2049 - 2051 |
State-resolved two-photon laser induced fluorescence detection of BrO Delmdahl RF, Gericke KH |
2052 - 2055 |
Silicide formation by high-temperature reaction of Rh with model SiO2 films Labich S, Kohl A, Taglauer E, Knozinger H |
2056 - 2064 |
A strictly variational procedure for cluster embedding based on the extended subspace approach Gutdeutsch U, Birkenheuer U, Rosch N |
2065 - 2070 |
Identifying collective dynamical observables bearing on local features of potential surfaces Lazarides AA, Rabitz H, Chang J, Brown NJ |
2071 - 2079 |
Inflection spacing symmetry of diatomic potential curves Herrick DR, O'Connor S |
2080 - 2091 |
Path integrals for Fokker-Planck dynamics with singular diffusion : Accurate factorization for the time evolution operator Drozdov AN, Talkner P |
2092 - 2098 |
A new inhomogeneity parameter in density-functional theory Becke AD |
2099 - 2110 |
A nonequilibrium statistical grand-canonical ensemble : Description in terms of flux operators Madureira JR, Vasconcellos AR, Luzzi R |
2111 - 2122 |
Gustavson's procedure and the dynamics of highly excited vibrational states Joyeux M |
2123 - 2134 |
A comparison of the efficiency of Fourier- and discrete time-path integral Monte Carlo Chakravarty C, Gordillo MC, Ceperley DM |
2135 - 2143 |
Effective Hamiltonian for near-degenerate states in relativistic direct perturbation theory. II. H-2(+)-like systems Rutkowski A, Schwarz WHE, Kozlowski R, Beczek J, Franke R |
2144 - 2154 |
RG+Cl(P-2) (RG = He, Ne, Ar) interactions : Ab initio potentials and collision properties Burcl R, Krems RV, Buchachenko AA, Szczesniak MM, Chalasinski G, Cybulski SM |
2155 - 2161 |
Electron bombardment matrix isolation of Rg/Rg '/methanol mixtures (Rg = Ar, Kr, Xe) : Fourier-transform infrared characterization of the proton-bound dimers Kr2H+, Xe2H+, (ArHKr)(+) and (ArHXe)(+) in Ar matrices and (KrHXe)(+) and Xe2H+ in Kr matrices Fridgen TD, Parnis JM |
2162 - 2168 |
Density functional theory study of the proton-bound rare-gas dimers Rg(2)H(+) and (RgHRg ')(+) (Rg = Ar, Kr, Xe) : Interpretation of experimental matrix isolation infrared data Fridgen TD, Parnis JM |
2169 - 2175 |
Intermolecular interaction potential of the carbon dioxide dimer Tsuzuki S, Uchimaru T, Mikami M, Tanabe K |
2176 - 2184 |
Molecular dynamics study of the Ag-6 cluster using an ab initio many-body model potential Garzon IL, Kaplan IG, Santamaria R, Novaro O |
2185 - 2193 |
The 16 valence electronic states of nitric oxide dimer (NO)(2) East ALL |
2194 - 2201 |
Resonant coherent hyper-Raman scattering (CHRS). II. A theory on the general relationship between CHRS and coherent Raman scattering (CRS) processes Cho MH |
2202 - 2209 |
A theoretical characterization of the quartet states of the SO+ molecular ion Ornellas FR, Borin AC |
2210 - 2219 |
Vuv photolysis of hydrazoic acid : Absorption and fluorescence excitation spectra Schonnenbeck G, Biehl H, Stuhl F, Meier U, Staemmler V |
2220 - 2232 |
Electronic spectroscopy and ab initio quantum chemical study of the (A)over-tilde((1)A '')-(X)over-tilde((1)A ') transition of CFBr Knepp PT, Scalley CK, Bacskay GB, Kable SH |
2233 - 2241 |
Benchmark calculations with correlated molecular wave functions. IX. The weakly bound complexes Ar-H-2 and Ar-HCl Woon DE, Peterson KA, Dunning TH |
2242 - 2245 |
Rotational spectra of (NeH+)-Ne-20, (NeD+)-Ne-20, (NeH+)-Ne-22, and (NeD+)-Ne-22 Matsushima F, Ohtaki Y, Torige O, Takagi K |
2246 - 2253 |
Dissociative photoionization of SO2 from 16 to 120 eV Masuoka T, Chung YM, Lee EM, Samson JAR |
2254 - 2256 |
Relativistic corrections to the energies of the EF, GK, and H(H)over-bar (1)Sigma(g) states of the hydrogen molecule Wolniewicz L |
2257 - 2263 |
Nonadiabatic effects in the photodissociation of vibrationally excited HNCO : The branching between singlet (a (1)Delta) and triplet (X (3)Sigma(-)) NH Berghout HL, Brown SS, Delgado R, Crim FF |
2264 - 2274 |
Electric field gradient, generalized Sternheimer shieldings and electric field gradient polarizabilities by multiconfigurational SCF response Rizzo A, Ruud K, Helgaker T, Jaszunski M |
2275 - 2278 |
Photoelectron spectra of Nb-n(-) clusters : Correlation between electronic structure and hydrogen chemisorption Kietzmann H, Morenzin J, Bechthold PS, Gantefor G, Eberhardt W |
2279 - 2286 |
Two-dimensional treatment of the methyl and aldehydic torsions in gas phase propanal Vivier-Bunge A, Uc VH, Smeyers YG |
2287 - 2293 |
Proton transfer in benzoic acid crystals : Another look using quantum operator theory Antoniou D, Schwartz SD |
2294 - 2305 |
Spectroscopic study of Cr3+ ions in fluorochloro- and fluorobromozirconate glasses Bunuel MA, Alcala R, Cases R |
2306 - 2309 |
Size-dependent electronic level structure of InAs nanocrystal quantum dots : Test of multiband effective mass theory Banin U, Lee CJ, Guzelian AA, Kadavanich AV, Alivisatos AP, Jaskolski W, Bryant GW, Efros AL, Rosen M |
2310 - 2315 |
Adsorption of a hard-sphere fluid in a slitlike pore with molecularly rough walls Bryk P, Pizio O, Sokolowski S |
2316 - 2324 |
A unified model for ion conduction in crystals of beta- and beta ''-alumina structure Meyer M, Maass P, Bunde A |
2325 - 2338 |
Electron transfer reaction dynamics in non-Debye solvents Bicout DJ, Szabo A |
2339 - 2345 |
Closed-shell interaction in silver and gold chlorides Doll K, Pyykko P, Stoll H |
2346 - 2354 |
A molecular-orbital derived polarization potential for liquid water Gao JL |
2355 - 2360 |
Concentration-profile- and molecular-size-dependent instabilities associated with the free diffusion and self-assembling of amphiphiles along a solid-fluid-fluid meniscus Haidara H, Vonna L, Schultz J |
2361 - 2370 |
A theory for the liquid-crystalline phase behavior of the Gay-Berne model Velasco E, Mederos L |
2371 - 2379 |
Elastic constants from a microscopic model of bilayer membrane Chacon E, Somoza AM, Tarazona P |
2380 - 2393 |
Multidimensional solid-state nuclear magnetic resonance for determining the dihedral angle from the correlation of C-13-H-1 and C-13-C-13 dipolar interactions under magic-angle spinning conditions Fujiwara T, Shimomura T, Ohigashi Y, Akutsu H |
2394 - 2402 |
Hydration of ions at various temperatures : The role of electrostriction Danielewicz-Ferchmin I, Ferchmin AR |
2403 - 2412 |
Solvation and conformational dynamics of dicarboxylic suberic acid Nilsson JA, Laaksonen A, Eriksson LA |
2413 - 2422 |
The metastable T-P phase diagram and anomalous thermodynamic properties of supercooled water Ponyatovsky EG, Sinitsyn VV, Pozdnyakova TA |
2423 - 2428 |
The screening length of charge-asymmetric electrolytes : A hypernetted chain calculation McBride A, Kohonen M, Attard P |
2429 - 2431 |
Effects of initial conditions on the development of spinodal decomposition Chikina I |
2432 - 2436 |
Differential scanning calorimetry, x-ray diffraction and F-19 nuclear magnetic resonance investigations of the crystallization of InF3-based glasses Franco RWA, Tambelli CC, Magon CJ, Donoso JP, Messaddeq Y, Ribeiro SJL, Poulain M |
2437 - 2441 |
Effect of convective transport on droplet spinodal decomposition in fluids Kumaran V |
2442 - 2449 |
Energetics of silicon hydrides on the Si(100)-(2x1) surface Brown AR, Doren DJ |
2450 - 2459 |
The influence of molecular rotation on the direct subsurface absorption of H-2 on Pd(111) Olsen RA, Kroes GJ, Baerends EJ |
2460 - 2466 |
Picosecond infrared pump-probe spectrum of D2O adsorbed at acid OD group of zeolite Fujino T, Kashitani M, Onda K, Wada A, Domen K, Hirose C, Ishida M, Goto F, Kano SS |
2467 - 2473 |
Adsorption dynamics of monoenergetic iodine monobromide (IBr) on the Si(111)-7x7 surface Liu Y, Komrowski AJ, Taylor PR, Kummel AC |
2474 - 2479 |
Substrate mediated photochemistry on a molecular surface : OCS on Ag clusters Brown LA, Rayner DM |
2480 - 2489 |
Ion-ion correlations in electrolyte solutions adsorbed in disordered electroneutral charged matrices from replica Ornstein-Zernike equations Hribar B, Pizio O, Trokhymchuk A, Vlachy V |
2490 - 2502 |
Collision induced desorption and dissociation of O-2 chemisorbed on Ag(001) Vattuone L, Gambardella P, Burghaus U, Cemic F, Cupolillo A, Valbusa U, Rocca M |
2503 - 2508 |
Free convection and surface kinetics in crystal growth from solution Baird JK, Guo LH |
2509 - 2512 |
Radial compression and controlled cutting of carbon nanotubes Lordi V, Yao N |
2513 - 2518 |
On the relationship between C-C and C-D order parameters and its use for studying the conformation of lipid acyl chains in biomembranes Douliez JP, Ferrarini A, Dufourc EJ |
2519 - 2527 |
Molecular self assembly of rodlike particles : An application to collagen Evans GT |
2528 - 2535 |
Non-Arrhenius modes in the relaxation of model proteins Skorobogatiy M, Guo H, Zuckermann M |
2536 - 2542 |
Langevin dynamics simulations of early-stage polymer nucleation and crystallization Liu C, Muthukumar M |
2543 - 2548 |
Vibrational spectroscopic study of 5,5 ''-bis(dicyanomethylene)-5,5 ''-dihydro-Delta(2,2 ' : 5 ',2 '')-terthiophene bearing a heteroquinonoid structure as a model of doped polythiophene Hernandez V, Hotta S, Navarrete JTL |
2549 - 2555 |
Linear and nonlinear optical response of polyenes : A density matrix renormalization group study Shuai Z, Bredas JL, Saxena A, Bishop AR |
2556 - 2561 |
Small angle neutron scattering experiments from colloidal dispersions at rest and under sheared conditions Dux C, Musa S, Reus V, Versmold H, Schwahn D, Lindner P |
2562 - 2564 |
A new scheme to calculate dipole-allowed singlets in conjugated polymers Zhang GP, George TF, Pandey LN |
2565 - 2571 |
Effective Hamiltonians of polymethineimine, polyazine and polyazoethene : A density matrix variation approach Chen GH, Su ZM, Shen ZW, Yan YJ |
2572 - 2578 |
Transient relaxation of a charged polymer chain subject to an external field in a random tube Burlatsky SF, Deutch JM |
2579 - 2587 |
The correlation functions of hard-sphere chains : Monodisperse chains as a complete association limit Chang J, Kim H |