2351 - 2356 |
Range definitions for Gaussian-type charge distributions in fast multipole methods Kudin KN, Scuseria GE |
2357 - 2370 |
Path integral centroid variables and the formulation of their exact real time dynamics Jang S, Voth GA |
2371 - 2384 |
A derivation of centroid molecular dynamics and other approximate time evolution methods for path integral centroid variables Jang S, Voth GA |
2385 - 2391 |
The calculation of molecular parameters for a molecule with an internal rotor Duan YB, Wang L, Wu XDT, Mukhopadhyay I, Takagi K |
2392 - 2400 |
Bond configurations in the Peierls-Hubbard model of small ring-shaped molecules Liviotti E, Ubertini F, Erdos P |
2401 - 2406 |
Vibrational-rotational energy transfer in H-2-H-2 collisions. I. Semiclassical decoupling approximation Zenevich VA, Billing GD |
2407 - 2413 |
Ab initio calculation of the interaction potential for the krypton dimer: The use of bond function basis sets Tao FM |
2414 - 2422 |
Fluorescence quenching by reversible excimer formation: Kinetic study on the basis of generalized, non-Markovian rate equations Naumann W |
2423 - 2435 |
Quantum fluid dynamics in the Lagrangian representation and applications to photodissociation problems Mayor FS, Askar A, Rabitz HA |
2436 - 2443 |
Vibrational spectroscopy of methanol and acetonitrile clusters in cold helium droplets Behrens M, Frochtenicht R, Hartmann M, Siebers JG, Buck U, Hagemeister FC |
2444 - 2450 |
The near infrared, visible, and near ultraviolet overtone spectrum of water Carleer M, Jenouvrier A, Vandaele AC, Bernath PF, Merienne MF, Colin R, Zobov NF, Polyansky OL, Tennyson J, Savin VA |
2451 - 2463 |
Quantum scattering study of electronic Coriolis and nonadiabatic coupling effects in O(D-1)+H-2 -> OH+H Drukker K, Schatz GC |
2464 - 2469 |
The electronic structure of MoC and WC by anion photoelectron spectroscopy Li X, Liu SS, Chen WW, Wang LS |
2470 - 2477 |
ArHF vibrational predissociation dynamics using the diatomics-in-molecule potential energy surface Buchachenko AA, Stepanov NF, Grigorenko BL, Nemukhin AV |
2478 - 2483 |
The one-atom cage effect in I-2(B)-Ar: Evidence that caging is inefficient for the T-shaped isomer Burroughs A, Van Marter T, Heaven MC |
2484 - 2489 |
Spectroscopic characterization of the weakly bound Ca(4s4d sigma D-3(3))center dot Ar[(3)Sigma(+)] state: Evidence for a substantial maximum in the potential curve at long range Leung AWK, Kaup JG, Bellert D, McCaffrey JG, Breckenridge WH |
2490 - 2498 |
Differential cross sections for H+D-2 -> HD (v '=2, J '=0,3,5)+D at 1.55 eV Fernandez-Alonso F, Bean BD, Zare RN |
2499 - 2506 |
Time-dependent density functional calculations on the electronic absorption spectrum of free base porphin van Gisbergen SJA, Rosa A, Ricciardi G, Baerends EJ |
2507 - 2512 |
Reaction of state-selected ammonia ions with methane Everest MA, Poutsma JC, Flad JE, Zare RN |
2513 - 2518 |
Observation of linear isomers of the ionized rare gas tetramers Ar-4(+) and Xe-4(+) Von Issendorff B, Hofmann A, Haberland H |
2519 - 2531 |
Rotational state-to-state rate constants and pressure broadening coefficients for He-C2H2 collisions: Theory and experiment Heijmen TGA, Moszynski R, Wormer PES, van der Avoird A, Rudert AD, Halpern JB, Martin J, Gao WB, Zacharias H |
2532 - 2541 |
The infrared spectrum of the nitric oxide dimer cation: Problems for density functional theory and a muddled relationship to experiment Xie YM, Schaefer HF, Fu XY, Liu RZ |
2542 - 2555 |
Bonding in hypohalous acids HOX (X=F, Cl, Br, and I) from the topological analysis of the electron localization function Berski S, Silvi B, Latajka Z, Leszczynski J |
2556 - 2564 |
Autoionizing Rydberg states of NO in strong electric fields Warntjes JBM, Robicheaux F, Bakker JM, Noordam LD |
2565 - 2587 |
A new six-dimensional analytical potential up to chemically significant energies for the electronic ground state of hydrogen peroxide Kuhn B, Rizzo TR, Luckhaus D, Quack M, Suhm MA |
2588 - 2594 |
Electronic nonadiabaticity in highly vibrationally excited O-2(X (3)Sigma(-)(g)): Spin-orbit coupling between X (3)Sigma(-)(g) and b (1)Sigma(+)(g) Jongma RT, Shi SM, Wodtke AM |
2595 - 2605 |
Photodissociation of HBr molecules and clusters: Anisotropy parameters, branching ratios, and kinetic energy distributions Baumfalk R, Buck U, Frischkorn C, Nahler NH, Huwel L |
2606 - 2619 |
Photodissociation of Ar-HCl: An energy-resolved study of the dynamics of total fragmentation into H+Ar+Cl Juanes-Marcos JC, Garcia-Vela A |
2620 - 2632 |
A quantum mechanical view of molecular alignment and cooling in seeded supersonic expansions Aquilanti V, Ascenzi D, Vitores MD, Pirani F, Cappelletti D |
2633 - 2640 |
Structures and energetics of Ne-n-HN2+ clusters Meuwly M |
2641 - 2646 |
The structure of fluid argon from high-pressure neutron diffraction and ab initio molecular dynamics simulations Pfleiderer T, Waldner I, Bertagnolli H, Todheide K, Kirchner B, Huber H, Fischer HE |
2647 - 2656 |
A single-bond approach to orientation-dependent interactions and its implications for liquid water Truskett TM, Debenedetti PG, Sastry S, Torquato S |
2657 - 2664 |
The induction period of the CaCl2-Na2CO3 system: Theory and experiment Chien WC, Tai CY, Hsu JP |
2665 - 2677 |
Fractional power dependence of mean lifetime of electron transfer reaction on viscosity of solvent Okada A |
2678 - 2685 |
Quadratic response of molecules in a nonequilibrium and equilibrium solvation model: Generalizations to include both singlet and triplet perturbations Poulsen TD, Ogilby PR, Mikkelsen KV |
2686 - 2694 |
Exponential intermolecular dynamics in optical Kerr effect spectroscopy of small-molecule liquids Loughnane BJ, Scodinu A, Farrer RA, Fourkas JT, Mohanty U |
2695 - 2700 |
Nonlinear thermal response at the glass transition Schick C, Merzlyakov M, Hensel A |
2701 - 2709 |
Dynamical properties of the soft sticky dipole model of water: Molecular dynamics simulations Chandra A, Ichiye T |
2710 - 2719 |
Translational-rotational coupling in supercooled liquids: Heterodyne detected density induced molecular alignment Hinze G, Francis RS, Fayer MD |
2720 - 2725 |
Scattered and recoiled ion fractions from LiTaO3(100) surfaces with different electrical properties Kim Y, Kim SS, Ada E, Yang YL, Jacobson AJ, Rabalais JW |
2726 - 2734 |
Diffusion and evaporation kinetics of large islands and vacancies on surfaces Lo A, Skodje RT |
2735 - 2743 |
Simulation of self-diffusion of point-like and finite-size tracers in stochastically reconstructed Vycor porous glasses Kainourgiakis ME, Kikkinides ES, Stubos AK, Kanellopoulos NK |
2744 - 2750 |
XPS studies of Ru-polypyridine complexes for solar cell applications Rensmo H, Westermark K, Sodergren S, Kohle O, Persson P, Lunell S, Siegbahn H |
2751 - 2760 |
A transition-state theory approach to adsorbate dynamics at arbitrary loadings Tunca C, Ford DM |
2761 - 2769 |
Screening ionic motion in sodalite cages: A dynamical study Filippone F, Gianturco FA |
2770 - 2778 |
Surface-induced reactions of acetone cluster cations Mair C, Fiegele T, Biasioli F, Herman Z, Mark TD |
2779 - 2788 |
Birefringence and second-order nonlinear optics as probes of polymer cooperative segmental mobility: Demonstration of Debye-type relaxation Hooker JC, Burghardt WR, Torkelson JM |
2789 - 2796 |
Self-diffusion of an asymmetric diblock copolymer above and below the order-to-disorder transition temperature Fleischer G, Rittig F, Karger J, Papadakis CM, Mortensen K, Almdal K, Stepanek P |
2797 - 2808 |
Wetting of a fluid interface by a homopolymer: A system with a rich prewetting behavior Leermakers FAM, Dorrepaal C, Besseling NAM |
2809 - 2817 |
Associating polyelectrolytes: Finite size cluster stabilization versus physical gel formation Potemkin II, Vasilevskaya VV, Khokhlov AR |
2818 - 2828 |
Complexation to macromolecules with a large number of sites Garces JL, Mas F, Puy J |
2829 - 2841 |
On the nature of electronic excitations in poly(paraphenylenevinylene): A quantum-chemical investigation Beljonne D, Shuai Z, Cornil J, dos Santos DA, Bredas JL |
2842 - 2843 |
Droplet size dependence upon volume expansion rate Ashurst WT, Holian BL |
2844 - 2845 |
Comment on "Improving protein circular dichroism calculations in the far-ultraviolet through reparametrizing the amide chromophore" [J. Chem. Phys. 109, 782, (1998)] Woody RW, Sreerama N |
2846 - 2847 |
Response to "Comment on 'Improving protein circular dichroism calculations in the far-ultraviolet through reparameterizing the amide chromophore' " [ J. Chem. Phys. 111, 2844 (1999)] Hirst JD, Besley NA |
2848 - 2848 |
An advanced dielectric continuum approach for treating solvation effects: Time correlation functions. I. Local treatment (vol 108, pg 1103, 1998) Basilevsky MV, Parsons DF, Vener MV |