Phonon and maxon instability in Bose–Einstein condensates with parity-time symmetric spin–orbit coupling

Parity-time ( $\mathcal{PT}$ ) symmetry has drawn great research interest in non-Hermitian physics. Recently, there is an emerging model of $\mathcal{PT}$ -symmetric spin–orbit coupling (SOC) which could be realized with spin-1/2 atomic Bose–Einstein condensates (BECs) when the two spin components a...

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Main Authors: Jieli Qin, Lu Zhou, Guangjiong Dong
Format: Article
Language:English
Published: IOP Publishing 2023-01-01
Series:New Journal of Physics
Subjects:
Online Access:https://doi.org/10.1088/1367-2630/ad1417
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author Jieli Qin
Lu Zhou
Guangjiong Dong
author_facet Jieli Qin
Lu Zhou
Guangjiong Dong
author_sort Jieli Qin
collection DOAJ
description Parity-time ( $\mathcal{PT}$ ) symmetry has drawn great research interest in non-Hermitian physics. Recently, there is an emerging model of $\mathcal{PT}$ -symmetric spin–orbit coupling (SOC) which could be realized with spin-1/2 atomic Bose–Einstein condensates (BECs) when the two spin components are respectively subjected to momentum-dependent gain and loss (Qin et al 2022 New J. Phys. 24 063025). In this model, inter-atom interaction has no influence on the $\mathcal{PT}$ -symmetric plane waves. Thus, collective excitation playing the role of fingerprint of inter-atom interaction is investigated in this paper. For the phonon excitation, it is shown that the repulsive interaction between atoms in different spin states, which tends to drive the atoms to populate in only one spin component, can break the $\mathcal{PT}$ -symmetry, and leads to a phonon instability. Whereas, for the case of the phonon-maxon-roton collective excitation spectrum, the repulsive interaction between atoms in different spin states can lead to a maxon instability, which does not occur in Hermitian BEC systems (dipolar BECs or BECs with Raman induced SOC). Simulation of the time evolution of the plane wave solution against small noise shows that the maxon instability can result in the formation of a supersolid-like stripe pattern at the initial stage, but the non-Hermitian nature of the system finally destroys the pattern. The phase diagram of stability shows that the Rabi coupling and repulsive interaction between the atoms in the same spin state can stabilize the system.
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spelling doaj.art-e8d5f81ee702420d8a66b2836d2648812023-12-29T06:20:24ZengIOP PublishingNew Journal of Physics1367-26302023-01-01251212305310.1088/1367-2630/ad1417Phonon and maxon instability in Bose–Einstein condensates with parity-time symmetric spin–orbit couplingJieli Qin0https://orcid.org/0000-0003-4112-2875Lu Zhou1Guangjiong Dong2School of Physics and Materials Science, Guangzhou University, Guangzhou Higher Education Mega Center, 230 Wai Huan Xi Road, Guangzhou 510006, People’s Republic of ChinaDepartment of Physics, School of Physics and Electronic Science, East China Normal University , Shanghai 200241, People’s Republic of China; Collaborative Innovation Center of Extreme Optics, Shanxi University , Taiyuan, Shanxi 030006, People’s Republic of ChinaState Key Laboratory of Precision Spectroscopy, East China Normal University , Shanghai 200241, People’s Republic of China; Collaborative Innovation Center of Extreme Optics, Shanxi University , Taiyuan, Shanxi 030006, People’s Republic of ChinaParity-time ( $\mathcal{PT}$ ) symmetry has drawn great research interest in non-Hermitian physics. Recently, there is an emerging model of $\mathcal{PT}$ -symmetric spin–orbit coupling (SOC) which could be realized with spin-1/2 atomic Bose–Einstein condensates (BECs) when the two spin components are respectively subjected to momentum-dependent gain and loss (Qin et al 2022 New J. Phys. 24 063025). In this model, inter-atom interaction has no influence on the $\mathcal{PT}$ -symmetric plane waves. Thus, collective excitation playing the role of fingerprint of inter-atom interaction is investigated in this paper. For the phonon excitation, it is shown that the repulsive interaction between atoms in different spin states, which tends to drive the atoms to populate in only one spin component, can break the $\mathcal{PT}$ -symmetry, and leads to a phonon instability. Whereas, for the case of the phonon-maxon-roton collective excitation spectrum, the repulsive interaction between atoms in different spin states can lead to a maxon instability, which does not occur in Hermitian BEC systems (dipolar BECs or BECs with Raman induced SOC). Simulation of the time evolution of the plane wave solution against small noise shows that the maxon instability can result in the formation of a supersolid-like stripe pattern at the initial stage, but the non-Hermitian nature of the system finally destroys the pattern. The phase diagram of stability shows that the Rabi coupling and repulsive interaction between the atoms in the same spin state can stabilize the system.https://doi.org/10.1088/1367-2630/ad1417parity-time symmetrycollective excitationmodulation instabilityBose–Einstein condensatespin–orbit coupling
spellingShingle Jieli Qin
Lu Zhou
Guangjiong Dong
Phonon and maxon instability in Bose–Einstein condensates with parity-time symmetric spin–orbit coupling
New Journal of Physics
parity-time symmetry
collective excitation
modulation instability
Bose–Einstein condensate
spin–orbit coupling
title Phonon and maxon instability in Bose–Einstein condensates with parity-time symmetric spin–orbit coupling
title_full Phonon and maxon instability in Bose–Einstein condensates with parity-time symmetric spin–orbit coupling
title_fullStr Phonon and maxon instability in Bose–Einstein condensates with parity-time symmetric spin–orbit coupling
title_full_unstemmed Phonon and maxon instability in Bose–Einstein condensates with parity-time symmetric spin–orbit coupling
title_short Phonon and maxon instability in Bose–Einstein condensates with parity-time symmetric spin–orbit coupling
title_sort phonon and maxon instability in bose einstein condensates with parity time symmetric spin orbit coupling
topic parity-time symmetry
collective excitation
modulation instability
Bose–Einstein condensate
spin–orbit coupling
url https://doi.org/10.1088/1367-2630/ad1417
work_keys_str_mv AT jieliqin phononandmaxoninstabilityinboseeinsteincondensateswithparitytimesymmetricspinorbitcoupling
AT luzhou phononandmaxoninstabilityinboseeinsteincondensateswithparitytimesymmetricspinorbitcoupling
AT guangjiongdong phononandmaxoninstabilityinboseeinsteincondensateswithparitytimesymmetricspinorbitcoupling