Abstract

The electronic properties of YbRh2Si2 are studied by means of band structure calculations based on thedensity functional theory within the LDA (local density approximation),LDA+U, and fully relativistic scheme. The 4f derived bands are studied within a relativisticframework which yields flat and spin–orbit split bands, and a correlated band method(LDA+U) that includes correlation corrections. In both cases the uppermost4f band is located roughly 150 meV below the Fermi energyEF, and hybridizes weakly with the dispersive Rh 4d bands and a Rh4dxy band that does not disperse perpendicular to the Rh layers. When weapplied the fully relativistic scheme, the 4f derived bands split intoj = 7/2 and 5/2 excitations due to spin–orbit coupling effects. Thef7/2 multiplet is locatedmuch closer to EF, hybridizing anisotropically with a Rh 4d derived conductionband. This mixing induces a non-integer occupation of the f levelsnf and hencereveals that YbRh2Si2 is a mixed-valence heavy fermion. The 4f electrons can be delocalized through the hybridization withconduction electrons. And the hybridization between f and conduction d electrons plays a importantrole in YbRh2Si2. The Fermi surface splits into three different non-touching sheets. There are two tinycylinder Fermi surfaces around Z points which are from the Rh 4d bands and the largerFermi surfaces are from the 4f derived bands.

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