{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:FCDQ3Q2JCWXUPOD2IE7TF7EDFM","short_pith_number":"pith:FCDQ3Q2J","schema_version":"1.0","canonical_sha256":"28870dc34915af47b87a413f32fc832b2a5eef33ef29b7e9c24e279958806e80","source":{"kind":"arxiv","id":"2011.10001","version":2},"attestation_state":"computed","paper":{"title":"AdS$_3$ gravity and the complex SYK models","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Boyang Yu, Ioannis Papadimitriou, Pankaj Chaturvedi, Wei Song","submitted_at":"2020-11-19T17:57:45Z","abstract_excerpt":"We provide a non conformal generalization of the Comp\\`ere-Song-Strominger (CSS) boundary conditions for AdS$_3$ gravity that breaks the $\\widehat u(1)$ Kac-Moody-Virasoro symmetry to two $u(1)$s. The holographic dual specified by the new boundary conditions can be understood as an irrelevant deformation of a warped conformal field theory (WCFT). Upon consistent reduction to two dimensions, AdS$_3$ gravity results in a deformed Jackiw-Teitelboim dilaton gravity model coupled to a Maxwell field. We show that near extremality the boundary conditions inherited from generalized CSS boundary condit"},"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":"2011.10001","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2020-11-19T17:57:45Z","cross_cats_sorted":[],"title_canon_sha256":"ba15dd05a4b93e880f10ac24ac894d116781190d6b04c4dfcc26dc62f44b7e3a","abstract_canon_sha256":"3f909f9ef8e766688a932287747d1378a5780c3d8f4273a1a7676a96dbc9baed"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T02:40:30.209726Z","signature_b64":"1R90UYYWZWvXmoK74qhcx03YeDIlH6Y7ElKAULj8OEuFtuwEg/WPEP4Wy50pO4qd5uqUmQytiCJWBMfKLMUBAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"28870dc34915af47b87a413f32fc832b2a5eef33ef29b7e9c24e279958806e80","last_reissued_at":"2026-07-05T02:40:30.209298Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T02:40:30.209298Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"AdS$_3$ gravity and the complex SYK models","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Boyang Yu, Ioannis Papadimitriou, Pankaj Chaturvedi, Wei Song","submitted_at":"2020-11-19T17:57:45Z","abstract_excerpt":"We provide a non conformal generalization of the Comp\\`ere-Song-Strominger (CSS) boundary conditions for AdS$_3$ gravity that breaks the $\\widehat u(1)$ Kac-Moody-Virasoro symmetry to two $u(1)$s. The holographic dual specified by the new boundary conditions can be understood as an irrelevant deformation of a warped conformal field theory (WCFT). Upon consistent reduction to two dimensions, AdS$_3$ gravity results in a deformed Jackiw-Teitelboim dilaton gravity model coupled to a Maxwell field. We show that near extremality the boundary conditions inherited from generalized CSS boundary condit"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2011.10001","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/2011.10001/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":"2011.10001","created_at":"2026-07-05T02:40:30.209364+00:00"},{"alias_kind":"arxiv_version","alias_value":"2011.10001v2","created_at":"2026-07-05T02:40:30.209364+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2011.10001","created_at":"2026-07-05T02:40:30.209364+00:00"},{"alias_kind":"pith_short_12","alias_value":"FCDQ3Q2JCWXU","created_at":"2026-07-05T02:40:30.209364+00:00"},{"alias_kind":"pith_short_16","alias_value":"FCDQ3Q2JCWXUPOD2","created_at":"2026-07-05T02:40:30.209364+00:00"},{"alias_kind":"pith_short_8","alias_value":"FCDQ3Q2J","created_at":"2026-07-05T02:40:30.209364+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2607.08482","citing_title":"Quantum corrections to the near-extremal thermodynamics of (warped) BTZ black holes","ref_index":68,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/FCDQ3Q2JCWXUPOD2IE7TF7EDFM","json":"https://pith.science/pith/FCDQ3Q2JCWXUPOD2IE7TF7EDFM.json","graph_json":"https://pith.science/api/pith-number/FCDQ3Q2JCWXUPOD2IE7TF7EDFM/graph.json","events_json":"https://pith.science/api/pith-number/FCDQ3Q2JCWXUPOD2IE7TF7EDFM/events.json","paper":"https://pith.science/paper/FCDQ3Q2J"},"agent_actions":{"view_html":"https://pith.science/pith/FCDQ3Q2JCWXUPOD2IE7TF7EDFM","download_json":"https://pith.science/pith/FCDQ3Q2JCWXUPOD2IE7TF7EDFM.json","view_paper":"https://pith.science/paper/FCDQ3Q2J","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2011.10001&json=true","fetch_graph":"https://pith.science/api/pith-number/FCDQ3Q2JCWXUPOD2IE7TF7EDFM/graph.json","fetch_events":"https://pith.science/api/pith-number/FCDQ3Q2JCWXUPOD2IE7TF7EDFM/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FCDQ3Q2JCWXUPOD2IE7TF7EDFM/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FCDQ3Q2JCWXUPOD2IE7TF7EDFM/action/storage_attestation","attest_author":"https://pith.science/pith/FCDQ3Q2JCWXUPOD2IE7TF7EDFM/action/author_attestation","sign_citation":"https://pith.science/pith/FCDQ3Q2JCWXUPOD2IE7TF7EDFM/action/citation_signature","submit_replication":"https://pith.science/pith/FCDQ3Q2JCWXUPOD2IE7TF7EDFM/action/replication_record"}},"created_at":"2026-07-05T02:40:30.209364+00:00","updated_at":"2026-07-05T02:40:30.209364+00:00"}