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Mulliken charge-transfer integral

A plane wave basis set with an orbital cutoff distance of 3.9 A was used. All-electron calculations and a double numerical basis set with polarization functions (DNP) were employed. Wave function integration in reciprocal space was performed via fine grid sampling of k points with a separation of 0.02 A . For the calculation of the density of states (DOS), a 5 X 8 X 3 Monkhorst-Pack grid was used. Charge transfer was calculated based on the Mulliken Population Analysis (MPA) (Mulliken 1955). [Pg.1371]

When the fiillerene was allowed to relax, conductance is reduced drastically. Only the LUMO orbital preserves its extended character, while the rest of the orbitals become localized at the interfaces. A Mulliken population analysis and the integration of the local density of states show that the excess transferred charge ( 3.3 e) concentrates mostly at the interface hexagons. Such a finding confirms that the details of the interactions between the metal-molecule contacts are the most important factors which determine the transport properties of the molecular bridge. [Pg.115]


See other pages where Mulliken charge-transfer integral is mentioned: [Pg.2]    [Pg.2]    [Pg.360]    [Pg.208]    [Pg.437]    [Pg.34]    [Pg.162]    [Pg.701]    [Pg.188]   


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