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Quantum electron self-interaction in a strong laser field
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The quantum state of an electron in a strong laser field is altered if the interaction of the electron with its own electromagnetic field is taken into account. Starting from the Schwinger-Dirac equation, we determine the states of an electron in a plane-wave field with inclusion, at leading order, of its electromagnetic self-interaction. On the one hand, the electron states show a pure "quantum" contribution to the electron quasi-momentum, conceptually different from the conventional "classical" one arising from the quiver motion of the electron. On the other hand, the electron self-interaction induces a distinct dynamics of the electron spin, whose effects are shown to be measurable in principle with available technology.
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One loop Volkov propagator in the Lorentz class of gauges
The one-loop correction to the laser-induced mass shift in QED is gauge dependent, vanishing in Landau gauge where only vacuum renormalisation is needed.
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