2013
DOI: 10.1007/s00205-012-0609-1
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Construction of the Pauli–Villars-Regulated Dirac Vacuum in Electromagnetic Fields

Abstract: Abstract. Using the Pauli-Villars regularization and arguments from convex analysis, we construct solutions to the classical time-independent Maxwell equations in Dirac's vacuum, in the presence of small external electromagnetic sources. The vacuum is not an empty space, but rather a quantum fluctuating medium which behaves as a nonlinear polarizable material. Its behavior is described by a Dirac equation involving infinitely many particles. The quantum corrections to the usual Maxwell equations are nonlinear … Show more

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Cited by 16 publications
(24 citation statements)
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“…The complicated form of this expression is largely due to the greater number of regularising terms as compared to [11]. The response of the positive energy states is given by…”
Section: The Stability Of Homogeneous Systemsmentioning
confidence: 99%
See 1 more Smart Citation
“…The complicated form of this expression is largely due to the greater number of regularising terms as compared to [11]. The response of the positive energy states is given by…”
Section: The Stability Of Homogeneous Systemsmentioning
confidence: 99%
“…As we said, the regularisation used in (1) is not the only possible choice. Following [11], one can also consider the Pauli-Villars energy…”
Section: Introductionmentioning
confidence: 99%
“…The issue of the unidentified phase particularly concerns the so-called phenomenon of "vacuum polarization" as well as the dynamical description of pair creation processes for which only a few rigorous treatments are available; e.g., see [13] for vacuum polarization in the Hartree-Fock approximation for static external sources, [17] for adiabatic pair creation, and for a more fundamental approach the so-called "Theory of Causal Fermion Systems" [7,8,9], which is based on a reformulation of quantum electrodynamics by means of an action principle.…”
Section: Discussionmentioning
confidence: 99%
“…However, quantities such as the charge-current density depend manifestly on this unidentified phase. In particular, this concerns the so-called phenomenon of vacuum polarization but also the dynamical description of pair creation processes for which so far only a few rigorous treatments are available; see [GHLS13] for vacuum polarization in the Hartree-Fock approximation for static external sources and [DP07] for adiabatic pair creation. The involved degrees of freedom can be reduced further by imposing the Bogolyubov causality condition [BS59,(17.30)] or more or less equivalently by implementing second-quantized evolution maps between Fock spaces associated to space-like Cauchy hypersurfaces, which is the content of a follow-up work.…”
Section: Introductionmentioning
confidence: 99%