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This study establishes a universal scaling law for cooperative photon emission in atomic ensembles, demonstrating that geometric optical depth dictates the maximum emission rate across both ordered arrays and disordered clouds. The work unifies regimes from independent emission to the Dicke limit while clarifying how detector numerical aperture influences observed directional versus total emission rates. These findings provide fundamental bounds for many-body quantum optics experiments involving spatially extended systems.
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Optical depth dictates universal bounds on many-body decay in atomic ensembles

arXiv2 min read

arXiv:2604.24680v2 Announce Type: replace Abstract: Cooperative emission is well understood for idealized symmetric systems, but its fundamental limits in spatially extended, free-space ensembles remain an open question. Here, we derive a universal law for the scaling of the maximum photon emission rate with system size that unifies both ordered arrays and disordered atomic clouds in arbitrary dimensions at fixed density. We demonstrate that, for a fixed atomic density, the maximum emission rate scales universally as the product of the atom number and the system's geometric optical depth. The geometric optical depth differs from the result of the Beer-Lambert law at high density and encodes the dimensional scaling across all regimes from independent emission to the Dicke limit. Furthermore, we establish a scaling law for directional detection, revealing that the observed rate depends on the detector's numerical aperture: small apertures yield Dicke-like quadratic scaling, whereas large apertures recover our integrated universal bound. Our results establish optical depth as the parameter governing many-body cooperative emission in both ordered and disordered ensembles, and reveal that directional and total-emission scalings must be carefully distinguished in experimental settings.

Abstract:Cooperative emission is well understood for idealized symmetric systems, but its fundamental limits in spatially extended, free-space ensembles remain an open question. Here, we derive a universal law for the scaling of the maximum photon emission rate with system size that unifies both ordered arrays and disordered atomic clouds in arbitrary dimensions at fixed density. We demonstrate that, for a fixed atomic density, the maximum emission rate scales universally as the product of the atom number and the system's geometric optical depth. The geometric optical depth differs from the result of the Beer-Lambert law at high density and encodes the dimensional scaling across all regimes from independent emission to the Dicke limit. Furthermore, we establish a scaling law for directional detection, revealing that the observed rate depends on the detector's numerical aperture: small apertures yield Dicke-like quadratic scaling, whereas large apertures recover our integrated universal bound. Our results establish optical depth as the parameter governing many-body cooperative emission in both ordered and disordered ensembles, and reveal that directional and total-emission scalings must be carefully distinguished in experimental settings.

Main text: 9 pages + 3 figures. Supplemental Material: 18 pages + 6 figures. v2: Published version

arXiv:2604.24680 [quant-ph]

(or arXiv:2604.24680v2 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2604.24680 Focus to learn more arXiv-issued DOI via DataCite

Phys. Rev. Lett. 137, 143603 (2026)

https://doi.org/10.1103/xvt4-1vg7 Focus to learn more DOI(s) linking to related resources

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Full text under the publisher's open licence · 300 words

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