Directed molecular states

E. Directed molecular states. Can you build a wave-packet of rotational states, giving a different amplitude to different m states, such that the wave-packet will be initially localized in a given direction and will then rotate as the hand of a... 

Calculations for Ceo in the LDA approximation [62, 60] yield a narrow band (- 0.4 0.6 eV bandwidth) solid, with a HOMO-LUMO-derived direct band gap of - 1.5 eV at the X point of the fee Brillouin zone. The narrow energy bands and the molecular nature of the electronic structure of fullerenes are indicative of a highly correlated electron system. Since the HOMO and LUMO levels both have the same odd parity, electric dipole transitions between these levels are symmetry forbidden in the free Ceo moleeule. In the crystalline solid, transitions between the direct bandgap states at the T and X points in the cubic Brillouin zone arc also forbidden, but are allowed at the lower symmetry points in the Brillouin zone. The allowed electric dipole... 

Dissociative chemisorption was considered to be either direct, when the incoming diatomic molecule has sufficient energy to surmount the barrier without being trapped into the molecular state, or indirect, when it passes via the molecular (precursor) state into the dissociated state. If the dissociated state is not immediately equilibrated with the lattice, the fragments will move across... 

Hence, for modern FRET and FLIM techniques in Molecular Biology and Biochemistry it is important to keep the enthusiasm for the in situ technique, yielding unprecedented rich information on molecular states in live cells, and to keep the advantages of easy labeling techniques, modern microscopes and automated data processing. However, we need to educate the new generations of FRET scientists in the theoretical background of the technique, how it should be done correctly, and what the sources of errors are. Only then it will be clear that FRET-(FLIM) is a very direct, robust, extremely sensitive, and reliable technique. 

II electronic states, 634-640 theoretical background, 625-626 triatomic molecules, 611-615 pragmatic models, 620-621 Ab initio multiple spawning (AIMS) conical intersection location, 491-492 direct molecular dynamics, 411-414 theoretical background, 360-361 Adiabatic approximation geometric phase theory ... 

Asymptotic analysis, electronic states, triatomic quantum reaction dynamics, 317—318 Azulene molecule, direct molecular dynamics, complete active space self-consistent field (CASSCF) technique, 408-410... 

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