{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:BUPCOLOCDOCGBJXTX7AK5QBT5P","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":"bd84042cc41987470fffdd765ee7aaafbc72e8075ba695c4c4104a42208fd55c","cross_cats_sorted":["cond-mat.quant-gas","cond-mat.stat-mech","gr-qc","quant-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-04-20T19:18:05Z","title_canon_sha256":"bee5b5b1cc4b9eeab839745879873e4063a5088a86a2176b78b899f7643ace9e"},"schema_version":"1.0","source":{"id":"2204.09749","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2204.09749","created_at":"2026-07-05T05:33:45Z"},{"alias_kind":"arxiv_version","alias_value":"2204.09749v2","created_at":"2026-07-05T05:33:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2204.09749","created_at":"2026-07-05T05:33:45Z"},{"alias_kind":"pith_short_12","alias_value":"BUPCOLOCDOCG","created_at":"2026-07-05T05:33:45Z"},{"alias_kind":"pith_short_16","alias_value":"BUPCOLOCDOCGBJXT","created_at":"2026-07-05T05:33:45Z"},{"alias_kind":"pith_short_8","alias_value":"BUPCOLOC","created_at":"2026-07-05T05:33:45Z"}],"graph_snapshots":[{"event_id":"sha256:6833de6460540f3fddc5c997fe20038a5a897ecfcb614dc892051a3f96cbc56c","target":"graph","created_at":"2026-07-05T05:33:45Z","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/2204.09749/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We explore the implications of stable gravitational orbits around an AdS black hole for the boundary conformal field theory. The orbits are long-lived states that eventually decay due to gravitational radiation and tunneling. They appear as narrow resonances in the heavy-light OPE when the spectrum becomes effectively continuous due to the presence of the black hole horizon. Alternatively, they can be identified with quasi-normal modes with small imaginary part in the thermal two-point function. The two pictures are related via the eigenstate thermalisation hypothesis. When the decay effects c","authors_text":"Alexander Zhiboedov, Matthew Dodelson","cross_cats":["cond-mat.quant-gas","cond-mat.stat-mech","gr-qc","quant-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-04-20T19:18:05Z","title":"Gravitational orbits, double-twist mirage, and many-body scars"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2204.09749","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":"sha256:8cdca49502abba051c49706e8f532d3e09bc05edd520b133834f57acf6edb752","target":"record","created_at":"2026-07-05T05:33:45Z","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":"bd84042cc41987470fffdd765ee7aaafbc72e8075ba695c4c4104a42208fd55c","cross_cats_sorted":["cond-mat.quant-gas","cond-mat.stat-mech","gr-qc","quant-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-04-20T19:18:05Z","title_canon_sha256":"bee5b5b1cc4b9eeab839745879873e4063a5088a86a2176b78b899f7643ace9e"},"schema_version":"1.0","source":{"id":"2204.09749","kind":"arxiv","version":2}},"canonical_sha256":"0d1e272dc21b8460a6f3bfc0aec033ebdb4b4d7180b5fc82b46cc5d4c3265fd9","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0d1e272dc21b8460a6f3bfc0aec033ebdb4b4d7180b5fc82b46cc5d4c3265fd9","first_computed_at":"2026-07-05T05:33:45.998044Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T05:33:45.998044Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"hDSRNkIKmFWOCLkkqkfk4zThUrBlh4xv12drAbVlYKQtBsDJDlO0GuzhlX87s555Hp6aGawxZ0Y4NJiCUCTBBA==","signature_status":"signed_v1","signed_at":"2026-07-05T05:33:45.998593Z","signed_message":"canonical_sha256_bytes"},"source_id":"2204.09749","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8cdca49502abba051c49706e8f532d3e09bc05edd520b133834f57acf6edb752","sha256:6833de6460540f3fddc5c997fe20038a5a897ecfcb614dc892051a3f96cbc56c"],"state_sha256":"30a519aeb88634c4cea2ff66a008937202484807d0bfa66df9f02052e8eff35c"}