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    Interference bunching and antibunching of coherent and atomic radiation fields

    P. R. Berman, H. Nguyen, Y. Mei*, Y. Li, and A. Kuzmich

    • Physics Department, University of Michigan, Ann Arbor, Michigan 48109, USA

    • *Current address: Department of Physics and Astronomy, Washington State University, Pullman, Washington 99164, USA.

    Phys. Rev. A 108, 043713 – Published 16 October, 2023

    DOI: https://doi.org/10.1103/PhysRevA.108.043713

    Abstract

    When a coherent field is combined with the phase-matched output of an atomic ensemble, the second-order correlation function of the total field can exhibit superbunching or antibunching. Homodyning the reference field with the atomic emission can amplify the nonclassical characteristics of the atomic emission. A theoretical description of these phenomena is presented. It is pointed out that, even if the number of excitations in the ensemble is much less than unity, truncating a factorized state to have at most two excitations can lead to errors in calculating the second-order correlation function. We also include the effects of dephasing produced by Rydberg-Rydberg interactions and show how they modify the bunching and antibunching that occur in the absence of atom-atom interactions. It is shown that the particle separation probability distribution and the joint particle separation probability distribution play critical roles in determining the effects of dephasing.

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