{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:PBWEDGRM43VHQQ75YMXIZEWFXP","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":"f05250d253baa9ffa54f1fd06c9533518962e524e29c5f0e8fe488c6d9f2fad5","cross_cats_sorted":["cond-mat.dis-nn","quant-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2025-09-23T14:23:15Z","title_canon_sha256":"eb7de6fce2f70e126714179f8c44d07a4c93a165595ba6352d8ccb86ff257fe8"},"schema_version":"1.0","source":{"id":"2509.19059","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2509.19059","created_at":"2026-06-23T01:12:47Z"},{"alias_kind":"arxiv_version","alias_value":"2509.19059v2","created_at":"2026-06-23T01:12:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2509.19059","created_at":"2026-06-23T01:12:47Z"},{"alias_kind":"pith_short_12","alias_value":"PBWEDGRM43VH","created_at":"2026-06-23T01:12:47Z"},{"alias_kind":"pith_short_16","alias_value":"PBWEDGRM43VHQQ75","created_at":"2026-06-23T01:12:47Z"},{"alias_kind":"pith_short_8","alias_value":"PBWEDGRM","created_at":"2026-06-23T01:12:47Z"}],"graph_snapshots":[{"event_id":"sha256:958b69e88b57d9cc2c19bcdb24e8b1961e641ef1aff61194809f038e4942f56f","target":"graph","created_at":"2026-06-23T01:12:47Z","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/2509.19059/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We investigate excitation transfer in an engineered cavity QED transport architecture consisting of an N-site donor ring coupled coherently to a central acceptor and driven by a single quantized photon mode. The system evolves under a Lindblad master equation including spontaneous loss and pure dephasing. In the ordered symmetric limit, the dynamics reduce exactly to a photon-bright mode-acceptor trimer, allowing closed-form analytic expressions for transfer efficiencies and mode-resolved losses.\n  We demonstrate that near-unity efficiency arises from photon-mediated hybridization that generat","authors_text":"Oliver Fox, Roger Andrews, Sarben Sarkar, Stephon Alexander","cross_cats":["cond-mat.dis-nn","quant-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2025-09-23T14:23:15Z","title":"Photon-Mediated Hybridization and Dissipative Transport in a Cavity-QED Ring-Acceptor Architecture"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2509.19059","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":"sha256:00dc65543ecd6b90e3e00d600976d5b42303dcc63677bc7a18eb7834c6b7ae28","target":"record","created_at":"2026-06-23T01:12:47Z","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":"f05250d253baa9ffa54f1fd06c9533518962e524e29c5f0e8fe488c6d9f2fad5","cross_cats_sorted":["cond-mat.dis-nn","quant-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2025-09-23T14:23:15Z","title_canon_sha256":"eb7de6fce2f70e126714179f8c44d07a4c93a165595ba6352d8ccb86ff257fe8"},"schema_version":"1.0","source":{"id":"2509.19059","kind":"arxiv","version":2}},"canonical_sha256":"786c419a2ce6ea7843fdc32e8c92c5bbf7f6ff89b7fe5024add9b594b07e648c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"786c419a2ce6ea7843fdc32e8c92c5bbf7f6ff89b7fe5024add9b594b07e648c","first_computed_at":"2026-06-23T01:12:47.352179Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-06-23T01:12:47.352179Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"BIDIpog81gSAtshjMkr7ChDEdvfDaKSEp9xI2BPBNN2evr/PccMIsAZ92rwfWtZJV5xsVlBJWCbxksaGKzM+BA==","signature_status":"signed_v1","signed_at":"2026-06-23T01:12:47.352764Z","signed_message":"canonical_sha256_bytes"},"source_id":"2509.19059","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:00dc65543ecd6b90e3e00d600976d5b42303dcc63677bc7a18eb7834c6b7ae28","sha256:958b69e88b57d9cc2c19bcdb24e8b1961e641ef1aff61194809f038e4942f56f"],"state_sha256":"895bc0fec53cc4b0c129f65768c521c76ef7a71f0598edd3d6240c3dd137f469"}