Higher-order renormalization of graphene many-body theory
J. Gonzalez

TL;DR
This paper demonstrates that the many-body theory of graphene with Coulomb interactions is renormalizable in the ladder approximation, allowing for consistent calculations of physical quantities and identifying a critical interaction strength for chiral symmetry breaking.
Contribution
It provides a detailed proof of the renormalizability of graphene's many-body theory beyond the large-N approximation using ladder diagrams, and computes the critical coupling for gap opening.
Findings
Graphene many-body theory is renormalizable in the ladder approximation.
A scale-invariant anomalous dimension is computed to all orders.
The critical coupling for chiral symmetry breaking matches previous gap equation results.
Abstract
We study the many-body theory of graphene Dirac quasiparticles interacting via the long-range Coulomb potential, taking as a starting point the ladder approximation to different vertex functions. We test in this way the low-energy behavior of the electron system beyond the simple logarithmic dependence of electronic correlators on the high-energy cutoff, which is characteristic of the large-N approximation. We show that the graphene many-body theory is perfectly renormalizable in the ladder approximation, as all higher powers in the cutoff dependence can be absorbed into the redefinition of a finite number of parameters (namely, the Fermi velocity and the weight of the fields) that remain free of infrared divergences even at the charge neutrality point. We illustrate this fact in the case of the vertex for the current density, where a complete cancellation between the cutoff dependences…
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