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QED Fermions in a noisy magnetic field background
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QED Fermions in a noisy magnetic field background
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We consider the effects of a noisy magnetic field background over the fermion propagator in QED, as an approximation to the spatial inhomogeneities that would naturally arise in certain physical scenarios, such as heavy-ion collisions or the quark-gluon plasma in the early stages of the evolution of the Universe. We considered a classical, finite and uniform average magnetic field background $\langle\mathbf{B}(\mathbf{x})\rangle = \mathbf{B}$, subject to white-noise spatial fluctuations with auto-correlation of magnitude $\Delta_B$. By means of the Schwinger representation of the propagator in the average magnetic field as a reference system, we used the replica formalism to study the effects of the magnetic noise in the form of renormalized quasi-particle parameters, leading to an effective charge and an effective refraction index, that depend not only on the energy scale, as usual, but also on the magnitude of the noise $\Delta_B$ and the average field $\mathbf{B}$.
Forward citations
Cited by 3 Pith papers
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QED vertex and anomalous magnetic moment in the presence of a magnetic field
In a background magnetic field the QED vertex decomposes into parallel and transverse structures even at tree level; the one-loop transverse anomalous magnetic moment is complex, forbids LLL-to-LLL transitions, and is...
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QED vertex and anomalous magnetic moment in the presence of a magnetic field
A one-loop QED calculation finds a magnetic-field-induced transverse anomalous magnetic moment with Landau-level selection rules, zero LLL-to-LLL strength, and opposite signs for reverse transitions.
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QED vertex and anomalous magnetic moment in the presence of a magnetic field
In a magnetic field the QED fermion–photon vertex already splits at tree level into longitudinal and transverse pieces, and one-loop corrections generate direction-dependent anomalous magnetic moments with selection r...
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