{"metadata":{"publication_info":[{"year":1999,"material":"reprint","page_end":"1133","page_start":"1113","journal_title":"Int.J.Theor.Phys.","journal_record":{"$ref":"https://inspirehep.net/api/journals/1214707"},"journal_volume":"38"},{"year":1998,"material":"publication","page_end":"252","page_start":"231","journal_title":"Adv.Theor.Math.Phys.","journal_record":{"$ref":"https://inspirehep.net/api/journals/1212914"},"journal_volume":"2"}],"report_numbers":[{"value":"HUTP-97-A097"},{"value":"HUTP-98-A097"}],"citation_count_without_self_citations":21979,"citation_count":22036,"core":true,"dois":[{"value":"10.4310/ATMP.1998.v2.n2.a1","source":"International Press","material":"publication"},{"value":"10.1023/A:1026654312961","material":"reprint"}],"titles":[{"title":"The Large $N$ limit of superconformal field theories and supergravity"},{"title":"The large N limit of superconformal field theories and supergravity.","source":"arXiv"},{"title":"The Large N Limit of Superconformal Field Theories and Supergravity","source":"arXiv"}],"$schema":"https://inspirehep.net/schemas/records/hep.json","authors":[{"ids":[{"value":"INSPIRE-00304313","schema":"INSPIRE ID"}],"uuid":"2a189c7c-eadf-4b47-8a2b-e71e3dcec326","record":{"$ref":"https://inspirehep.net/api/authors/999108"},"full_name":"Maldacena, Juan Martin","affiliations":[{"value":"Harvard U.","record":{"$ref":"https://inspirehep.net/api/institutions/902835"}}],"signature_block":"MALDACANj","curated_relation":true}],"curated":true,"texkeys":["Maldacena:1997re"],"citeable":true,"keywords":[{"value":"field theory: conformal","schema":"INSPIRE"},{"value":"expansion 1/N","schema":"INSPIRE"},{"value":"supergravity","schema":"INSPIRE"},{"value":"Hilbert space","schema":"INSPIRE"},{"value":"space-time: anti-de Sitter","schema":"INSPIRE"},{"value":"membrane model","schema":"INSPIRE"},{"value":"string model","schema":"INSPIRE"},{"value":"geometry: horizon","schema":"INSPIRE"},{"value":"gauge field theory: U(N)","schema":"INSPIRE"},{"value":"supersymmetry","schema":"INSPIRE"},{"value":"duality","schema":"INSPIRE"},{"value":"M-theory","schema":"INSPIRE"},{"value":"bibliography","schema":"INSPIRE"},{"value":"AdS/CFT correspondence","schema":"INSPIRE"}],"refereed":true,"abstracts":[{"value":"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 present in the superconformal group (as opposed to just the super-Poincare group). The 't Hooft limit of 4-d ${\\cal N} =4$ super-Yang-Mills at the conformal point is shown to contain strings: they are IIB strings. We conjecture that compactifications of M/string theory on various Anti-deSitter spacetimes are dual to various conformal field theories. This leads to a new proposal for a definition of M-theory which could be extended to include five non-compact dimensions.","source":"arXiv"}],"references":[{"record":{"$ref":"https://inspirehep.net/api/literature/449261"},"raw_refs":[{"value":"[1] J. Maldacena and A. 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