Electron liquid state in the symmetric Anderson lattice
arXiv:2103.07359 · doi:10.1038/s41598-021-85317-z
Abstract
Using mean field approach, we provide analytical and numerical solution of the symmetric Anderson lattice for arbitrary dimension at half filling. The symmetric Anderson lattice is equivalent to the Kondo lattice, which makes it possible to study the behavior of an electron liquid in the Kondo lattice. We have shown that, due to hybridization (through an effective field due to localized electrons) of electrons with different spins and momenta and , the gap in the electron spectrum opens at half filling. Such hybridization breaks the conservation of the total magnetic momentum of electrons, the spontaneous symmetry is broken. The state of electron liquid is characterized by a large Fermi surface. A gap in the spectrum is calculated depending on the magnitude of the on-site Coulomb repulsion and value of s-d hybridization for the chain, as well as for square and cubic lattices. Anomalous behavior of the heat capacity at low temperatures in the gapped state, which is realized in the symmetric Anderson lattice, was also found.
arXiv comment8 pages, 6 figures
References in corpus (7)
- Kondo Insulators Modeled by the One Dimensional Anderson Lattice: A Numerical Renormalization Group Study
- Exactly Solvable Kondo Lattice Model in Anisotropic Limit
- Spontaneous breaking of time-reversal symmetry in topological superconductors
- Spontaneous breaking of time-reversal symmetry in topological insulators
- An On-Site Density Matrix Description of the Extended Falicov--Kimball Model at Finite Temperatures
- Mott transition in two-band fermion model with on-site Coulomb repulsion
- Exactly solvable 2D topological Kondo lattice model