{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1998:UWVJ7PNJCGM6GNMQZNY3AML2KA","short_pith_number":"pith:UWVJ7PNJ","schema_version":"1.0","canonical_sha256":"a5aa9fbda91199e33590cb71b0317a500457d23a3f1710f4126f787bca7c6e01","source":{"kind":"arxiv","id":"hep-th/9802109","version":2},"attestation_state":"computed","paper":{"title":"Gauge Theory Correlators from Non-Critical String Theory","license":"","headline":"Gauge theory correlators are extracted from how the supergravity action in anti-de Sitter space depends on boundary conditions.","cross_cats":[],"primary_cat":"hep-th","authors_text":"A.M. Polyakov, I.R. Klebanov, S.S. Gubser","submitted_at":"1998-02-16T18:38:17Z","abstract_excerpt":"We suggest a means of obtaining certain Green's functions in 3+1-dimensional ${\\cal N} = 4$ supersymmetric Yang-Mills theory with a large number of colors via non-critical string theory. The non-critical string theory is related to critical string theory in anti-deSitter background. We introduce a boundary of the anti-deSitter space analogous to a cut-off on the Liouville coordinate of the two-dimensional string theory. Correlation functions of operators in the gauge theory are related to the dependence of the supergravity action on the boundary conditions. From the quadratic terms in supergra"},"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":true,"formal_links_present":true},"canonical_record":{"source":{"id":"hep-th/9802109","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1998-02-16T18:38:17Z","cross_cats_sorted":[],"title_canon_sha256":"1f34a30ef8be57566694324e0fce2395c601bbe66a54fa6813eaf2eff1008cd5","abstract_canon_sha256":"4947f9c07120e929af77897c5b83ad7b8cdb020cc31e9fea0ad35b657cfd4c66"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:32:30.271142Z","signature_b64":"e2T7xswbDuyXyTLaNZIeYcs42YF81Bgz9fSJ7L0YG0ASu9+OuXWFtpEraCLgntAq9V0/GUU++oQP3PXrTc/BDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a5aa9fbda91199e33590cb71b0317a500457d23a3f1710f4126f787bca7c6e01","last_reissued_at":"2026-07-04T15:32:30.270721Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:32:30.270721Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Gauge Theory Correlators from Non-Critical String Theory","license":"","headline":"Gauge theory correlators are extracted from how the supergravity action in anti-de Sitter space depends on boundary conditions.","cross_cats":[],"primary_cat":"hep-th","authors_text":"A.M. Polyakov, I.R. Klebanov, S.S. Gubser","submitted_at":"1998-02-16T18:38:17Z","abstract_excerpt":"We suggest a means of obtaining certain Green's functions in 3+1-dimensional ${\\cal N} = 4$ supersymmetric Yang-Mills theory with a large number of colors via non-critical string theory. The non-critical string theory is related to critical string theory in anti-deSitter background. We introduce a boundary of the anti-deSitter space analogous to a cut-off on the Liouville coordinate of the two-dimensional string theory. Correlation functions of operators in the gauge theory are related to the dependence of the supergravity action on the boundary conditions. From the quadratic terms in supergra"},"claims":{"count":4,"items":[{"kind":"strongest_claim","text":"The operators that couple to massive string states at level n acquire anomalous dimensions that grow as 2 (n g_YM sqrt(2 N))^{1/2} for large 't Hooft coupling. This is a new prediction about the strong coupling behavior of large N SYM theory.","source":"verdict.strongest_claim","status":"machine_extracted","claim_id":"C1","attestation":"unclaimed"},{"kind":"weakest_assumption","text":"The non-critical string theory is related to critical string theory in anti-de Sitter background, with a boundary analogous to a Liouville cut-off, and gauge theory correlation functions are given by the dependence of the supergravity action on boundary conditions.","source":"verdict.weakest_assumption","status":"machine_extracted","claim_id":"C2","attestation":"unclaimed"},{"kind":"one_line_summary","text":"Gauge theory correlators in 3+1D N=4 SYM with large N are obtained from the supergravity action on the AdS boundary, with anomalous dimensions for massive string modes growing as 2(n g_YM sqrt(2N))^{1/2} at strong 't Hooft coupling.","source":"verdict.one_line_summary","status":"machine_extracted","claim_id":"C3","attestation":"unclaimed"},{"kind":"headline","text":"Gauge theory correlators are extracted from how the supergravity action in anti-de Sitter space depends on boundary conditions.","source":"verdict.pith_extraction.headline","status":"machine_extracted","claim_id":"C4","attestation":"unclaimed"}],"snapshot_sha256":"023d7f8f2532f904392c1d3540ef56767b0b093082a78bcbb3e3257da531be35"},"source":{"id":"hep-th/9802109","kind":"arxiv","version":2},"verdict":{"id":"29c02aad-61fa-4efe-880c-5010fde9672f","model_set":{"reader":"grok-4.3"},"created_at":"2026-05-11T15:52:09.773353Z","strongest_claim":"The operators that couple to massive string states at level n acquire anomalous dimensions that grow as 2 (n g_YM sqrt(2 N))^{1/2} for large 't Hooft coupling. This is a new prediction about the strong coupling behavior of large N SYM theory.","one_line_summary":"Gauge theory correlators in 3+1D N=4 SYM with large N are obtained from the supergravity action on the AdS boundary, with anomalous dimensions for massive string modes growing as 2(n g_YM sqrt(2N))^{1/2} at strong 't Hooft coupling.","pipeline_version":"pith-pipeline@v0.9.0","weakest_assumption":"The non-critical string theory is related to critical string theory in anti-de Sitter background, with a boundary analogous to a Liouville cut-off, and gauge theory correlation functions are given by the dependence of the supergravity action on boundary conditions.","pith_extraction_headline":"Gauge theory correlators are extracted from how the supergravity action in anti-de Sitter space depends on boundary conditions."},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-th/9802109/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":24,"sample":[{"doi":"","year":1980,"title":"Gauge Fields as Rings of Glue","work_id":"36fb3c61-73de-4996-94cf-c0a587c720a4","ref_index":1,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":1979,"title":"Exact Equation for the Lo op Average in Mul- ticolor QCD","work_id":"52cd698d-fbc8-450c-9d4d-fd080c69ca9d","ref_index":2,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":1974,"title":"A planar diagram theory for strong interact ions","work_id":"6c48e883-60be-4e03-bb9a-987632e969c3","ref_index":3,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":null,"title":"String theory and quark conﬁnement","work_id":"95ba559d-7161-4665-9f1b-312b3198df77","ref_index":4,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":1985,"title":"Eﬀective Field Theory f rom Quantized Strings","work_id":"4f593ae0-3884-4a69-8865-da37849a14bd","ref_index":5,"cited_arxiv_id":"","is_internal_anchor":false}],"resolved_work":24,"snapshot_sha256":"b775a95cb8bfe1859c644126dfb4fe43b1ab98e5d52c53ae7ca5c92826a93104","internal_anchors":1},"formal_canon":{"evidence_count":2,"snapshot_sha256":"2f90907784d8224d5fbf5c6094546852ea519269ae6c93fcc4afc915a72a7de0"},"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/9802109","created_at":"2026-07-04T15:32:30.270786+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9802109v2","created_at":"2026-07-04T15:32:30.270786+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9802109","created_at":"2026-07-04T15:32:30.270786+00:00"},{"alias_kind":"pith_short_12","alias_value":"UWVJ7PNJCGM6","created_at":"2026-07-04T15:32:30.270786+00:00"},{"alias_kind":"pith_short_16","alias_value":"UWVJ7PNJCGM6GNMQ","created_at":"2026-07-04T15:32:30.270786+00:00"},{"alias_kind":"pith_short_8","alias_value":"UWVJ7PNJ","created_at":"2026-07-04T15:32:30.270786+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":170,"internal_anchor_count":170,"sample":[{"citing_arxiv_id":"2607.08481","citing_title":"Gram--Wishart--Stiefel formulation of the $N=2$, large--$d$ gauge theory in 1D","ref_index":23,"is_internal_anchor":true},{"citing_arxiv_id":"2607.08737","citing_title":"The mini-Page Curve in Cosmology","ref_index":30,"is_internal_anchor":true},{"citing_arxiv_id":"2607.08684","citing_title":"Entanglement Wedge Reconstruction without Holographic Quantum Error Correction","ref_index":2,"is_internal_anchor":true},{"citing_arxiv_id":"2607.06867","citing_title":"On Integrable Structures on Non-compact Boundaries in Three-Dimensional Gravity","ref_index":72,"is_internal_anchor":true},{"citing_arxiv_id":"2607.06870","citing_title":"Phase transitions and uberholography of holographic pure-state geometries","ref_index":3,"is_internal_anchor":true},{"citing_arxiv_id":"2606.24382","citing_title":"Exact and Finite de Sitter QFT from CFT","ref_index":3,"is_internal_anchor":true},{"citing_arxiv_id":"2606.24328","citing_title":"Holographic Entanglement Anisotropy as a Dark Deformation RG Probe in Hyperscaling-Violating $p$-Wave Superfluids","ref_index":2,"is_internal_anchor":true},{"citing_arxiv_id":"2606.24285","citing_title":"Topics in Celestial holography: A bottom-up perspective","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":86,"is_internal_anchor":true},{"citing_arxiv_id":"2606.26241","citing_title":"An observer's quantization of 3d de Sitter","ref_index":107,"is_internal_anchor":true},{"citing_arxiv_id":"2606.26163","citing_title":"Large-$N$ Carrollian Thermodynamics from AdS Black-Hole Phase-Space Contractions","ref_index":10,"is_internal_anchor":true},{"citing_arxiv_id":"2606.23779","citing_title":"Excitability of Gaussian states with VEVs","ref_index":13,"is_internal_anchor":true},{"citing_arxiv_id":"2606.22679","citing_title":"On the temperature dependence of quasinormal modes in SYK and holography","ref_index":3,"is_internal_anchor":true},{"citing_arxiv_id":"2606.22598","citing_title":"When does a state-dependent proto-area define a bulk geometry?","ref_index":2,"is_internal_anchor":true},{"citing_arxiv_id":"2606.21662","citing_title":"On the Universality of Probe Complexity in $\\mathcal{N}=4$ SYM","ref_index":3,"is_internal_anchor":true},{"citing_arxiv_id":"2606.21537","citing_title":"Near-horizon modifications in finite $N$ holography","ref_index":2,"is_internal_anchor":true},{"citing_arxiv_id":"2606.21081","citing_title":"The Entanglement Wedge Polygon","ref_index":4,"is_internal_anchor":true},{"citing_arxiv_id":"2606.21079","citing_title":"Linear Growth of Holographic Time-like Entanglement Entropy and Kasner exponents","ref_index":2,"is_internal_anchor":true},{"citing_arxiv_id":"2606.20981","citing_title":"Gluon GTMD at strong coupling: fixed-spin saddle factorization and Reggeization","ref_index":39,"is_internal_anchor":true},{"citing_arxiv_id":"2606.18929","citing_title":"Higher-Trace Operators and Cut Diagrammatics in the Conformal Block Expansion","ref_index":3,"is_internal_anchor":true},{"citing_arxiv_id":"2606.18629","citing_title":"Holographic Dual of PT Symmetric BCFT","ref_index":43,"is_internal_anchor":true},{"citing_arxiv_id":"2606.24285","citing_title":"Topics in Celestial holography: A bottom-up perspective","ref_index":4,"is_internal_anchor":true},{"citing_arxiv_id":"2606.17909","citing_title":"A Lindbladian for holographic Brownian motion","ref_index":2,"is_internal_anchor":true},{"citing_arxiv_id":"2606.17758","citing_title":"A Double--Scaling Large--\\(d\\) Saddle of BFSS/BMN Matrix Quantum Mechanics","ref_index":23,"is_internal_anchor":true},{"citing_arxiv_id":"2606.17719","citing_title":"Aspects of Witten Diagrams for Holographic Defects","ref_index":3,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":2,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/UWVJ7PNJCGM6GNMQZNY3AML2KA","json":"https://pith.science/pith/UWVJ7PNJCGM6GNMQZNY3AML2KA.json","graph_json":"https://pith.science/api/pith-number/UWVJ7PNJCGM6GNMQZNY3AML2KA/graph.json","events_json":"https://pith.science/api/pith-number/UWVJ7PNJCGM6GNMQZNY3AML2KA/events.json","paper":"https://pith.science/paper/UWVJ7PNJ"},"agent_actions":{"view_html":"https://pith.science/pith/UWVJ7PNJCGM6GNMQZNY3AML2KA","download_json":"https://pith.science/pith/UWVJ7PNJCGM6GNMQZNY3AML2KA.json","view_paper":"https://pith.science/paper/UWVJ7PNJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9802109&json=true","fetch_graph":"https://pith.science/api/pith-number/UWVJ7PNJCGM6GNMQZNY3AML2KA/graph.json","fetch_events":"https://pith.science/api/pith-number/UWVJ7PNJCGM6GNMQZNY3AML2KA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UWVJ7PNJCGM6GNMQZNY3AML2KA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UWVJ7PNJCGM6GNMQZNY3AML2KA/action/storage_attestation","attest_author":"https://pith.science/pith/UWVJ7PNJCGM6GNMQZNY3AML2KA/action/author_attestation","sign_citation":"https://pith.science/pith/UWVJ7PNJCGM6GNMQZNY3AML2KA/action/citation_signature","submit_replication":"https://pith.science/pith/UWVJ7PNJCGM6GNMQZNY3AML2KA/action/replication_record"}},"created_at":"2026-07-04T15:32:30.270786+00:00","updated_at":"2026-07-04T15:32:30.270786+00:00"}