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LCGTO-LDF method

Table 2 clearly shows that the pronounced increase in intensity observed for bands C-E vs bands A-B is related to changes in photoionization cross-sections. Bands F-I were assigned to Ugand-based orbital ionizations on the basis of comparison with the UPS spectrum of PMes. Bancroft and coworkers have attributed bands A and B to ionization from orbitals with Au—C and Au—P characters, respectively, on the basis of Xa calculations and comparison with the spectrum of HgMe2. More recent calculations using the relativistic LCGTO-LDF method have provided more details about orbital compositions in AuMePMes (Table 3). They have also indicated that the role of Au6p orbitals in bonding is minimal. Table 2 clearly shows that the pronounced increase in intensity observed for bands C-E vs bands A-B is related to changes in photoionization cross-sections. Bands F-I were assigned to Ugand-based orbital ionizations on the basis of comparison with the UPS spectrum of PMes. Bancroft and coworkers have attributed bands A and B to ionization from orbitals with Au—C and Au—P characters, respectively, on the basis of Xa calculations and comparison with the spectrum of HgMe2. More recent calculations using the relativistic LCGTO-LDF method have provided more details about orbital compositions in AuMePMes (Table 3). They have also indicated that the role of Au6p orbitals in bonding is minimal.

See other pages where LCGTO-LDF method is mentioned: [Pg.213]    [Pg.203]    [Pg.108]    [Pg.240]    [Pg.256]    [Pg.696]    [Pg.63]    [Pg.213]    [Pg.203]    [Pg.108]    [Pg.240]    [Pg.256]    [Pg.696]    [Pg.63]    [Pg.421]    [Pg.1441]    [Pg.641]   
See also in sourсe #XX -- [ Pg.108 ]

See also in sourсe #XX -- [ Pg.108 ]




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LDF method

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