{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:7N4T5YJKJ4F6NPUO2G4AFX3TGX","short_pith_number":"pith:7N4T5YJK","schema_version":"1.0","canonical_sha256":"fb793ee12a4f0be6be8ed1b802df7335e58f0e4f488eccb0135829a0f695121d","source":{"kind":"arxiv","id":"2607.26453","version":1},"attestation_state":"computed","paper":{"title":"Asymmetric Floquet-Engineered Mode Coupling in Hybrid Magnonics","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["physics.app-ph"],"primary_cat":"cond-mat.mes-hall","authors_text":"Amin Pishehvar, Benedetta Flebus, Jayakrishnan M. P. Nair, Xufeng Zhang, Yu Jiang, Zixin Yan","submitted_at":"2026-07-29T04:07:11Z","abstract_excerpt":"In hybrid magnonic systems, linear magnon--photon hybridization inherently produces symmetric, reciprocal interactions, precluding asymmetric mode coupling. Floquet driving can tailor mode coupling strengths but, with single-tone modulation, inevitably generates a symmetric interaction that preserves this reciprocity. Here we introduce dual-tone Floquet modulation to unlock a new degree of freedom in hybrid magnonic systems, where the relative phase $\\theta$ of two commensurate drives continuously controls the asymmetry of the Floquet-engineered interaction, enabling asymmetric mode coupling a"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2607.26453","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2026-07-29T04:07:11Z","cross_cats_sorted":["physics.app-ph"],"title_canon_sha256":"74be21b9c4126b9160895135d54434a33e05c0db8483e793da47abec53d6af85","abstract_canon_sha256":"cb34da6edae7202bdca67ab99cd1b1ea33ecdc2b4b3070f85bfba3fe12e86512"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fb793ee12a4f0be6be8ed1b802df7335e58f0e4f488eccb0135829a0f695121d","last_reissued_at":"2026-07-30T01:20:32.907389Z","signature_status":"unsigned_v0","first_computed_at":"2026-07-30T01:20:32.907389Z"},"graph_snapshot":{"paper":{"title":"Asymmetric Floquet-Engineered Mode Coupling in Hybrid Magnonics","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["physics.app-ph"],"primary_cat":"cond-mat.mes-hall","authors_text":"Amin Pishehvar, Benedetta Flebus, Jayakrishnan M. P. Nair, Xufeng Zhang, Yu Jiang, Zixin Yan","submitted_at":"2026-07-29T04:07:11Z","abstract_excerpt":"In hybrid magnonic systems, linear magnon--photon hybridization inherently produces symmetric, reciprocal interactions, precluding asymmetric mode coupling. Floquet driving can tailor mode coupling strengths but, with single-tone modulation, inevitably generates a symmetric interaction that preserves this reciprocity. Here we introduce dual-tone Floquet modulation to unlock a new degree of freedom in hybrid magnonic systems, where the relative phase $\\theta$ of two commensurate drives continuously controls the asymmetry of the Floquet-engineered interaction, enabling asymmetric mode coupling a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2607.26453","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2607.26453/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"2607.26453","created_at":"2026-07-30T01:20:32.912684+00:00"},{"alias_kind":"arxiv_version","alias_value":"2607.26453v1","created_at":"2026-07-30T01:20:32.912684+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2607.26453","created_at":"2026-07-30T01:20:32.912684+00:00"},{"alias_kind":"pith_short_12","alias_value":"7N4T5YJKJ4F6","created_at":"2026-07-30T01:20:32.912684+00:00"},{"alias_kind":"pith_short_16","alias_value":"7N4T5YJKJ4F6NPUO","created_at":"2026-07-30T01:20:32.912684+00:00"},{"alias_kind":"pith_short_8","alias_value":"7N4T5YJK","created_at":"2026-07-30T01:20:32.912684+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/7N4T5YJKJ4F6NPUO2G4AFX3TGX","json":"https://pith.science/pith/7N4T5YJKJ4F6NPUO2G4AFX3TGX.json","graph_json":"https://pith.science/api/pith-number/7N4T5YJKJ4F6NPUO2G4AFX3TGX/graph.json","events_json":"https://pith.science/api/pith-number/7N4T5YJKJ4F6NPUO2G4AFX3TGX/events.json","paper":"https://pith.science/paper/7N4T5YJK"},"agent_actions":{"view_html":"https://pith.science/pith/7N4T5YJKJ4F6NPUO2G4AFX3TGX","download_json":"https://pith.science/pith/7N4T5YJKJ4F6NPUO2G4AFX3TGX.json","view_paper":"https://pith.science/paper/7N4T5YJK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2607.26453&json=true","fetch_graph":"https://pith.science/api/pith-number/7N4T5YJKJ4F6NPUO2G4AFX3TGX/graph.json","fetch_events":"https://pith.science/api/pith-number/7N4T5YJKJ4F6NPUO2G4AFX3TGX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7N4T5YJKJ4F6NPUO2G4AFX3TGX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7N4T5YJKJ4F6NPUO2G4AFX3TGX/action/storage_attestation","attest_author":"https://pith.science/pith/7N4T5YJKJ4F6NPUO2G4AFX3TGX/action/author_attestation","sign_citation":"https://pith.science/pith/7N4T5YJKJ4F6NPUO2G4AFX3TGX/action/citation_signature","submit_replication":"https://pith.science/pith/7N4T5YJKJ4F6NPUO2G4AFX3TGX/action/replication_record"}},"created_at":"2026-07-30T01:20:32.912684+00:00","updated_at":"2026-07-30T01:20:32.912684+00:00"}