Lifshitz Transitions in Magnetic Phases of the Periodic Anderson Model
arXiv:1507.04067 · doi:10.7566/JPSJ.84.094702
Abstract
We investigate the reconstruction of a Fermi surface, which is called a Lifshitz transition, in magnetically ordered phases of the periodic Anderson model on a square lattice with a finite Coulomb interaction between f electrons. We apply the variational Monte Carlo method to the model by using the Gutzwiller wavefunctions for the paramagnetic, antiferromagnetic, ferromagnetic, and charge-density-wave states. We find that an antiferromagnetic phase is realized around half-filling and a ferromagnetic phase is realized when the system is far away from half-filling. In both magnetic phases, Lifshitz transitions take place. By analyzing the electronic states, we conclude that the Lifshitz transitions to large ordered-moment states can be regarded as itinerant-localized transitions of the f electrons.
9 pages, 13 figures, to be published in J. Phys. Soc. Jpn
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- Antiferromagnetic Phases of the Kondo Lattice
- Enhanced Spin-Orbit Coupling in a Correlated Metal
- Quasiparticle Band Structure and Spin Excitation Spectrum of the Kondo Lattice
- Variational Wavefunction for the Periodic Anderson Model with Onsite Correlation Factors
- Degenerate orbital effect in a three orbital periodic Anderson model
- Magnetic phases of the periodic Anderson model in two dimensions