Vacancies in Graphene : Dirac Physics and Fractional Vacuum Charges

TL;DR

This paper explores how vacancies in graphene induce fractional charges and zero energy states, linking them to Dirac physics and topological phenomena, thus providing a platform for studying quantum electrodynamics features without gauge field coupling.

Contribution

It introduces a continuous Dirac model connecting vacancy-induced zero modes to vacuum fractional charge and parity anomaly, using chiral boundary conditions and relating vacancy physics to edge state phenomena.

Findings

Vacancies induce localized fractional charges in graphene.

Zero energy states are linked to parity anomaly and index theorem.

Vacancy physics mimics features of 2+1 quantum electrodynamics.

Abstract

The study of vacancies in graphene is a topic of growing interest. A single vacancy induces a localized stable charge of order unity interacting with other charges of the conductor through an unscreened Coulomb potential. It also breaks the symmetry between the two triangular graphene sublattices hence inducing zero energy states at the Dirac points. Here we show the fractional and pseudo-scalar nature of this vacancy charge. A continuous Dirac model is presented which relates zero modes to vacuum fractional charge and to a parity anomaly. This relation constitutes an Index theorem and is achieved by using particular chiral boundary conditions, which map the vacancy problem onto edge state physics. Vacancies in graphene thus allow to realize prominent features of $2+1$ quantum electrodynamics but without coupling to a gauge field. This essential difference makes vacancy physics relatively easy to implement and an interesting playground for topological switching.