{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1998:TKMKLYFNXMK53L6TK52MVP46A7","short_pith_number":"pith:TKMKLYFN","schema_version":"1.0","canonical_sha256":"9a98a5e0adbb15ddafd35774cabf9e07f91ba0da9eca4c15c9425eddee27f90d","source":{"kind":"arxiv","id":"hep-th/9808016","version":1},"attestation_state":"computed","paper":{"title":"AdS Dynamics from Conformal Field Theory","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Emil Martinec, Gary T. Horowitz, Michael R. Douglas, Tom Banks","submitted_at":"1998-08-04T21:49:51Z","abstract_excerpt":"We explore the extent to which a local string theory dynamics in anti-de Sitter space can be determined from its proposed Conformal Field Theory (CFT) description. Free fields in the bulk are constructed from the CFT operators, but difficulties are encountered when one attempts to incorporate interactions. We also discuss general features of black hole dynamics as seen from the CFT perspective. In particular, we argue that the singularity of AdS_3 black holes is resolved in the CFT description."},"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":"hep-th/9808016","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1998-08-04T21:49:51Z","cross_cats_sorted":[],"title_canon_sha256":"64dd4df34a20be881afc544da64ea4abd579112306e8efa21ce0981e73c85e2c","abstract_canon_sha256":"ee01a0b6fbd1ef0aafb43ae0caf2fd06ddae18e4683c29e60fc2f2362b736fd6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:33:14.820238Z","signature_b64":"84Z8bNgpMYE8uq+jiR9OJweO3AUoc/CAEtKngb6cqJVqEzYiIQX4yOLS7TkvIPdS1uMJoj8s6qUgmbzuChnPDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9a98a5e0adbb15ddafd35774cabf9e07f91ba0da9eca4c15c9425eddee27f90d","last_reissued_at":"2026-07-04T14:33:14.819847Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:33:14.819847Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"AdS Dynamics from Conformal Field Theory","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Emil Martinec, Gary T. Horowitz, Michael R. Douglas, Tom Banks","submitted_at":"1998-08-04T21:49:51Z","abstract_excerpt":"We explore the extent to which a local string theory dynamics in anti-de Sitter space can be determined from its proposed Conformal Field Theory (CFT) description. Free fields in the bulk are constructed from the CFT operators, but difficulties are encountered when one attempts to incorporate interactions. We also discuss general features of black hole dynamics as seen from the CFT perspective. In particular, we argue that the singularity of AdS_3 black holes is resolved in the CFT description."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9808016","kind":"arxiv","version":1},"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/hep-th/9808016/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":"hep-th/9808016","created_at":"2026-07-04T14:33:14.819902+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9808016v1","created_at":"2026-07-04T14:33:14.819902+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9808016","created_at":"2026-07-04T14:33:14.819902+00:00"},{"alias_kind":"pith_short_12","alias_value":"TKMKLYFNXMK5","created_at":"2026-07-04T14:33:14.819902+00:00"},{"alias_kind":"pith_short_16","alias_value":"TKMKLYFNXMK53L6T","created_at":"2026-07-04T14:33:14.819902+00:00"},{"alias_kind":"pith_short_8","alias_value":"TKMKLYFN","created_at":"2026-07-04T14:33:14.819902+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":10,"internal_anchor_count":7,"sample":[{"citing_arxiv_id":"2607.08684","citing_title":"Entanglement Wedge Reconstruction without Holographic Quantum Error Correction","ref_index":4,"is_internal_anchor":true},{"citing_arxiv_id":"2606.26302","citing_title":"Dirichlet, Neumann, Mixed and self-dual holography: (self-dual) Yang--Mills theory II","ref_index":85,"is_internal_anchor":true},{"citing_arxiv_id":"2606.30797","citing_title":"On Black Holes Surrounded by Radiation II: Thermodynamics","ref_index":48,"is_internal_anchor":true},{"citing_arxiv_id":"2605.25481","citing_title":"Bulk Motion in Global AdS$_3$ from the Boundary Energy-Density Perspective","ref_index":31,"is_internal_anchor":true},{"citing_arxiv_id":"2309.04231","citing_title":"Subregion Complementarity in AdS/CFT","ref_index":5,"is_internal_anchor":true},{"citing_arxiv_id":"2605.16641","citing_title":"On bulk reconstruction in Lorentzian AdS and its flat space limit","ref_index":6,"is_internal_anchor":true},{"citing_arxiv_id":"2508.20094","citing_title":"(Un)solvable Matrix Models for BPS Correlators","ref_index":2,"is_internal_anchor":true},{"citing_arxiv_id":"2605.03155","citing_title":"Flat Space Physics from AdS Actions","ref_index":1,"is_internal_anchor":false},{"citing_arxiv_id":"2605.03037","citing_title":"Generalized Free Fields in de Sitter from 1D CFT","ref_index":12,"is_internal_anchor":false},{"citing_arxiv_id":"2605.06780","citing_title":"A Semiclassical Diagnostic for Spacetime Emergence","ref_index":6,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/TKMKLYFNXMK53L6TK52MVP46A7","json":"https://pith.science/pith/TKMKLYFNXMK53L6TK52MVP46A7.json","graph_json":"https://pith.science/api/pith-number/TKMKLYFNXMK53L6TK52MVP46A7/graph.json","events_json":"https://pith.science/api/pith-number/TKMKLYFNXMK53L6TK52MVP46A7/events.json","paper":"https://pith.science/paper/TKMKLYFN"},"agent_actions":{"view_html":"https://pith.science/pith/TKMKLYFNXMK53L6TK52MVP46A7","download_json":"https://pith.science/pith/TKMKLYFNXMK53L6TK52MVP46A7.json","view_paper":"https://pith.science/paper/TKMKLYFN","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9808016&json=true","fetch_graph":"https://pith.science/api/pith-number/TKMKLYFNXMK53L6TK52MVP46A7/graph.json","fetch_events":"https://pith.science/api/pith-number/TKMKLYFNXMK53L6TK52MVP46A7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TKMKLYFNXMK53L6TK52MVP46A7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TKMKLYFNXMK53L6TK52MVP46A7/action/storage_attestation","attest_author":"https://pith.science/pith/TKMKLYFNXMK53L6TK52MVP46A7/action/author_attestation","sign_citation":"https://pith.science/pith/TKMKLYFNXMK53L6TK52MVP46A7/action/citation_signature","submit_replication":"https://pith.science/pith/TKMKLYFNXMK53L6TK52MVP46A7/action/replication_record"}},"created_at":"2026-07-04T14:33:14.819902+00:00","updated_at":"2026-07-04T14:33:14.819902+00:00"}