pith. sign in

arxiv: 0708.1471 · v4 · submitted 2007-08-10 · ❄️ cond-mat.mes-hall · hep-ph· hep-th· nucl-th

The Schwinger mechanism and graphene

classification ❄️ cond-mat.mes-hall hep-phhep-thnucl-th
keywords grapheneschwingermechanismelectricfermionsfieldmasslesspossible
0
0 comments X p. Extension
read the original abstract

The Schwinger mechanism, the production of charged particle-antiparticle pairs in a macroscopic external electric field, is derived for 2+1 dimensional theories. The rate of pair production per unit area for four species of massless fermions, with charge $q$, in a constant electric field $E$ is given by $ \pi^{-2} \hbar^{-3/2} \tilde{c}^{-1/2} (q E)^{3/2} $ where $\tilde{c}$ is the speed of light for the two-dimensional system. To the extent undoped graphene behaves like the quantum field-theoretic vacuum for massless fermions in 2+1 dimensions, the Schwinger mechanism should be testable experimentally. A possible experimental configuration for this is proposed. Effects due to deviations from this idealized picture of graphene are briefly considered. It is argued that with present day samples of graphene, tests of the Schwinger formula may be possible.

This paper has not been read by Pith yet.

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Forward citations

Cited by 1 Pith paper

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Classical constant electric fields and the Schwinger effect in de Sitter

    hep-ph 2025-08 unverdicted novelty 6.0

    Constant electric fields in de Sitter require a tachyonic photon mass ~H, yielding finite positive Schwinger currents for massless fermions and scalars after on-shell renormalization.