Filling-enforced Kondo semimetals in two-dimensional non-symmorphic crystals
arXiv:1609.04023 · doi:10.1103/PhysRevB.96.081105
Abstract
We study the competition between Kondo screening and frustrated magnetism on the non-symmorphic Shastry-Sutherland Kondo lattice at a filling of two conduction electrons per unit cell. A previous analysis of this model identified a set of gapless partially Kondo screened phases intermediate between the Kondo-destroyed paramagnet and the heavy Fermi liquid. Based on crystal symmetries, we argue that (i)~both the paramagnet and the heavy Fermi liquid are {\it semimetals} protected by a glide symmetry; and (ii)~partial Kondo screening breaks the symmetry, removing this protection and allowing the partially-Kondo-screened phase to be deformed into a Kondo insulator via a Lifshitz transition. We confirm these results using large- mean field theory and then use non-perturbative arguments to derive a generalized Luttinger sum rule constraining the phase structure of 2D non-symmorphic Kondo lattices beyond the mean-field limit.
5 pages, 3 figures + Supplemental Material 2 pages
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- Quantum Monte Carlo Simulation of Frustrated Kondo Lattice Models
- Topological Kondo semimetal and insulator in AB-stacked heterobilayer transition metal dichalcogenides
- Topological phases of non-symmorphic crystals : Shastry-Sutherland lattice at integer filling
- Topological Kondo semimetals emulated in hetero-bilayer transition metal dichalcogenides