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Main Authors: Klimkin, Nikolai D., Ivanov, Misha
Format: Preprint
Published: 2025
Subjects:
Online Access:https://arxiv.org/abs/2511.03590
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author Klimkin, Nikolai D.
Ivanov, Misha
author_facet Klimkin, Nikolai D.
Ivanov, Misha
contents Creation and manipulation of non-classical states of light is rapidly becoming the focus of modern attosecond science. Here, we demonstrate numerically how interaction with such states can trigger the emergence of a many-body system with spontaneously broken symmetry by considering a modification of the well-known problem of superradiance encountered already by Dicke. Similarly to him, we investigate photon emission by ensembles of indistinguishable atoms. In contrast to him, however, we leverage symmetry-based selection rules to suppress emission of single photons by single atoms. A steady state is therefore only reached following a spontaneous transition into a collective symmetry-broken state of atoms and photonic modes. This transition permanently locks the atomic dipoles to the quantum field experienced by the system at a particular instant, transforming the entire setup into a potent quantum sensor reproducing the phase of the recorded quantum fluctuation.
format Preprint
id arxiv_https___arxiv_org_abs_2511_03590
institution arXiv
publishDate 2025
record_format arxiv
spellingShingle Spontaneous symmetry breaking in nonlinear superradiance
Klimkin, Nikolai D.
Ivanov, Misha
Quantum Physics
Optics
Creation and manipulation of non-classical states of light is rapidly becoming the focus of modern attosecond science. Here, we demonstrate numerically how interaction with such states can trigger the emergence of a many-body system with spontaneously broken symmetry by considering a modification of the well-known problem of superradiance encountered already by Dicke. Similarly to him, we investigate photon emission by ensembles of indistinguishable atoms. In contrast to him, however, we leverage symmetry-based selection rules to suppress emission of single photons by single atoms. A steady state is therefore only reached following a spontaneous transition into a collective symmetry-broken state of atoms and photonic modes. This transition permanently locks the atomic dipoles to the quantum field experienced by the system at a particular instant, transforming the entire setup into a potent quantum sensor reproducing the phase of the recorded quantum fluctuation.
title Spontaneous symmetry breaking in nonlinear superradiance
topic Quantum Physics
Optics
url https://arxiv.org/abs/2511.03590