Yukawa-Lorentz Symmetry of Tilted Non-Hermitian Dirac Semimetals at Quantum Criticality
Sergio Pino-Alarc\'on, Vladimir Juri\v{c}i\'c

TL;DR
This paper demonstrates that Yukawa-Lorentz symmetry can emerge at quantum critical points in tilted non-Hermitian Dirac semimetals, with tilt effects becoming irrelevant near the criticality, supported by epsilon expansion analysis.
Contribution
It shows that tilt terms in non-Hermitian Dirac Hamiltonians are irrelevant at the quantum critical point, extending the understanding of emergent Lorentz symmetry in open quantum systems.
Findings
Tilt term becomes irrelevant near the QCP.
Velocity anisotropy also becomes irrelevant at the QCP.
Predictions can be tested via quantum Monte Carlo simulations.
Abstract
Dirac materials, hosting linearly dispersing quasiparticles at low energies, exhibit an emergent Lorentz symmetry close to a quantum critical point (QCP) separating semimetallic state from a strongly-coupled gapped insulator or superconductor. This feature appears to be quite robust even in the open Dirac systems coupled to an environment, featuring non-Hermitian (NH) Dirac fermions: close to a strongly coupled QCP, a Yukawa-Lorentz symmetry emerges in terms of a unique terminal velocity for both the fermion and the bosonic order parameter fluctuations, while the system can either retain non-Hermiticity or completely decouple from the environment thus recovering Hermiticity as an emergent phenomenon. We here show that such a Yukawa-Lorentz symmetry can emerge at the quantum criticality even when the NH Dirac Hamiltonian includes a tilt term at the lattice scale. As we demonstrate by…
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Taxonomy
TopicsQuantum Mechanics and Non-Hermitian Physics · Topological Materials and Phenomena · Graphene research and applications
