{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:COZCFYGCBM52W3QQ2MDECKKCDX","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":"4e1539e15bbbe1c160fd31c285e7bb0a9c40e6508dbab82d501f7e5ceb23080b","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2025-07-29T00:31:50Z","title_canon_sha256":"0fd22ddf5f19bfc7f5658b712c4b29f3800d994717884ff8fa40f35493333659"},"schema_version":"1.0","source":{"id":"2507.21408","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2507.21408","created_at":"2026-07-05T11:46:00Z"},{"alias_kind":"arxiv_version","alias_value":"2507.21408v2","created_at":"2026-07-05T11:46:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2507.21408","created_at":"2026-07-05T11:46:00Z"},{"alias_kind":"pith_short_12","alias_value":"COZCFYGCBM52","created_at":"2026-07-05T11:46:00Z"},{"alias_kind":"pith_short_16","alias_value":"COZCFYGCBM52W3QQ","created_at":"2026-07-05T11:46:00Z"},{"alias_kind":"pith_short_8","alias_value":"COZCFYGC","created_at":"2026-07-05T11:46:00Z"}],"graph_snapshots":[{"event_id":"sha256:63500a8b6c209e7efb4468d5c451e54fc3fd39ed020f1dbab13e08937167dbb5","target":"graph","created_at":"2026-07-05T11:46:00Z","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/2507.21408/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Phenomenological approaches to photon loss have long been the workhorse of cavity-QED, but prove inadequate in the presence of sufficiently broadband light-matter interactions. We present a rigorous and ab initio derivation of a quantum master equation for a quantized optical cavity mode coupled to a dipole, using a quasinormal mode (QNM) quantization procedure for plasmonic and dielectric open-system cavity-QED, which is valid in broadband light-matter interaction regimes, including ultrastrong coupling (USC). The theory supports general three-dimensional resonators with arbitrary dispersion ","authors_text":"Chris Gustin, Juanjuan Ren, Sebastian Franke, Stephen Hughes","cross_cats":["physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2025-07-29T00:31:50Z","title":"Dissipation in the Broadband and Ultrastrong Coupling Regimes of Cavity Quantum Electrodynamics: An Ab Initio Quantized Quasinormal Mode Approach"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2507.21408","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":"sha256:18c7039f08d639f8e30a2db552b55e6616a6da966074cc3c966324867b3cb0f2","target":"record","created_at":"2026-07-05T11:46:00Z","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":"4e1539e15bbbe1c160fd31c285e7bb0a9c40e6508dbab82d501f7e5ceb23080b","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2025-07-29T00:31:50Z","title_canon_sha256":"0fd22ddf5f19bfc7f5658b712c4b29f3800d994717884ff8fa40f35493333659"},"schema_version":"1.0","source":{"id":"2507.21408","kind":"arxiv","version":2}},"canonical_sha256":"13b222e0c20b3bab6e10d3064129421dcc141f3aad7935cf6ef19e9a78ff0ef5","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"13b222e0c20b3bab6e10d3064129421dcc141f3aad7935cf6ef19e9a78ff0ef5","first_computed_at":"2026-07-05T11:46:00.224701Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T11:46:00.224701Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"tTMkXh/9Uv5wrKahlBMVpN6K9omx4Uj54bP703J/7V7a5ND/UZGMs8N1b60PAkXfovCtKsb44n14gWrr53VoAw==","signature_status":"signed_v1","signed_at":"2026-07-05T11:46:00.225243Z","signed_message":"canonical_sha256_bytes"},"source_id":"2507.21408","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:18c7039f08d639f8e30a2db552b55e6616a6da966074cc3c966324867b3cb0f2","sha256:63500a8b6c209e7efb4468d5c451e54fc3fd39ed020f1dbab13e08937167dbb5"],"state_sha256":"df76b6f3e730e643362f87ca3d3c17691848f8c74246eb19f6c890e57d5f0807"}