Selective cooling and squeezing in a lossy optomechanical closed loop embodying an exceptional surface

buir.contributor.authorEge, Beyza Sütlüoğlu
buir.contributor.authorBulutay, Ceyhun
buir.contributor.orcidEge, Beyza Sütlüoğlu|0000-0001-8818-6548
buir.contributor.orcidBulutay, Ceyhun|0000-0003-2493-517X
dc.citation.epage18
dc.citation.issueNumber6
dc.citation.spage1
dc.citation.volumeNumber139
dc.contributor.authorEge, Beyza Sütlüoğlu
dc.contributor.authorBulutay, Ceyhun
dc.date.accessioned2025-02-12T07:27:21Z
dc.date.available2025-02-12T07:27:21Z
dc.date.issued2024-06-14
dc.departmentDepartment of Physics
dc.description.abstractA closed-loop, lossy optomechanical system consisting of one optical and two degenerate mechanical resonators is computationally investigated. This system constitutes an elementary synthetic plaquette derived from the loop phase of the intercoupling coefficients. In examining a specific quantum attribute, we delve into the control of quadrature variances within the resonator selected through the plaquette phase. An amplitude modulation is additionally applied to the cavity-pumping laser to incorporate mechanical squeezing. Our numerical analysis relies on the integration-free computation of steady-state covariances for cooling and the Floquet technique for squeezing. We provide physical insights into how non-Hermiticity plays a crucial role in enhancing cooling and squeezing in proximity to exceptional points. This enhancement is associated with the behavior of complex eigenvalue loci as a function of the intermechanical coupling rate. Additionally, we demonstrate that the parameter space embodies an exceptional surface, ensuring the robustness of exceptional point singularities under experimental parameter variations. However, the pump laser detuning breaks away from the exceptional surface unless it resides on the red-sideband by an amount sufficiently close to the mechanical resonance frequency. Finally, we show that this disparate parametric character entitles frequency-dependent cooling and squeezing, which is of technological importance.
dc.description.provenanceSubmitted by İlknur Sarıkaya (ilknur.sarikaya@bilkent.edu.tr) on 2025-02-12T07:27:21Z No. of bitstreams: 1 Selective_cooling_and_squeezing_in_a_lossy_optomechanical_closed_loop_embodying_an_exceptional_surface.pdf: 2604253 bytes, checksum: 57d4a6a0aa13c496cc58e4fd1cc511b7 (MD5)en
dc.description.provenanceMade available in DSpace on 2025-02-12T07:27:21Z (GMT). No. of bitstreams: 1 Selective_cooling_and_squeezing_in_a_lossy_optomechanical_closed_loop_embodying_an_exceptional_surface.pdf: 2604253 bytes, checksum: 57d4a6a0aa13c496cc58e4fd1cc511b7 (MD5) Previous issue date: 2024-06-14en
dc.identifier.doi10.1140/epjp/s13360-024-05263-3
dc.identifier.eissn2190-5444
dc.identifier.urihttps://hdl.handle.net/11693/116220
dc.language.isoEnglish
dc.publisherSpringer
dc.relation.isversionofhttps://doi.org/10.1140/epjp/s13360-024-05263-3
dc.rightsCC BY 40
dc.rights.urihttps://creativecommons.org/licenses/by/4.0/
dc.source.titleEuropean Physical Journal Plus
dc.titleSelective cooling and squeezing in a lossy optomechanical closed loop embodying an exceptional surface
dc.typeArticle

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