873 - 877 |
The role of dark states in the photodynamics of the green fluorescent protein examined with two-color fluorescence excitation spectroscopy Jung G, Mais S, Zumbusch A, Brauchle C |
878 - 882 |
Photoelectron spectroscopy and circular dichroism in chiral biomolecules: L-alanine Powis I |
883 - 893 |
Luminescence and energy transfer of [Ru(bpy)(3)](2+), [Cr(ox)(3)](3-), and [Os(bpy)(3)](2+) in three-dimensional oxalato-networks von Arx ME, Burattini E, Hauser A, van Pieterson L, Pellaux R, Decurtins S |
894 - 898 |
Determination of the ground and excited state dipole moments of free base chlorin and isobacteriochlorin Singh A, Huang WY, Johnson LW |
899 - 907 |
Solvent and intramolecular effects on the absorption spectrum of betaine-30 Lobaugh J, Rossky PJ |
908 - 914 |
Alkali metal NMR chemical shielding as a probe of local structure: An experimental and theoretical study of Rb+ in halide lattices de Dios AC, Walling A, Cameron I, Ratcliffe CI, Ripmeester JA |
915 - 921 |
Carbon-oxygen bond dissociation enthalpies in peroxyl radicals Kranenburg M, Ciriano MV, Cherkasov A, Mulder P |
922 - 927 |
Theoretical analysis of concerted and stepwise mechanisms of Diels-Alder reaction between butadiene and ethylene Sakai S |
928 - 934 |
Selected ion flow tube studies of air plasma cations reacting with alkylbenzenes Arnold ST, Dotan I, Williams S, Viggiano AA, Morris RA |
935 - 946 |
Mechanism of the reaction of CH3SO with NO2 in relation to atmospheric oxidation of dimethyl sulfide: Experimental and theoretical study Kukui A, Bossoutrot V, Laverdet G, Le Bras G |
947 - 953 |
Direct space representation of the metallic bond Silvi B, Gatti C |
954 - 961 |
Vibrational spectroscopy and ab initio calculations on [N(C2F5SO2)(2)](-) and the corresponding superacid HN(C2F5SO2)(2) Johansson P, Tegenfeldt J, Lindgren J |
962 - 967 |
Interactions of molecular hydrogen with alkali metal halides in argon matrices: A computational model McKee ML, Sweany RL |
968 - 973 |
The acetylene-ammonia dimer as a prototypical C-H center dot center dot center dot N hydrogen-bonded system: An assessment of theoretical procedures Hartmann M, Radom L |
974 - 981 |
Geometry, vibrational frequencies, and ionization energies of BeX2 (X = F, Cl, Br, and I) Lee EPF, Wright TG |
982 - 989 |
C6F6 and sym-C6F3H3: Ab initio and DFT studies of structure, vibrations, and inelastic neutron scattering spectra Braden DA, Hudson BS |
990 - 994 |
A theoretical study of the cluster vibrations in Cr2O2,Cr2O3, and Cr2O4 Xiang KH, Pandey R, Recio JM, Francisco E, Newsam JM |
995 - 1003 |
Theoretical study of the double proton transfer in the CHX-XH center dot center dot center dot CHX-XH (X = O, S) complexes Jaque P, Toro-Labbe A |
1004 - 1008 |
Density functional study on phenol derivative-ammonia complexes in the gas phase Abkowicz-Bienko AJ, Latajka Z |
1009 - 1019 |
Three-dimensional photodissociation dynamics of rotational state selected methyl iodide Xie DQ, Guo H, Amatatsu Y, Kosloff R |
1020 - 1029 |
Effects of alkyl substituents on the excited states of naphthalene: Semiempirical study Mora-Diez N, Boyd RJ, Heard GL |
1030 - 1038 |
Initio investigation of XCH2CH2 and XCHCH3 radicals (X = F, Cl, Br) Zheng XM, Phillips DL |
1039 - 1046 |
Hartree-Fock and density functional theory ab initio calculation of optical rotation using GIAOs: Basis set dependence Cheeseman JR, Frisch MJ, Devlin FJ, Stephens PJ |
1047 - 1054 |
Experimental charge density of alpha-glycine at 23 K Destro R, Roversi P, Barzaghi M, Marsh RE |
1055 - 1063 |
Orientation of asymmetric top molecules in a uniform electric field: Calculations for species without symmetry axes Kong W, Bulthuis J |
1064 - 1074 |
Estimating heats of formation of hydrocarbon radicals by a combination of semiempirical calculation and family correlation with experimental values Ma XL, Schobert HH |
1075 - 1077 |
Comment on "Fluorescence of antiaromatic systems: An experimental and theoretical study of 1,3,5-tri-tert-butylpentalene" Bearpark MJ, Robb MA |