{"paper":{"title":"Floquet engineering of nonreciprocal light-induced dipolar interactions","license":"http://creativecommons.org/licenses/by/4.0/","headline":"Floquet driving of nonreciprocal dipolar forces produces beamsplitter, squeezing, and tunable complex frequencies between trapped particles.","cross_cats":["physics.atom-ph","physics.optics"],"primary_cat":"quant-ph","authors_text":"Benjamin A. Stickler, Iurie Coroli, Livia Egyed, Manuel Reisenbauer, Murad Abuzarli, Uro\\v{s} Deli\\'c","submitted_at":"2026-05-13T15:46:28Z","abstract_excerpt":"Tweezer arrays of polarizable objects are a promising platform for assembling quantum matter and building next-generation quantum sensors. Light-induced dipolar interactions have emerged as a method to couple their motion, thereby establishing a new paradigm for controlling collective mechanical degrees of freedom. Here, we extend these into the regime of Floquet-driven interactions, combined with the intrinsic nonreciprocity of optical forces. We demonstrate beamsplitter, single-, and two-mode squeezing operations, as well as signatures of a negative-mass-like oscillator arising from the nonr"},"claims":{"count":4,"items":[{"kind":"strongest_claim","text":"We demonstrate beamsplitter, single-, and two-mode squeezing operations, as well as signatures of a negative-mass-like oscillator arising from the nonreciprocity. Moreover, we show that a programmable combination of these operations enables continuous tuning of complex eigenfrequencies.","source":"verdict.strongest_claim","status":"machine_extracted","claim_id":"C1","attestation":"unclaimed"},{"kind":"weakest_assumption","text":"That the idealized Floquet-driven nonreciprocal dipolar interactions can be realized in actual tweezer arrays without dominant experimental imperfections such as heating, decoherence, or scattering losses that would wash out the predicted operations.","source":"verdict.weakest_assumption","status":"machine_extracted","claim_id":"C2","attestation":"unclaimed"},{"kind":"one_line_summary","text":"Floquet engineering of nonreciprocal light-induced dipolar interactions in tweezer arrays realizes beamsplitter, squeezing operations, negative-mass-like signatures, and tunable complex eigenfrequencies.","source":"verdict.one_line_summary","status":"machine_extracted","claim_id":"C3","attestation":"unclaimed"},{"kind":"headline","text":"Floquet driving of nonreciprocal dipolar forces produces beamsplitter, squeezing, and tunable complex frequencies between trapped particles.","source":"verdict.pith_extraction.headline","status":"machine_extracted","claim_id":"C4","attestation":"unclaimed"}],"snapshot_sha256":"9df533db2758f25fa82c5d4ccec091fa874aeafbdf25d5bc70f34923636e0fbd"},"source":{"id":"2605.13694","kind":"arxiv","version":1},"verdict":{"id":"609f2eba-3589-4f2f-9373-e13e52fc0f33","model_set":{"reader":"grok-4.3"},"created_at":"2026-05-14T18:10:18.871654Z","strongest_claim":"We demonstrate beamsplitter, single-, and two-mode squeezing operations, as well as signatures of a negative-mass-like oscillator arising from the nonreciprocity. Moreover, we show that a programmable combination of these operations enables continuous tuning of complex eigenfrequencies.","one_line_summary":"Floquet engineering of nonreciprocal light-induced dipolar interactions in tweezer arrays realizes beamsplitter, squeezing operations, negative-mass-like signatures, and tunable complex eigenfrequencies.","pipeline_version":"pith-pipeline@v0.9.0","weakest_assumption":"That the idealized Floquet-driven nonreciprocal dipolar interactions can be realized in actual tweezer arrays without dominant experimental imperfections such as heating, decoherence, or scattering losses that would wash out the predicted operations.","pith_extraction_headline":"Floquet driving of nonreciprocal dipolar forces produces beamsplitter, squeezing, and tunable complex frequencies between trapped particles."},"references":{"count":65,"sample":[{"doi":"","year":2025,"title":"Progress in quantum metrology and applications for optical atomic clocks","work_id":"aaf4e80a-33aa-46ff-8b84-755b1dfd1a26","ref_index":1,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2024,"title":"J. Ye and P. Zoller, Phys. Rev. Lett.132, 190001 (2024)","work_id":"4a8076a4-eadf-41c7-9930-12c6735bc7c5","ref_index":2,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2022,"title":"S. Colombo, E. Pedrozo-Pe˜ nafiel, and V. Vuleti´ c, Ap- plied Physics Letters121, 210502 (2022)","work_id":"91310913-efc3-42d0-ae40-a536b0652568","ref_index":3,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2008,"title":"I. Bloch, J. Dalibard, and W. Zwerger, Rev. Mod. Phys. 80, 885 (2008)","work_id":"8fba0263-5580-4644-89e3-f750bc5854d7","ref_index":4,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2023,"title":"N. Defenu, T. Donner, T. Macrı, G. Pagano, S. Ruffo, and A. Trombettoni, Reviews of Modern Physics95, 035002 (2023)","work_id":"c0fb6e96-426a-4990-b6fb-095a24768642","ref_index":5,"cited_arxiv_id":"","is_internal_anchor":false}],"resolved_work":65,"snapshot_sha256":"87d5628b68b273c7335d4cd08ce21b0e094f2049b8122b44fa963735b130dc0c","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"}