Van Hove singularities and excited-state quantum phase transitions in graphene-like microwave billiards

Abstract

We discuss solutions of an algebraic model of the hexagonal lattice vibrations, which point out interesting localization properties of the eigenstates at van Hove singularities (vHs), whose energies correspond to Excited-State Quantum Phase Transitions (ESQPT). We show that these states form stripes oriented parallel to the zig-zag direction of the lattice, similar to the well-known edge states found at the Dirac point, however the vHs-stripes appear in the bulk. We interpret the states as lines of cell-tilting vibrations, and inspect their stability in the large lattice-size limit. The model can be experimentally realized by superconducting 2D microwave resonators containing triangular lattices of metallic cylinders, which simulate finite-sized graphene flakes. Thus we can assume that the effects discussed here could be experimentally observed.

Excited-state quantum phase transitions

“…In particular, the n = 1 band contains two logarithmic divergences of the level density separated by the so-called Dirac point with vanishing level density [40]. In both lattice types, the wave functions ψ k (x i , y i ) of the eigenstates close to the ESQPT energies manifest some anomalous localization properties [41,238]. This is reminiscent of D = 0 systems with f = 1, for which anomalous spatial localization of eigenstates is also observed near ESQPT energies, but a possible deeper connection of these phenomena needs to be clarified.…”