{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1998:UWVJ7PNJCGM6GNMQZNY3AML2KA","short_pith_number":"pith:UWVJ7PNJ","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"},"canonical_sha256":"a5aa9fbda91199e33590cb71b0317a500457d23a3f1710f4126f787bca7c6e01","source":{"kind":"arxiv","id":"hep-th/9802109","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/9802109","created_at":"2026-07-04T15:32:30Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9802109v2","created_at":"2026-07-04T15:32:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9802109","created_at":"2026-07-04T15:32:30Z"},{"alias_kind":"pith_short_12","alias_value":"UWVJ7PNJCGM6","created_at":"2026-07-04T15:32:30Z"},{"alias_kind":"pith_short_16","alias_value":"UWVJ7PNJCGM6GNMQ","created_at":"2026-07-04T15:32:30Z"},{"alias_kind":"pith_short_8","alias_value":"UWVJ7PNJ","created_at":"2026-07-04T15:32:30Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1998:UWVJ7PNJCGM6GNMQZNY3AML2KA","target":"record","payload":{"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"},"canonical_sha256":"a5aa9fbda91199e33590cb71b0317a500457d23a3f1710f4126f787bca7c6e01","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"},"source_kind":"arxiv","source_id":"hep-th/9802109","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T15:32:30Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"JHd6m1s1a+BrhxyjLtpjM7GP01wXjDUiJtlfBemrD+A0LXx+DWfsh4L+xS/1iSEC5+qu36QQ1WiPR/9BzDz6Aw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-14T03:23:34.959721Z"},"content_sha256":"1af42edbaa2b5554d25a17149ca9b7434df50af82bfbcbac75b8061d0d7e7df0","schema_version":"1.0","event_id":"sha256:1af42edbaa2b5554d25a17149ca9b7434df50af82bfbcbac75b8061d0d7e7df0"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1998:UWVJ7PNJCGM6GNMQZNY3AML2KA","target":"graph","payload":{"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"},"verdict_id":"29c02aad-61fa-4efe-880c-5010fde9672f"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T15:32:30Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"w3pb7oWStrdY5V02kxaaIJ1X5xDPJudN9XPEF9gesdeB+pw8WhjgpJmyXut4ydnlaoyOAtqW4C+e8NcEikmeBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-14T03:23:34.961161Z"},"content_sha256":"713748460535ac73c2694cd258485fec0db6e1df65d74c53d77f9f0c8f83b9ae","schema_version":"1.0","event_id":"sha256:713748460535ac73c2694cd258485fec0db6e1df65d74c53d77f9f0c8f83b9ae"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/UWVJ7PNJCGM6GNMQZNY3AML2KA/bundle.json","state_url":"https://pith.science/pith/UWVJ7PNJCGM6GNMQZNY3AML2KA/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/UWVJ7PNJCGM6GNMQZNY3AML2KA/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-08-14T03:23:34Z","links":{"resolver":"https://pith.science/pith/UWVJ7PNJCGM6GNMQZNY3AML2KA","bundle":"https://pith.science/pith/UWVJ7PNJCGM6GNMQZNY3AML2KA/bundle.json","state":"https://pith.science/pith/UWVJ7PNJCGM6GNMQZNY3AML2KA/state.json","well_known_bundle":"https://pith.science/.well-known/pith/UWVJ7PNJCGM6GNMQZNY3AML2KA/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1998:UWVJ7PNJCGM6GNMQZNY3AML2KA","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"4947f9c07120e929af77897c5b83ad7b8cdb020cc31e9fea0ad35b657cfd4c66","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"1998-02-16T18:38:17Z","title_canon_sha256":"1f34a30ef8be57566694324e0fce2395c601bbe66a54fa6813eaf2eff1008cd5"},"schema_version":"1.0","source":{"id":"hep-th/9802109","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/9802109","created_at":"2026-07-04T15:32:30Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9802109v2","created_at":"2026-07-04T15:32:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9802109","created_at":"2026-07-04T15:32:30Z"},{"alias_kind":"pith_short_12","alias_value":"UWVJ7PNJCGM6","created_at":"2026-07-04T15:32:30Z"},{"alias_kind":"pith_short_16","alias_value":"UWVJ7PNJCGM6GNMQ","created_at":"2026-07-04T15:32:30Z"},{"alias_kind":"pith_short_8","alias_value":"UWVJ7PNJ","created_at":"2026-07-04T15:32:30Z"}],"graph_snapshots":[{"event_id":"sha256:713748460535ac73c2694cd258485fec0db6e1df65d74c53d77f9f0c8f83b9ae","target":"graph","created_at":"2026-07-04T15:32:30Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":4,"items":[{"attestation":"unclaimed","claim_id":"C1","kind":"strongest_claim","source":"verdict.strongest_claim","status":"machine_extracted","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."},{"attestation":"unclaimed","claim_id":"C2","kind":"weakest_assumption","source":"verdict.weakest_assumption","status":"machine_extracted","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."},{"attestation":"unclaimed","claim_id":"C3","kind":"one_line_summary","source":"verdict.one_line_summary","status":"machine_extracted","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."},{"attestation":"unclaimed","claim_id":"C4","kind":"headline","source":"verdict.pith_extraction.headline","status":"machine_extracted","text":"Gauge theory correlators are extracted from how the supergravity action in anti-de Sitter space depends on boundary conditions."}],"snapshot_sha256":"023d7f8f2532f904392c1d3540ef56767b0b093082a78bcbb3e3257da531be35"},"formal_canon":{"evidence_count":2,"snapshot_sha256":"2f90907784d8224d5fbf5c6094546852ea519269ae6c93fcc4afc915a72a7de0"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/hep-th/9802109/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"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","authors_text":"A.M. Polyakov, I.R. Klebanov, S.S. Gubser","cross_cats":[],"headline":"Gauge theory correlators are extracted from how the supergravity action in anti-de Sitter space depends on boundary conditions.","license":"","primary_cat":"hep-th","submitted_at":"1998-02-16T18:38:17Z","title":"Gauge Theory Correlators from Non-Critical String Theory"},"references":{"count":24,"internal_anchors":1,"resolved_work":24,"sample":[{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":1,"title":"Gauge Fields as Rings of Glue","work_id":"36fb3c61-73de-4996-94cf-c0a587c720a4","year":1980},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":2,"title":"Exact Equation for the Lo op Average in Mul- ticolor QCD","work_id":"52cd698d-fbc8-450c-9d4d-fd080c69ca9d","year":1979},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":3,"title":"A planar diagram theory for strong interact ions","work_id":"6c48e883-60be-4e03-bb9a-987632e969c3","year":1974},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":4,"title":"String theory and quark confinement","work_id":"95ba559d-7161-4665-9f1b-312b3198df77","year":null},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":5,"title":"Effective Field Theory f rom Quantized Strings","work_id":"4f593ae0-3884-4a69-8865-da37849a14bd","year":1985}],"snapshot_sha256":"b775a95cb8bfe1859c644126dfb4fe43b1ab98e5d52c53ae7ca5c92826a93104"},"source":{"id":"hep-th/9802109","kind":"arxiv","version":2},"verdict":{"created_at":"2026-05-11T15:52:09.773353Z","id":"29c02aad-61fa-4efe-880c-5010fde9672f","model_set":{"reader":"grok-4.3"},"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","pith_extraction_headline":"Gauge theory correlators are extracted from how the supergravity action in anti-de Sitter space depends on boundary conditions.","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.","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."}},"verdict_id":"29c02aad-61fa-4efe-880c-5010fde9672f"}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:1af42edbaa2b5554d25a17149ca9b7434df50af82bfbcbac75b8061d0d7e7df0","target":"record","created_at":"2026-07-04T15:32:30Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"4947f9c07120e929af77897c5b83ad7b8cdb020cc31e9fea0ad35b657cfd4c66","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"1998-02-16T18:38:17Z","title_canon_sha256":"1f34a30ef8be57566694324e0fce2395c601bbe66a54fa6813eaf2eff1008cd5"},"schema_version":"1.0","source":{"id":"hep-th/9802109","kind":"arxiv","version":2}},"canonical_sha256":"a5aa9fbda91199e33590cb71b0317a500457d23a3f1710f4126f787bca7c6e01","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a5aa9fbda91199e33590cb71b0317a500457d23a3f1710f4126f787bca7c6e01","first_computed_at":"2026-07-04T15:32:30.270721Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T15:32:30.270721Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"e2T7xswbDuyXyTLaNZIeYcs42YF81Bgz9fSJ7L0YG0ASu9+OuXWFtpEraCLgntAq9V0/GUU++oQP3PXrTc/BDw==","signature_status":"signed_v1","signed_at":"2026-07-04T15:32:30.271142Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-th/9802109","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1af42edbaa2b5554d25a17149ca9b7434df50af82bfbcbac75b8061d0d7e7df0","sha256:713748460535ac73c2694cd258485fec0db6e1df65d74c53d77f9f0c8f83b9ae"],"state_sha256":"1104958e04565b17ca56610401aca3cbe524fae0fed58bbfbb32f53e86affb0b"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"5zQutFKgxID2WUuZhfwaCEeHo43rfZAWPTyze6J6Tss3B1UNF/xMTiKmSPRaL/e14D5qgnSC5qivA881ycdyCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-14T03:23:34.998263Z","bundle_sha256":"74bd985bd0b16934efea9038df9dfb4ce3a873ce7a1bed2afbadcff38cda1c3d"}}