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This research demonstrates how strong-field ionization driven by bright squeezed vacuum exhibits anomalous $I^{2/3}$ scaling in photoelectron momentum, contrasting with the linear response of coherent light sources. The study identifies field-amplitude saddle-point structures as the origin of this behavior and shows that photon-number resolution preserves quantum coherence to reveal parity-dependent modulations via time-domain interference. These findings establish longitudinal momentum transfer as a critical observable for encoding both photon statistics and field coherence in intense quantum optical regimes.
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Anomalous radiation pressure in strong-field ionization driven by quantum light

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arXiv:2608.15859v1 Announce Type: new Abstract: We show that in strong-field ionization driven by bright squeezed vacuum, the mean longitudinal photoelectron momentum scales with the mean incident intensity $I$ as $I^{2/3}$, rather than linearly as under coherent-light driving. This anomalous scaling originates from a field-amplitude saddle-point structure: nonlinear tunneling selects two dominant field amplitudes of equal magnitude and opposite sign from the broad quantum fluctuations. Tracing over the final photon state erases their relative-phase information, leaving their common magnitude to determine the field-dependent longitudinal momentum shift and its $I^{2/3}$ scaling. Photon-number resolution instead preserves this coherence, producing parity-dependent modulations of the longitudinal momentum transfer through time-domain double-slit interference between two field pathways separated by half a cycle. These results establish longitudinal momentum transfer as a distinct observable in strong-field quantum optics that encodes both the photon statistics and the field coherence of intense quantum light.

Abstract:We show that in strong-field ionization driven by bright squeezed vacuum, the mean longitudinal photoelectron momentum scales with the mean incident intensity $I$ as $I^{2/3}$, rather than linearly as under coherent-light driving. This anomalous scaling originates from a field-amplitude saddle-point structure: nonlinear tunneling selects two dominant field amplitudes of equal magnitude and opposite sign from the broad quantum fluctuations. Tracing over the final photon state erases their relative-phase information, leaving their common magnitude to determine the field-dependent longitudinal momentum shift and its $I^{2/3}$ scaling. Photon-number resolution instead preserves this coherence, producing parity-dependent modulations of the longitudinal momentum transfer through time-domain double-slit interference between two field pathways separated by half a cycle. These results establish longitudinal momentum transfer as a distinct observable in strong-field quantum optics that encodes both the photon statistics and the field coherence of intense quantum light.

arXiv:2608.15859 [quant-ph]

(or arXiv:2608.15859v1 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2608.15859 Focus to learn more arXiv-issued DOI via DataCite (pending registration)

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