Abstract
Abstract
We study the Kondo alloy model on a square lattice using dynamical mean-field theory for Kondo substitution and disorder effects, together with static mean-field approximations. We computed and analyzed photoemission properties as a function of electronic filling n
c
, Kondo impurity concentration x, and strength of Kondo temperature T
K. We provide a complete description of the angle resolved photoemission spectroscopy (ARPES) signals expected in the paramagnetic (PM) Kondo phases. By analyzing the Fermi surface (FS), we observe the Lifshitz-like transition predicted previously for strong T
K at x = n
c
and we discuss the evolution of the dispersion from the dense coherent to the dilute Kondo regimes. At smaller T
K, we find that this transition marking the breakdown of coherence at x = n
c
becomes a crossover. However, we identify another transition at a smaller concentration x
⋆ where the effective mass continuously vanishes. x
⋆ separates the one-branch and the two-branches ARPES dispersions characterizing respectively dilute and dense Kondo PM regimes. The x − T
K phase diagrams are also described, suggesting that the transition at x
⋆ might be experimentally observable since magnetically ordered phases are stabilized at much lower T
K. FS reconstructions in antiferromagnetic and ferromagnetic phases are also discussed.
Funder
Deutsche Forschungsgemeinschaft
Agence Nationale de la Recherche
Subject
General Physics and Astronomy
Cited by
1 articles.
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