Abstract

Band calculations for Ce compounds with the AuCu3_{3}-type crystal structure were carried out on the basis of dynamical mean field theory (DMFT). The auxiliary impurity problem was solved by a method named NCAf2f^{2}vc (noncrossing approximation including the f2f^{2} state as a vertex correction). The calculations take into account the crystal-field splitting, the spin-orbit interaction, and the correct exchange process of the f1f0,f2f^{1} \rightarrow f^{0},f^{2} virtual excitation. These are necessary features in the quantitative band theory for Ce compounds and in the calculation of their excitation spectra. The results of applying the calculation to CePd3_{3} and CeRh3_{3} are presented as the first in a series of papers. The experimental results of the photoemission spectrum (PES), the inverse PES, the angle-resolved PES, and the magnetic excitation spectra were reasonably reproduced by the first-principles DMFT band calculation. At low temperatures, the Fermi surface (FS) structure of CePd3_{3} is similar to that of the band obtained by the local density approximation. It gradually changes into a form that is similar to the FS of LaPd3_{3} as the temperature increases, since the 4f4f band shifts to the high-energy side and the lifetime broadening becomes large.}Comment: 12 pasges, 13 figure

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