{"paper":{"title":"The Large N Limit of Superconformal Field Theories and Supergravity","license":"","headline":"The large N limit of certain superconformal field theories contains a sector describing supergravity on Anti-de Sitter space times spheres.","cross_cats":[],"primary_cat":"hep-th","authors_text":"Juan M. Maldacena","submitted_at":"1997-11-27T23:53:13Z","abstract_excerpt":"We show that the large $N$ limit of certain conformal field theories in various dimensions include in their Hilbert space a sector describing supergravity on the product of Anti-deSitter spacetimes, spheres and other compact manifolds. This is shown by taking some branes in the full M/string theory and then taking a low energy limit where the field theory on the brane decouples from the bulk. We observe that, in this limit, we can still trust the near horizon geometry for large $N$. The enhanced supersymmetries of the near horizon geometry correspond to the extra supersymmetry generators prese"},"claims":{"count":4,"items":[{"kind":"strongest_claim","text":"We conjecture that compactifications of M/string theory on various Anti-deSitter spacetimes are dual to various conformal field theories.","source":"verdict.strongest_claim","status":"machine_extracted","claim_id":"C1","attestation":"unclaimed"},{"kind":"weakest_assumption","text":"That the low energy limit decouples the brane field theory from the bulk while still allowing trust in the near-horizon supergravity geometry for large N.","source":"verdict.weakest_assumption","status":"machine_extracted","claim_id":"C2","attestation":"unclaimed"},{"kind":"one_line_summary","text":"The large N limit of superconformal field theories is dual to supergravity on Anti-de Sitter spacetimes.","source":"verdict.one_line_summary","status":"machine_extracted","claim_id":"C3","attestation":"unclaimed"},{"kind":"headline","text":"The large N limit of certain superconformal field theories contains a sector describing supergravity on Anti-de Sitter space times spheres.","source":"verdict.pith_extraction.headline","status":"machine_extracted","claim_id":"C4","attestation":"unclaimed"}],"snapshot_sha256":"3f944e544e7bae9fb5a8f21a96a68dd1c0d7ef9e57e959e15b29625082fb341c"},"source":{"id":"hep-th/9711200","kind":"arxiv","version":3},"verdict":{"id":"ed0f9fd1-f230-45b8-849f-855cb75be2a0","model_set":{"reader":"grok-4.3"},"created_at":"2026-05-10T16:36:57.461330Z","strongest_claim":"We conjecture that compactifications of M/string theory on various Anti-deSitter spacetimes are dual to various conformal field theories.","one_line_summary":"The large N limit of superconformal field theories is dual to supergravity on Anti-de Sitter spacetimes.","pipeline_version":"pith-pipeline@v0.9.0","weakest_assumption":"That the low energy limit decouples the brane field theory from the bulk while still allowing trust in the near-horizon supergravity geometry for large N.","pith_extraction_headline":"The large N limit of certain superconformal field theories contains a sector describing supergravity on Anti-de Sitter space times spheres."},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-th/9711200/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":65,"sample":[{"doi":"","year":null,"title":"Semiclassical decay of near extremal fivebranes","work_id":"44207544-5ebe-4d78-91a4-990316840439","ref_index":1,"cited_arxiv_id":"hep-th/9710014","is_internal_anchor":false},{"doi":"","year":1997,"title":"Matrix Description of M-theory on $T^5$ and $T^5/Z_2$","work_id":"8dfde2bf-89a3-424a-ad89-c101ea5b3abe","ref_index":2,"cited_arxiv_id":"hep-th/9705221","is_internal_anchor":false},{"doi":"","year":1975,"title":"R. Haag, J. Lopuszanski and M. Sohnius, Nucl. Phys. B88 (1975) 257","work_id":"bfcf0ce0-f329-4f93-8c6f-471cbc7e2ed8","ref_index":3,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":1978,"title":"W. Nahm, Nucl. Phys. B135 (1978) 149","work_id":"90c0d1a9-4b69-4e8d-aec2-5f0a46425c7e","ref_index":4,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":1982,"title":"G. Gibbons, Nucl. Phys. B207, (1982) 337; R. Kallosh and A. Peet, Phys. Rev. D46 (1992) 5223, hep-th/9209116; S. Ferrara, G. Gibbons, R. Kal losh, Nucl. Phys. B500 (1997) 75, hep-th/9702103","work_id":"97e74662-b262-4fa5-9a8e-787160fde1b8","ref_index":5,"cited_arxiv_id":"hep-th/9209116","is_internal_anchor":true}],"resolved_work":65,"snapshot_sha256":"111c7ba19e655afed7622fd9c582106ac9656074ddbfa91a0f30c976b013b4ef","internal_anchors":17},"formal_canon":{"evidence_count":3,"snapshot_sha256":"b0cbfee5e3d133ea6ddd47cec5760cdd8d1edf6eaaa98e38f476d0fc401a62ae"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"}