Correlation and transport phenomena in topological nodal-loop semimetals
arXiv:1609.05529 · doi:10.1103/PhysRevB.95.075426
Abstract
We study the unique physical properties of topological nodal-loop semimetals protected by the coexistence of time-reversal and inversion symmetries with negligible spin-orbit coupling. We argue that strong correlation effects occur at the surface of such systems for relatively small Hubbard interaction , due to the narrow bandwidth of the "drumhead" surface states. In the Hartree-Fock approximation, at small we obtain a surface ferromagnetic phase through a continuous quantum phase transition characterized by the surface-mode divergence of the spin susceptibility, while the bulk states remain very robust against local interactions and remain non-ordered. At slightly increased interaction strength, the system quickly changes from a surface ferromagnetic phase to a surface charge-ordered phase through a first-order transition. When Rashba-type spin-orbit coupling is applied to the surface states, a canted ferromagnetic phase occurs at the surface for intermediate values of . The quantum critical behavior of the surface ferromagnetic transition is nontrivial in the sense that the surface spin order parameter couple to Fermi-surface excitations from both surface and bulk states. This leads to unconventional Landau damping and consequently a naïve dynamical critical exponent when the Fermi level is close to the bulk nodal energy. We also show that, already without interactions, quantum oscillations arise due to bulk states, despite the absence of a Fermi surface when the chemical potential is tuned to the energy of the nodal loop. The bulk magnetic susceptibility diverges logarithmically whenever the nodal loop exactly overlaps with a quantized magnetic orbit in the bulk Brillouin zone. These correlation and transport phenomena are unique signatures of nodal loop states.
8+7 pages, 7 figures, submitted to PRB
References in corpus (8)
- Superconducting proximity effect and Majorana fermions at the surface of a topological insulator
- Weyl semimetal phase in non-centrosymmetric transition metal monophosphides
- Topological Node-Line Semimetal in Three Dimensional Graphene Networks
- Strong spin-orbit splitting on Bi surfaces
- Low energy effective theory of Fermi surface coupled with U(1) gauge field in 2+1 dimensions
- Weyl semimetals from noncentrosymmetric topological insulators
- Dimensional crossover in topological matter: Evolution of the multiple Dirac point in the layered system to the flat band on the surface
- Universal phase diagrams for the quantum spin Hall systems
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