Multiplet Effects in the Quasiparticle Band Structure of the Anderson Model
arXiv:cond-mat/9411087 · doi:10.1103/PhysRevB.51.6167
Abstract
In this paper, we examine the mean field electronic structure of the Anderson lattice model in a slave boson approximation, which should be useful in understanding the physics of correlated metals with more than one f electron per site such as uranium-based heavy fermion superconductors. We find that the multiplet structure of the ion acts to quench the crystal field splitting in the quasiparticle electronic structure. This is consistent with experimental observations in such metals as .
9 pages, revtex, 3 uuencoded postscript figures attached at end
Cited by in corpus (8)
- Rotationally-invariant slave-boson formalism and momentum dependence of the quasiparticle weight
- Theory of Quasi-Universal Ratio of Seebeck Coefficient to Specific Heat in Zero-Temperature Limit in Correlated Metals
- Formation of heavy quasiparticle state in two-band Hubbard model
- Theoretical Uncertainties in Gamma_sl(b->u)
- Calculation of Effective Coulomb Interaction for , , and
- Kondo engineering : from single Kondo impurity to the Kondo lattice
- Interplay of crystal field structures with configuration to heavy fermions
- Non-factorizable terms, heavy quark masses, and semileptonic decays of D and B mesons