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This paper advances the theoretical framework of Quantum Electrodynamics by treating intense laser fields as dynamic quantum coherent states rather than static classical backgrounds. By incorporating functional integrals over these field histories, it derives an effective Maxwell equation that accounts for vacuum polarization and photon fluctuations alongside coherent-field dynamics. This formalism represents a significant step toward unifying high-intensity optics with fundamental quantum theory without relying on external approximations.
Coherent-field QED transitions based on coherent-state boundary conditions
arXiv:2512.21122v4 Announce Type: replace-cross Abstract: We develop a coherent-field formulation of quantum electrodynamics (QED) based on coherent-state boundary conditions, in which laser fields are represented by asymptotic coherent states rather than by prescribed classical background fields. Starting from coherent-state boundary conditions and the displacement-operator formalism, we construct operator and path-integral descriptions of transitions between distinct electromagnetic coherent states. This formulation provides a coherent-field extension of conventional background-field QED and incorporates the quantum dynamics of the coherent field itself. The corresponding path-integral representation contains a functional integral over coherent-field histories in addition to the usual functional integral over quantum fluctuations, thereby extending the conventional background-field description. The resulting path-integral representation naturally leads to an effective action for the stationary coherent-field configuration. The corresponding saddle-point condition yields an effective Maxwell equation containing contributions from vacuum polarization, photon fluctuations, and coherent-field fluctuations. In the limit where the latter two contributions vanish, the formalism reduces to the conventional Heisenberg-Euler description.
Abstract:We develop a coherent-field formulation of quantum electrodynamics (QED) based on coherent-state boundary conditions, in which laser fields are represented by asymptotic coherent states rather than by prescribed classical background fields. Starting from coherent-state boundary conditions and the displacement-operator formalism, we construct operator and path-integral descriptions of transitions between distinct electromagnetic coherent states. This formulation provides a coherent-field extension of conventional background-field QED and incorporates the quantum dynamics of the coherent field itself. The corresponding path-integral representation contains a functional integral over coherent-field histories in addition to the usual functional integral over quantum fluctuations, thereby extending the conventional background-field description. The resulting path-integral representation naturally leads to an effective action for the stationary coherent-field configuration. The corresponding saddle-point condition yields an effective Maxwell equation containing contributions from vacuum polarization, photon fluctuations, and coherent-field fluctuations. In the limit where the latter two contributions vanish, the formalism reduces to the conventional Heisenberg-Euler description.
Plasma Physics (physics.plasm-ph); High Energy Physics - Phenomenology (hep-ph); Optics (physics.optics); Quantum Physics (quant-ph)
arXiv:2512.21122 [physics.plasm-ph]
(or arXiv:2512.21122v4 [physics.plasm-ph] for this version)
https://doi.org/10.1016/j.aop.2026.170660 DOI(s) linking to related resources
Full text under the publisher's open licence · 179 words
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