Theory of a quantum critical phenomenon in a topological insulator: (3+1)-dimensional quantum electrodynamics in solids
arXiv:1205.2427 · doi:10.1103/PhysRevB.86.165127
Abstract
We study theoretically the quantum critical phenomenon of the phase transition between the trivial insulator and the topological insulator in (3+1) dimensions, which is described by a Dirac fermion coupled to the electromagnetic field. The renormalization group (RG) equations for the running coupling constant α, the speed of light c and electron v are derived. The almost exact analytic solutions to these RG equations are obtained to reveal that (i) c and v approach to the common value with combination c^2v being almost unrenormalized, (ii) the RG flow of αis the same as that of usual QED with c^3 being replaced by c^2v, and (iii) there are two crossover momentum/energy scales separating three regions of different scaling behaviors. The dielectric and magnetic susceptibilities, angle-resolved photoemission spectroscopy (ARPES), and the behavior of the gap are discussed from this viewpoint.
6 pages, 4 figures
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- Bulk contributions to the Casimir interaction of Dirac materials
- Superconductivity from piezoelectric interactions in Weyl semimetals
- Yukawa-Lorentz symmetry of interacting non-Hermitian birefringent Dirac fermions
- Tilted Dirac superconductor at quantum criticality: Restoration of Lorentz symmetry
- Yukawa-Lorentz Symmetry of Tilted Non-Hermitian Dirac Semimetals at Quantum Criticality
- Re-assessing special aspects of Dirac fermions in presence of Lorentz-symmetry violation
- Conformal anomaly and helicity effects in kinetic theory via scale-dependent coupling
- Renormalization of fermion velocity in finite temperature QED_{3}
- Disordered non-Fermi liquid fixed point for two-dimensional metals at Ising-nematic quantum critical points
- SUSY QED with Lorentz-asymmetric fermionic matter and a glance at the electron's EDM