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Lead hopping, techniques

The summation over n is eliminated by the projection operator P and its complementary projection operator Q = I — P. The operator P projects to the IV-electron states with Nr electrons in the R-system. By acting on the states of eq. (1.227) it cuts off all the terms with electron distributions different from the required one. The general technique with the projection operator P in the previous section leads to the effective Hamiltonian with the intersubsystem electron hopping Wr projected out ... [Pg.81]

See other pages where Lead hopping, techniques is mentioned: [Pg.417]    [Pg.93]    [Pg.123]    [Pg.392]    [Pg.80]    [Pg.133]    [Pg.710]    [Pg.322]    [Pg.341]    [Pg.58]    [Pg.323]    [Pg.139]    [Pg.369]    [Pg.322]    [Pg.265]    [Pg.323]    [Pg.230]    [Pg.340]    [Pg.484]    [Pg.45]    [Pg.224]    [Pg.168]    [Pg.485]    [Pg.499]    [Pg.1518]    [Pg.251]    [Pg.258]    [Pg.265]    [Pg.137]    [Pg.387]    [Pg.728]    [Pg.280]    [Pg.72]    [Pg.465]    [Pg.375]    [Pg.168]   
See also in sourсe #XX -- [ Pg.417 ]



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Hops

Lead hopping

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