{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:GA4MCUO3BIZIMQP27WKKW4EFEG","short_pith_number":"pith:GA4MCUO3","schema_version":"1.0","canonical_sha256":"3038c151db0a328641fafd94ab708521960ffc1762161d839febd4266f1036ac","source":{"kind":"arxiv","id":"2603.18933","version":2},"attestation_state":"computed","paper":{"title":"Cavity Control of Strongly Correlated Electrons Beyond Resonant Coupling","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.mes-hall","cond-mat.str-el"],"primary_cat":"quant-ph","authors_text":"Angel Rubio, Dante M. Kennes, Emil Vi\\~nas Bostr\\\"om, Lukas Grunwald, Marios H. Michael, Michael Ruggenthaler, Xinle Cheng","submitted_at":"2026-03-19T14:10:39Z","abstract_excerpt":"Interfacing materials with electromagnetic cavities offers a route to modify equilibrium properties through structured vacuum fluctuations. The coupling between light and correlated electrons lacks a characteristic energy scale, making vacuum induced ground state modifications of such systems inherently off-resonant and sensitive to the full photon mode structure. We develop a consistent cavity-QED formalism for dispersive electromagnetic environments in the Coulomb gauge, capturing both dynamical dressing via the vector potential and static screening by the dielectric. With this formalism, we"},"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":"2603.18933","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2026-03-19T14:10:39Z","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.str-el"],"title_canon_sha256":"5ecc713ac4d41c1daaffe7c572f7a0fb130526dcb8ad0cfebc91d863908aaeb0","abstract_canon_sha256":"5ee6eefcbe4d142641ed002917f700b58d0d2c02959dbe721e36f2391f641add"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-28T02:24:18.530280Z","signature_b64":"y68ql00geCQAYUTCvHbZ8Yebts7yiA1MDJ/N+uOiv5vX8xn8s1AjpNw9QM+3ZulP5ZAv1LYfXeDhWW8JuaAUDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3038c151db0a328641fafd94ab708521960ffc1762161d839febd4266f1036ac","last_reissued_at":"2026-07-28T02:24:18.529303Z","signature_status":"signed_v1","first_computed_at":"2026-07-28T02:24:18.529303Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Cavity Control of Strongly Correlated Electrons Beyond Resonant Coupling","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.mes-hall","cond-mat.str-el"],"primary_cat":"quant-ph","authors_text":"Angel Rubio, Dante M. Kennes, Emil Vi\\~nas Bostr\\\"om, Lukas Grunwald, Marios H. Michael, Michael Ruggenthaler, Xinle Cheng","submitted_at":"2026-03-19T14:10:39Z","abstract_excerpt":"Interfacing materials with electromagnetic cavities offers a route to modify equilibrium properties through structured vacuum fluctuations. The coupling between light and correlated electrons lacks a characteristic energy scale, making vacuum induced ground state modifications of such systems inherently off-resonant and sensitive to the full photon mode structure. We develop a consistent cavity-QED formalism for dispersive electromagnetic environments in the Coulomb gauge, capturing both dynamical dressing via the vector potential and static screening by the dielectric. With this formalism, we"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2603.18933","kind":"arxiv","version":2},"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/2603.18933/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":"2603.18933","created_at":"2026-07-28T02:24:18.529771+00:00"},{"alias_kind":"arxiv_version","alias_value":"2603.18933v2","created_at":"2026-07-28T02:24:18.529771+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2603.18933","created_at":"2026-07-28T02:24:18.529771+00:00"},{"alias_kind":"pith_short_12","alias_value":"GA4MCUO3BIZI","created_at":"2026-07-28T02:24:18.529771+00:00"},{"alias_kind":"pith_short_16","alias_value":"GA4MCUO3BIZIMQP2","created_at":"2026-07-28T02:24:18.529771+00:00"},{"alias_kind":"pith_short_8","alias_value":"GA4MCUO3","created_at":"2026-07-28T02:24:18.529771+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/GA4MCUO3BIZIMQP27WKKW4EFEG","json":"https://pith.science/pith/GA4MCUO3BIZIMQP27WKKW4EFEG.json","graph_json":"https://pith.science/api/pith-number/GA4MCUO3BIZIMQP27WKKW4EFEG/graph.json","events_json":"https://pith.science/api/pith-number/GA4MCUO3BIZIMQP27WKKW4EFEG/events.json","paper":"https://pith.science/paper/GA4MCUO3"},"agent_actions":{"view_html":"https://pith.science/pith/GA4MCUO3BIZIMQP27WKKW4EFEG","download_json":"https://pith.science/pith/GA4MCUO3BIZIMQP27WKKW4EFEG.json","view_paper":"https://pith.science/paper/GA4MCUO3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2603.18933&json=true","fetch_graph":"https://pith.science/api/pith-number/GA4MCUO3BIZIMQP27WKKW4EFEG/graph.json","fetch_events":"https://pith.science/api/pith-number/GA4MCUO3BIZIMQP27WKKW4EFEG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GA4MCUO3BIZIMQP27WKKW4EFEG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GA4MCUO3BIZIMQP27WKKW4EFEG/action/storage_attestation","attest_author":"https://pith.science/pith/GA4MCUO3BIZIMQP27WKKW4EFEG/action/author_attestation","sign_citation":"https://pith.science/pith/GA4MCUO3BIZIMQP27WKKW4EFEG/action/citation_signature","submit_replication":"https://pith.science/pith/GA4MCUO3BIZIMQP27WKKW4EFEG/action/replication_record"}},"created_at":"2026-07-28T02:24:18.529771+00:00","updated_at":"2026-07-28T02:24:18.529771+00:00"}