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Potentials particle-hole scattering

Here, we use short-hand notation 1 = (fi, q) etc. W is a screened potential, and the kernel lQri,cr2 is a two-particle propagator. In the case of multiple electron-hole scattering, the kernel (electron-hole propagator) is a product of electron and hole time-ordered Green functions... [Pg.180]

See other pages where Potentials particle-hole scattering is mentioned: [Pg.115]    [Pg.65]    [Pg.68]    [Pg.70]    [Pg.84]    [Pg.105]    [Pg.112]    [Pg.114]    [Pg.300]    [Pg.88]    [Pg.122]    [Pg.209]    [Pg.40]    [Pg.164]    [Pg.372]    [Pg.538]    [Pg.216]    [Pg.190]    [Pg.215]    [Pg.255]    [Pg.215]    [Pg.101]    [Pg.195]    [Pg.382]    [Pg.32]    [Pg.10]    [Pg.70]    [Pg.357]    [Pg.142]    [Pg.177]   
See also in sourсe #XX -- [ Pg.112 , Pg.113 ]



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