The Heisenberg-Euler effective action in slowly varying electric field inhomogeneities of Lorentzian shape

Abstract

We use a locally constant field approximation (LCFA) to study the one-loop Heisenberg-Euler effective action in a particular class of slowly varying inhomogeneous electric fields of Lorentzian shape with $0\le d\le 4$ inhomogeneous directions. We show that for these fields, the LCFA of the Heisenberg-Euler effective action can be represented in terms of a single parameter integral, with the constant field effective Lagrangian with rescaled argument as integration kernel. The imaginary part of the Heisenberg-Euler effective action contains information about the instability of the quantum vacuum towards the formation of a state with real electrons and positrons. Here, we in particular focus on the dependence of the instantaneous vacuum decay rate on the dimension $d$ of the field inhomogeneity. Specifically for weak fields, we find an overall parametric suppression of the effect with $(E_0/E_{\mathrm{cr}}{)}^{d/2}$, where $E_0$ is the peak field strength of the inhomogeneity and $E_{\mathrm{cr}}$ the critical electric field strength.

11 pages; some clarifications added, matches journal version

References in corpus (4)

• Worldline Instantons II: The Fluctuation Prefactor
• The Schwinger mechanism revisited
• An Addendum to the Heisenberg-Euler effective action beyond one loop
• Pair production from residues of complex worldline instantons

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