{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:RHPUZXR2WRL3KTUF7CSFJ6YJWI","short_pith_number":"pith:RHPUZXR2","schema_version":"1.0","canonical_sha256":"89df4cde3ab457b54e85f8a454fb09b20eac5b7e56a91f07567e8d3cfa328d54","source":{"kind":"arxiv","id":"2311.04883","version":3},"attestation_state":"computed","paper":{"title":"Extremal surfaces in glue-on AdS/$T\\bar T$ holography","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Luis Apolo, Peng-Xiang Hao, Wei Song, Wen-Xin Lai","submitted_at":"2023-11-08T18:40:55Z","abstract_excerpt":"$T\\bar T$ deformed CFTs with positive deformation parameter have been proposed to be holographically dual to Einstein gravity in a glue-on $\\mathrm{AdS}_3$ spacetime. The latter is constructed from AdS$_3$ by gluing a patch of an auxiliary AdS$_3^*$ spacetime to its asymptotic boundary. In this work, we propose a glue-on version of the Ryu-Takayanagi formula, which is given by the signed area of an extremal surface. The extremal surface is anchored at the endpoints of an interval on a cutoff surface in the glue-on geometry. It consists of an RT surface lying in the AdS$_3$ part of the spacetim"},"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":"2311.04883","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2023-11-08T18:40:55Z","cross_cats_sorted":[],"title_canon_sha256":"6255315c2fd243afae946eb7f2273c912f8a39f8e753150c2a3585c134129356","abstract_canon_sha256":"009e7264bb62bb28e9b8f546a8bcd4107c5ee14751250b67f9fe895e1916c05a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:38:32.297528Z","signature_b64":"5pIr6jLwBxURrWIkzIAdpgdE3NiIZbq5ng3/+QSQkYHJoWA12wxyhSY83qHLgsknBWjhA0oXsehD1BgbHfMZBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"89df4cde3ab457b54e85f8a454fb09b20eac5b7e56a91f07567e8d3cfa328d54","last_reissued_at":"2026-07-05T07:38:32.297113Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:38:32.297113Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Extremal surfaces in glue-on AdS/$T\\bar T$ holography","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Luis Apolo, Peng-Xiang Hao, Wei Song, Wen-Xin Lai","submitted_at":"2023-11-08T18:40:55Z","abstract_excerpt":"$T\\bar T$ deformed CFTs with positive deformation parameter have been proposed to be holographically dual to Einstein gravity in a glue-on $\\mathrm{AdS}_3$ spacetime. The latter is constructed from AdS$_3$ by gluing a patch of an auxiliary AdS$_3^*$ spacetime to its asymptotic boundary. In this work, we propose a glue-on version of the Ryu-Takayanagi formula, which is given by the signed area of an extremal surface. The extremal surface is anchored at the endpoints of an interval on a cutoff surface in the glue-on geometry. It consists of an RT surface lying in the AdS$_3$ part of the spacetim"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2311.04883","kind":"arxiv","version":3},"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/2311.04883/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":"2311.04883","created_at":"2026-07-05T07:38:32.297168+00:00"},{"alias_kind":"arxiv_version","alias_value":"2311.04883v3","created_at":"2026-07-05T07:38:32.297168+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2311.04883","created_at":"2026-07-05T07:38:32.297168+00:00"},{"alias_kind":"pith_short_12","alias_value":"RHPUZXR2WRL3","created_at":"2026-07-05T07:38:32.297168+00:00"},{"alias_kind":"pith_short_16","alias_value":"RHPUZXR2WRL3KTUF","created_at":"2026-07-05T07:38:32.297168+00:00"},{"alias_kind":"pith_short_8","alias_value":"RHPUZXR2","created_at":"2026-07-05T07:38:32.297168+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2602.06113","citing_title":"Deforming the Double-Scaled SYK & Reaching the Stretched Horizon From Finite Cutoff Holography","ref_index":24,"is_internal_anchor":false},{"citing_arxiv_id":"2605.12616","citing_title":"Butterflies in $\\textrm{T}\\overline{\\textrm{T}}$ deformed anomalous CFT$_2$","ref_index":25,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/RHPUZXR2WRL3KTUF7CSFJ6YJWI","json":"https://pith.science/pith/RHPUZXR2WRL3KTUF7CSFJ6YJWI.json","graph_json":"https://pith.science/api/pith-number/RHPUZXR2WRL3KTUF7CSFJ6YJWI/graph.json","events_json":"https://pith.science/api/pith-number/RHPUZXR2WRL3KTUF7CSFJ6YJWI/events.json","paper":"https://pith.science/paper/RHPUZXR2"},"agent_actions":{"view_html":"https://pith.science/pith/RHPUZXR2WRL3KTUF7CSFJ6YJWI","download_json":"https://pith.science/pith/RHPUZXR2WRL3KTUF7CSFJ6YJWI.json","view_paper":"https://pith.science/paper/RHPUZXR2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2311.04883&json=true","fetch_graph":"https://pith.science/api/pith-number/RHPUZXR2WRL3KTUF7CSFJ6YJWI/graph.json","fetch_events":"https://pith.science/api/pith-number/RHPUZXR2WRL3KTUF7CSFJ6YJWI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RHPUZXR2WRL3KTUF7CSFJ6YJWI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RHPUZXR2WRL3KTUF7CSFJ6YJWI/action/storage_attestation","attest_author":"https://pith.science/pith/RHPUZXR2WRL3KTUF7CSFJ6YJWI/action/author_attestation","sign_citation":"https://pith.science/pith/RHPUZXR2WRL3KTUF7CSFJ6YJWI/action/citation_signature","submit_replication":"https://pith.science/pith/RHPUZXR2WRL3KTUF7CSFJ6YJWI/action/replication_record"}},"created_at":"2026-07-05T07:38:32.297168+00:00","updated_at":"2026-07-05T07:38:32.297168+00:00"}