transitions in Br-2 from a reanalysis of the ultraviolet-visible absorption at low resolution (vol 115, pg 10417, 2001) Tellinghuisen J |