We investigate the evolution of the second-order temporal coherence during the emission of a superradiant pulse by an elongated cloud of cold Rb atoms in free space. To do so, we measure the two-times intensity correlation function g(2) N (t1, t2) following the pulsed excitation of the cloud. By monitoring g(2) N (t, t) during the pulse, we observe the establishment of second-order coherence, and contrast it with the situation where the cloud is initially prepared in a steady state. We compare our findings to the predictions of the Dicke model, using an effective atom number to account for finite size effects, finding that the model reproduces the observed trend at early time. For longer times, we observe a subradiant decay, a feature that goes beyond Dicke's model. Finally, we measure the g(2) N (t1, t2) at different times and observe the appearance of anticorrelations during the pulse that are not present when starting from a steady state.
Emergence of Second-Order Coherence in the Superradiant Emission from a Free-Space Atomic Ensemble / Ferioli G.; Ferrier-Barbut I.; Browaeys A.. - In: PHYSICAL REVIEW LETTERS. - ISSN 1079-7114. - ELETTRONICO. - 134:(2025), pp. 153602.0-153602.0. [10.1103/PhysRevLett.134.153602]
Emergence of Second-Order Coherence in the Superradiant Emission from a Free-Space Atomic Ensemble
Ferioli G.
Writing – Review & Editing
;Browaeys A.
Supervision
2025
Abstract
We investigate the evolution of the second-order temporal coherence during the emission of a superradiant pulse by an elongated cloud of cold Rb atoms in free space. To do so, we measure the two-times intensity correlation function g(2) N (t1, t2) following the pulsed excitation of the cloud. By monitoring g(2) N (t, t) during the pulse, we observe the establishment of second-order coherence, and contrast it with the situation where the cloud is initially prepared in a steady state. We compare our findings to the predictions of the Dicke model, using an effective atom number to account for finite size effects, finding that the model reproduces the observed trend at early time. For longer times, we observe a subradiant decay, a feature that goes beyond Dicke's model. Finally, we measure the g(2) N (t1, t2) at different times and observe the appearance of anticorrelations during the pulse that are not present when starting from a steady state.I documenti in FLORE sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.



