{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:WBCVWZ57MCIP34JIQNUZMCGEQC","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"b96dd90fa3b53f4af01b4b4f5d3dc25fec42b5499499d40902465d9b2ca90853","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.app-ph","submitted_at":"2024-10-28T08:58:30Z","title_canon_sha256":"dc833ef22a83f45f95139597f46d68f9529930820ac4d124bb5c8c570229030f"},"schema_version":"1.0","source":{"id":"2410.20845","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2410.20845","created_at":"2026-07-05T12:07:36Z"},{"alias_kind":"arxiv_version","alias_value":"2410.20845v2","created_at":"2026-07-05T12:07:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2410.20845","created_at":"2026-07-05T12:07:36Z"},{"alias_kind":"pith_short_12","alias_value":"WBCVWZ57MCIP","created_at":"2026-07-05T12:07:36Z"},{"alias_kind":"pith_short_16","alias_value":"WBCVWZ57MCIP34JI","created_at":"2026-07-05T12:07:36Z"},{"alias_kind":"pith_short_8","alias_value":"WBCVWZ57","created_at":"2026-07-05T12:07:36Z"}],"graph_snapshots":[{"event_id":"sha256:e7474f7b4056f65d7c76b4dd3abe26e874b6b2d116f7d3a90a0ccd34875a66a8","target":"graph","created_at":"2026-07-05T12:07:36Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2410.20845/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We investigate the resonant interaction between a deep-subwavelength particle and a perfectly conducting rectangular cavity, with potential applications in cavity classical and quantum electrodynamics and wave physics. The particle may behave as a harmonic oscillator, such as a semiconductor plasmonic nanoparticle, a ferrite particle, or as a two-level system, such as a Rydberg atom or trapped ion operating in the microwave regime, where metals can be modeled as perfect conductors at microwave frequencies. Our primary objective is to determine the joint resonances (eigenfrequencies) of the cou","authors_text":"Koffi-Emmanuel Sadzi, Yakir Hadad","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.app-ph","submitted_at":"2024-10-28T08:58:30Z","title":"Exact Formulation of the Resonant Coupling of a Deep-Subwavelength Particle in a Rectangular Conducting Cavity: Beyond the Jaynes-Cummings Model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2410.20845","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:db875f5a987a3a49caa6ae805dc2946063a7e50da0bd3b9fd4a8178f7d757ae4","target":"record","created_at":"2026-07-05T12:07:36Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"b96dd90fa3b53f4af01b4b4f5d3dc25fec42b5499499d40902465d9b2ca90853","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.app-ph","submitted_at":"2024-10-28T08:58:30Z","title_canon_sha256":"dc833ef22a83f45f95139597f46d68f9529930820ac4d124bb5c8c570229030f"},"schema_version":"1.0","source":{"id":"2410.20845","kind":"arxiv","version":2}},"canonical_sha256":"b0455b67bf6090fdf12883699608c48082ce2a96b4b76283c0404d05d5b0e7ac","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b0455b67bf6090fdf12883699608c48082ce2a96b4b76283c0404d05d5b0e7ac","first_computed_at":"2026-07-05T12:07:36.533837Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T12:07:36.533837Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"zbPOM83RvC4cuxAJ8M7wsIsxUHCfdGAem0T6JF2/jd/MJA64CaUmhvlt6+0Jkvs6jnuXZ9C+gltVQcuKpa+kAg==","signature_status":"signed_v1","signed_at":"2026-07-05T12:07:36.534290Z","signed_message":"canonical_sha256_bytes"},"source_id":"2410.20845","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:db875f5a987a3a49caa6ae805dc2946063a7e50da0bd3b9fd4a8178f7d757ae4","sha256:e7474f7b4056f65d7c76b4dd3abe26e874b6b2d116f7d3a90a0ccd34875a66a8"],"state_sha256":"dc4303b5076d2484b1d3f91559a5efcfe03f641bc16aff77c329be7f05bb4680"}