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Core-Hole Spectrum in Xe and Surrounding Elements

The Fermi sea-correlation energy shift A% is-------1 fo —2 eV. From the experimental [Pg.37]

Equation (48) represents a rough estimate of the shift due to solid-state effects A d by subtracting the work function from the total shift. Our results for the atom-solid shift All agree quite well with the theoretical and semi-empirical results of Johansson and M rtensson83.  [Pg.38]

It is quite clear that when the gCK process reaches its maximum strength, the resulting shift idfR becomes a good deal larger than the normal static monopole relaxation shifts) f°. [Pg.39]

The renormalized second-order self-energy takes the form [Pg.40]

Higher order corrections are then included according to Eqs. (42) and (43). The TDAE part of the atomic dielectric response including the effect of the Hartree potential of a spectator 4d hole is taken into account by our choice of basis set  [Pg.41]

See other pages where Core-Hole Spectrum in Xe and Surrounding Elements is mentioned: [Pg.37]    [Pg.39]    [Pg.41]    [Pg.43]    [Pg.45]    [Pg.47]    [Pg.49]    [Pg.51]    [Pg.53]    [Pg.55]    [Pg.59]    [Pg.59]    [Pg.37]    [Pg.39]    [Pg.41]    [Pg.43]    [Pg.45]    [Pg.47]    [Pg.49]    [Pg.51]    [Pg.53]    [Pg.55]    [Pg.59]    [Pg.59]    [Pg.1]   


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Core hole

Element spectrum

Surround

Surrounding

Surroundings

Surroundings and

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