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This paper presents a fully quantized theoretical framework for nonlinear Compton scattering, specifically addressing pump depletion and back-action effects using exact quantum-Volkov states within Fock-state ladders. By incorporating squeezed coherent light parameters, the study offers new insights into how photon-number fluctuations influence high-energy emission spectra in extreme laser-matter interaction regimes.
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Nonlinear Compton scattering in a quantized pump field

arXiv1 min read

arXiv:2608.06289v1 Announce Type: new Abstract: We develop a fully quantized theory of nonlinear Compton scattering driven by a single-mode quantum field. Exact quantum-Volkov states retain pump depletion, back-action, and final-state correlations through displaced or squeezed-displaced Fock-state ladders. A finite Fock-state pump produces discrete photon-transfer edges and a terminal spectral cutoff. In the bright, weakly depleted regime, the exact theory reduces to a Wigner-function weighted-average of scattering probabilities evaluated at fixed complex field amplitudes, with ordinary and generalized Bessel functions describing the harmonic structure for circular and linear polarization, respectively. For squeezed coherent light, the squeezing angle controls the high-energy emission through photon-number fluctuations.

Abstract:We develop a fully quantized theory of nonlinear Compton scattering driven by a single-mode quantum field. Exact quantum-Volkov states retain pump depletion, back-action, and final-state correlations through displaced or squeezed-displaced Fock-state ladders. A finite Fock-state pump produces discrete photon-transfer edges and a terminal spectral cutoff. In the bright, weakly depleted regime, the exact theory reduces to a Wigner-function weighted-average of scattering probabilities evaluated at fixed complex field amplitudes, with ordinary and generalized Bessel functions describing the harmonic structure for circular and linear polarization, respectively. For squeezed coherent light, the squeezing angle controls the high-energy emission through photon-number fluctuations.

arXiv:2608.06289 [quant-ph]

(or arXiv:2608.06289v1 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2608.06289 Focus to learn more arXiv-issued DOI via DataCite (pending registration)

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Full text under the publisher's open licence · 189 words

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