Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/114597
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dc.contributorDepartment of Applied Mathematics-
dc.contributorMainland Development Office-
dc.creatorYin, XL-
dc.creatorLee, HWJ-
dc.creatorZhang, G-
dc.date.accessioned2025-08-18T03:02:02Z-
dc.date.available2025-08-18T03:02:02Z-
dc.identifier.issn2469-9926-
dc.identifier.urihttp://hdl.handle.net/10397/114597-
dc.language.isoenen_US
dc.publisherAmerican Physical Societyen_US
dc.rights©2025 American Physical Societyen_US
dc.rightsThe following publication Yin, X.-L., Lee, H.-w. J., & Zhang, G. (2025). Giant-atom dephasing dynamics and entanglement generation in a squeezed vacuum reservoir. Physical Review A, 111(3), 033707 is available at https://doi.org/10.1103/PhysRevA.111.033707.en_US
dc.titleGiant-atom dephasing dynamics and entanglement generation in a squeezed vacuum reservoiren_US
dc.typeJournal/Magazine Articleen_US
dc.identifier.volume111-
dc.identifier.issue3-
dc.identifier.doi10.1103/PhysRevA.111.033707-
dcterms.abstractThe study of atomic behaviors in a squeezed vacuum reservoir plays an important role in exploring quantum effect and quantum physics. We here propose a scheme to manipulate the dynamics of giant atoms coupled to a one-dimensional waveguide driven by a broadband squeezed field, which acts as a squeezed vacuum reservoir. By tuning the propagating phase of photons, the center-of-mass phase of the giant atom, and the squeezing parameter, both the dephasing dynamics and entanglement dynamics of giant atoms can be effectively controlled. In the single-giant-atom case, we obtain the expressions of the dephasing rates based on the Bloch equations derived from the quantum master equation of the giant atom. Adjusting these two phases enables the dephasing rates to be enhanced, suppressed, or reduced to zero, thereby changing the dephasing dynamics. For the two-giant-atom system, we find that the atomic individual and collective squeezing depend on these two phases simultaneously. The steady-state giant-atom population and entanglement are obtained by working in the collective state representation for the two atoms. Different from small atoms, the steady-state population and entanglement depend on not only the center-mass-of phase, but also the propagating phase. In addition, we identify the condition for achieving larger steady-state entanglement via analyzing the system parameters. This work will facilitate the study of light-matter interaction based on giant-atom waveguide QED systems driven by a squeezed vacuum reservoir and has potential applications in quantum information processing.-
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationPhysical review A, Mar. 2025, v. 111, no. 3, 033707-
dcterms.isPartOfPhysical review A-
dcterms.issued2025-03-
dc.identifier.scopus2-s2.0-105000320270-
dc.identifier.eissn2469-9934-
dc.identifier.artn033707-
dc.description.validate202508 bcch-
dc.description.oaVersion of Recorden_US
dc.identifier.FolderNumberOA_Othersen_US
dc.description.fundingSourceRGCen_US
dc.description.fundingSourceOthersen_US
dc.description.fundingTextInnovation Program for Quantum Science and Technology 2023ZD0300600; Guangdong Provincial Quantum Science Strategic Initiative (No. GDZX2200001); National Natural Science Foundation of China under Grant No. 62173288en_US
dc.description.pubStatusPublisheden_US
dc.description.oaCategoryVoR alloweden_US
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