219 - 223 |
Mediation of ultrafast electron transfer in biological systems by conical intersections Worth GA, Cederbaum LS |
224 - 230 |
Theoretical study of ZnO (10(1)over-bar-0) and Cu/ZnO (10(1)over-bar-0) surfaces Beltran A, Andres J, Calatayud M, Martins JBL |
231 - 236 |
Fabrication, characterization and Raman study of TiO2 nanowire arrays prepared by anodic oxidative hydrolysis of TiCl3 Lei Y, Zhang LD, Fan JC |
237 - 240 |
Skyrmion models for three-dimensional aromaticity in deltahedral boranes King RB |
241 - 246 |
Conductivity of fullerene-doped optical glasses Zeng HP, Sun ZR, Segawa Y, Lin FC, Mao S, Xu ZZ |
247 - 253 |
Novel method of estimating proton-proton dipolar couplings to aid the analyses of NMR spectra of oriented molecules using two-dimensional inverse experiment Vivekanandan S, Suryaprakash N |
254 - 262 |
Heterodyne detected transient grating spectroscopy in resonant and non-resonant systems using a simplified diffractive optics method Xu QH, Ma YZ, Fleming GR |
263 - 268 |
Deduction of the conformation of short chain luminescent conjugated polymers from single molecule photophysics White JD, Hsu JH, Fann WS, Yang SC, Pern GY, Chen SA |
269 - 276 |
Experimental observation of nonlinear circular dichroism in a pump-probe experiment Mesnil H, Schanne-Klein MC, Hache F, Alexandre M, Lemercier G, Andraud C |
277 - 284 |
Infrared water recombination lasers Michael EA, Keoshian CJ, Wagner DR, Anderson SK, Saykally RJ |
285 - 290 |
Non Franck-Condon effects in the photoionization of molecular nitrogen to the N-2(+) A (2)Pi(u) state in the 19-34 eV photon energy region Riu JRI, Karawajczyk A, Stankiewicz M, Franzen KY, Winiarczyk P, Veseth L |
291 - 296 |
Photochemical dynamics of Mg+-acetaldehyde: C-H vs. C-C bond activation pathways Lu WY, Kleiber PD |
297 - 302 |
Internal-state distribution and polarization in nascent NO X-2 Pi from the photodissociation of C6H5NO Li YM, Sun JL, Han KL, He GZ |
303 - 307 |
The stabilization of active oxygen species by Pt supported on TiO2 Einaga H, Ogata A, Futamura S, Ibusuki T |
308 - 316 |
Resonance Raman and density functional study of the A-band absorption of C5H5[WC equivalent to CPh]O-2 Cheng YF, Phillips DL, He GZ, Che CM, Chi Y |
317 - 322 |
Emission of SH radicals in solid krypton: mixed quantum-classical molecular dynamics simulations Firsov DA, Grigorenko BL, Nemukhin AV, Khriachtchev LY, Rasanen MO |
323 - 328 |
Energy functional of the one-particle reduced density matrix: a geminal approach Mazziotti DA |
329 - 336 |
Above threshold dissociation of LiNa+: monitoring an avoided crossing with femtosecond spectroscopy Magnier S, Toniolo A |
337 - 344 |
NMR implementation of a building block for scalable quantum computation Chang DE, Vandersypen LMK, Steffen M |
345 - 352 |
The change of picture contribution to relativistic corrections to second-order properties Turski P, Sadlej AJ |
353 - 360 |
Direct ab initio molecular dynamics study of the protonation of nitric acid Ishikawa Y, Binning RC |
361 - 366 |
A new measure of hydrogen bonding strength - ab initio and atoms in molecules studies Grabowski SJ |
367 - 374 |
A Gaussian-3 investigation of N-7 isomers Wang X, Tian AM, Wong NB, Law CK, Li WK |
375 - 384 |
Size-consistent wave functions for bond-breaking: the equation-of-motion spin-flip model Krylov AI |
385 - 388 |
Kinematic rotations in RRKM theory Bonnet L, Rayez JC |
389 - 397 |
Partial multidimensional grid generation method for efficient calculation of nuclear wavefunctions Iordanov T, Billeter SR, Webb SP, Hammes-Schiffer S |
398 - 406 |
Possibility of the magnetic field effect on the thermal decomposition of N2O: molecular dynamics simulation Takahashi O, Kurushima N, Kawano A, Saito K |
407 - 413 |
Ab initio g-tensor calculations of hydrogen bond effects on a nitroxide spin label Engstrom M, Owenius R, Vahtras O |