1841 - 1843 |
The vinyl radical, ((A)over-tilde-(2)A ''<-(X)over-tilde-(2)A ') spectrum between 530 and 415 nm measured by cavity ring-down spectroscopy Pibel CD, McIlroy A, Taatjes CA, Alfred S, Patrick K, Halpern JB |
1844 - 1855 |
Generalized linear-scaling localized-density-matrix method Liang WZ, Yokojima S, Chen GH |
1856 - 1872 |
Ewald artifacts in computer simulations of ionic solvation and ion-ion interaction: A continuum electrostatics study Hunenberger PH, McCammon JA |
1873 - 1878 |
Constraints on density functionals and density functional derivatives Joubert D |
1879 - 1881 |
Gallium compounds, a possible problem for the G2 approaches Bauschlicher CW, Melius CF, Allendorf MD |
1882 - 1887 |
Topology of electron-electron interactions in atoms and molecules. II. The correlation cage Cioslowski J, Liu GH |
1888 - 1895 |
Improved power series expansion for the time evolution operator: Application to two-dimensional systems Drozdov AN, Hayashi S |
1896 - 1904 |
Extensions to quantum optimal control algorithms and applications to special problems in state selective molecular dynamics Sundermann K, de Vivie-Riedle R |
1905 - 1915 |
Managing singular behavior in the tracking control of quantum dynamical observables Zhu WS, Smit M, Rabitz H |
1916 - 1920 |
Density-functional study of van der Waals forces on rare-gas diatomics: Hartree-Fock exchange Perez-Jorda JM, San-Fabian E, Perez-Jimenez AJ |
1921 - 1930 |
Calculation of atomization energies by a multiconfigurational localized perturbation theory - Application for closed shell cases Dunietz BD, Murphy RB, Friesner RA |
1931 - 1941 |
Pump-probe spectroscopy of H-bonds: Saturation kinetics and spectral transformation during and after pumping Burshtein AI, Chernobrod BM, Sivachenko AY |
1942 - 1948 |
Collisional relaxation of highly vibrationally excited CF2O prepared with different initial energies and distribution functions Pino GA, Rinaldi CA, Coronado EA, Ferrero JC |
1949 - 1958 |
The O(D-1) yield from O-2 photodissociation near H Lyman-alpha (121.6 nm) Lacoursiere J, Meyer SA, Faris GW, Slanger TG, Lewis BR, Gibson ST |
1959 - 1968 |
Line-mixing effects in N2O Q branches: Model, laboratory, and atmospheric spectra Hartmann JM, Bouanich JP, Jucks KW, Blanquet G, Walrand J, Bermejo D, Domenech JL, Lacome N |
1969 - 1978 |
Determination of the proton tunneling splitting of tropolone in the ground state by microwave spectroscopy Tanaka K, Honjo H, Tanaka T, Kohguchi H, Ohshima Y, Endo Y |
1979 - 1989 |
Intramolecular vibrational energy redistribution and conformational isomerization in vibrationally excited 2-fluoroethanol: High-resolution, microwave-infrared double-resonance spectroscopy investigation of the asymmetric -CH2(F) stretch near 2980 cm(-1) Green D, Hammond S, Keske J, Pate BH |
1990 - 1999 |
The rotational spectrum of a highly vibrationally mixed quantum state. II. The eigenstate-resolved spectroscopy analog to dynamic nuclear magnetic resonance spectroscopy Pate BH |
2000 - 2009 |
The rotational spectra of single molecular eigenstates of 2-fluoroethanol: Measurement of the conformational isomerization rate at 2980 cm(-1) McWhorter DA, Hudspeth E, Pate BH |
2010 - 2015 |
Infrared spectroscopy of jet-cooled neutral and ionized aniline-Ar Piest H, von Helden G, Meijer G |
2016 - 2028 |
The fluorescence depletion spectroscopy of CdCH3 Pushkarsky MB, Barckholtz TA, Miller TA |
2029 - 2041 |
Probing the alignment of NO(X-2 Pi) by [2+1] resonance-enhanced multiphoton ionization via the C-2 Pi state: A test of semiclassical theory in 355 nm photodissociation of NO2 Mo YX, Katayanagi H, Suzuki T |
2042 - 2050 |
Predissociation of acetylene from the (A)over-tilde (1)A(u) state studied by absorption, laser-induced fluorescence, and H-atom action spectroscopies Suzuki T, Hashimoto N |
2051 - 2058 |
Long-range coefficients for the low-lying electronic states of BeLi and Be-2 Begue D, Merawa M, Rerat M, Pouchan C |
2059 - 2068 |
Fragment recoil anisotropies in the photoinitiated decomposition of HNCO Zyrianov M, Droz-Georget T, Reisler H |
2069 - 2073 |
A computational study of the enthalpies of formation of halomethylidynes Marshall P, Misra A, Schwartz M |
2074 - 2086 |
The vibrational energy pattern in acetylene (IV): Updated global vibration constants for (C2H2)-C-12 El Idrissi MI, Lievin J, Campargue A, Herman M |
2087 - 2098 |
Rotational state dependence of collision induced line broadening and shift at low temperature Flatin DC, Goyette TM, Beaky MM, Ball CD, De Lucia FC |
2099 - 2108 |
Calculation of conformational transitions and barriers in solvated systems: Application to the alanine dipeptide in water Apostolakis J, Ferrara P, Caflisch A |
2109 - 2115 |
Voids and clusters in expanded water Mountain RD |
2116 - 2121 |
Hierarchies of nonclassical reaction kinetics due to anisotropic confinements Ahn J, Kopelman R, Argyrakis P |
2122 - 2128 |
Thermal mobility of atomic hydrogen in solid argon and krypton matrices Vaskonen K, Eloranta J, Kiljunen T, Kunttu H |
2129 - 2139 |
An infrared study on CO intercalated in solid C-60 Holleman I, von Helden G, van der Avoird A, Meijer G |
2140 - 2144 |
A simple weighted-density-functional method: Test and its application to hard sphere fluid in spherical cavity Zhou SQ |
2145 - 2150 |
A neutron diffraction and computer modeling study of the interatomic structure of phosphoric acid Tromp RH, Spieser SH, Neilson GW |
2151 - 2158 |
A sequential-analytic method for determining the radial distribution function and predicting the thermodynamic properties of real fluids Chen GJ, Guo TM |
2159 - 2163 |
Thermally driven escape over a barrier of arbitrary shape Drozdov AN, Brey JJ |
2164 - 2174 |
Excited-state reversible geminate reaction. I. Two different lifetimes Gopich IV, Solntsev KM, Agmon N |
2175 - 2180 |
Excited-state reversible geminate reaction. II. Contact geminate quenching Agmon N |
2181 - 2188 |
Barrier properties of oriented disk composites Fredrickson GH, Bicerano J |
2189 - 2194 |
A note on the green dyadic calculation of the decay rates for admolecules at multiple planar interfaces Hartman RL, Cohen SM, Leung PT |
2195 - 2201 |
Modeling self-assembling of proteins: Assembled structures, relaxation dynamics, and phase coexistence Vekhter B, Berry RS |
2202 - 2207 |
Nitrate ion detection in aerosols using morphology-dependent stimulated Raman scattering Aker PM, Zhang JX, Nichols W |
2208 - 2218 |
Optical line shapes of dynamically disordered ring aggregates Bakalis LD, Coca M, Knoester J |
2219 - 2225 |
Theoretical and experimental adsorption studies of polyelectrolytes on an oppositely charged surface Mashl RJ, Gronbech-Jensen N, Fitzsimmons MR, Lutt M, Li DQ |
2226 - 2239 |
Low-energy reactive ion scattering as a probe of surface femtochemical reaction: H+ and H- formation on ionic compound surfaces Souda R, Suzuki T, Kawanowa H, Asari E |
2240 - 2249 |
A first-principles potential energy surface for Eley-Rideal reaction dynamics of H atoms on Cu(111) Persson M, Stromquist J, Bengtsson L, Jackson B, Shalashilin DV, Hammer B |
2250 - 2256 |
Dynamics of surface directed mesophase formation in block copolymer melts Sevink GJA, Zvelindovsky AV, van Vlimmeren BAC, Maurits NM, Fraaije JGEM |
2257 - 2263 |
Thermal desorption from ordered chemisorbed phases studied by helium scattering: Oxygen on Ag(110) Canepa M, Terreni S, Narducci E, Mattera L |
2264 - 2266 |
Temperature-induced transition to a nonmicellar state de Moraes JNB, Figueiredo W |
2267 - 2279 |
Modeling of oscillatory dynamics of a simple enzyme-diffusion system with hysteresis. The case of lumped permeabilities Zou XQ, Siegel RA |
2280 - 2288 |
Metastable states and the kinetics of colloid phase separation Soga KG, Melrose JR, Ball RC |
2289 - 2296 |
Phase coexistence of neutral polymer gels under mechanical constraint Suzuki A, Ishii T |
2297 - 2304 |
Conformation of interacting lysozyme by polarized and depolarized light scattering Chirico G, Beretta S, Baldini G |