The band structure of aluminum has been calculated self-consistently with the use of the Kohn-Sham-Gaspar local exchange potential and the linear combination of Gaussian orbitals method. The resulting band structure, using a basis set of 28 contracted Gaussian-type orbitals, is in excellent agreement with the previous work of Singhal and Callaway in which a basis set of 60 uncontracted Gaussian functions was used. After projection of the bulk bands onto the two-dimensional (001) surface Brillouin zone, surface states and resonances have been calculated along the Δ line with the use of the Green's-function formalism. At point Γ, the surface state is located 2.92 eV below EF, in excellent agreement with the experimental result, 2.8±{}0.2 eV below EF. In addition, a resonance is found 0.7 eV below EF with a half-width of 0.4 eV, hitherto interpreted only as Fermi edge intensity. From the midpoint of the Δ axis moving onward up to the Fermi energy, the observed main peak is attributed to surface resonances.
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M. Seel (1983) studied this question.
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