{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:DZHGBWVVGQFN2PT2GGFQNPSXWT","short_pith_number":"pith:DZHGBWVV","schema_version":"1.0","canonical_sha256":"1e4e60dab5340add3e7a318b06be57b4c6973b0ffde8774d8acd89c6a22e3754","source":{"kind":"arxiv","id":"1803.01379","version":4},"attestation_state":"computed","paper":{"title":"AdS$_4$/CFT$_3$ for Unprotected Operators","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Shai M. Chester","submitted_at":"2018-03-04T16:50:53Z","abstract_excerpt":"We consider the four-point function of the lowest scalar in the stress-energy tensor multiplet in $\\mathcal{N}=8$ ABJ(M) theory \\cite{Aharony:2008ug, Aharony:2008gk}. At large central charge $c_T\\sim N^{3/2}$, this correlator is given by the corresponding holographic correlation function in 11d supergravity on $AdS_4\\times S^7$. We use Mellin space techniques to compute the leading $1/c_T$ correction to anomalous dimensions and OPE coefficients of operators that appear in this holographic correlator. For half and quarter-BPS operators, we find exact agreement with previously computed localizat"},"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":"1803.01379","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-03-04T16:50:53Z","cross_cats_sorted":[],"title_canon_sha256":"ae687afba904f5dcc1661a26fa5cc18851b9ad3b5ce1f7eea644c638dfbe844c","abstract_canon_sha256":"92379ae699846b60ee062f04187386483dcb945aef9b0d5f4a5690531bd6bc8d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:43:18.185778Z","signature_b64":"YkD0QGgr21gkevoxScMnGcyFqk+qcMj37za3Q1OAMdwhE8pKeGLrPCgCiSXULr9zjBL7Ib1guV8xCCdvJSaTBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1e4e60dab5340add3e7a318b06be57b4c6973b0ffde8774d8acd89c6a22e3754","last_reissued_at":"2026-05-17T23:43:18.185024Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:43:18.185024Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"AdS$_4$/CFT$_3$ for Unprotected Operators","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Shai M. Chester","submitted_at":"2018-03-04T16:50:53Z","abstract_excerpt":"We consider the four-point function of the lowest scalar in the stress-energy tensor multiplet in $\\mathcal{N}=8$ ABJ(M) theory \\cite{Aharony:2008ug, Aharony:2008gk}. At large central charge $c_T\\sim N^{3/2}$, this correlator is given by the corresponding holographic correlation function in 11d supergravity on $AdS_4\\times S^7$. We use Mellin space techniques to compute the leading $1/c_T$ correction to anomalous dimensions and OPE coefficients of operators that appear in this holographic correlator. For half and quarter-BPS operators, we find exact agreement with previously computed localizat"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1803.01379","kind":"arxiv","version":4},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"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":"1803.01379","created_at":"2026-05-17T23:43:18.185136+00:00"},{"alias_kind":"arxiv_version","alias_value":"1803.01379v4","created_at":"2026-05-17T23:43:18.185136+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1803.01379","created_at":"2026-05-17T23:43:18.185136+00:00"},{"alias_kind":"pith_short_12","alias_value":"DZHGBWVVGQFN","created_at":"2026-05-18T12:32:19.392346+00:00"},{"alias_kind":"pith_short_16","alias_value":"DZHGBWVVGQFN2PT2","created_at":"2026-05-18T12:32:19.392346+00:00"},{"alias_kind":"pith_short_8","alias_value":"DZHGBWVV","created_at":"2026-05-18T12:32:19.392346+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2412.08689","citing_title":"The type IIA Virasoro-Shapiro amplitude in AdS$_4$ $\\times$ CP$^3$ from ABJM theory","ref_index":51,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/DZHGBWVVGQFN2PT2GGFQNPSXWT","json":"https://pith.science/pith/DZHGBWVVGQFN2PT2GGFQNPSXWT.json","graph_json":"https://pith.science/api/pith-number/DZHGBWVVGQFN2PT2GGFQNPSXWT/graph.json","events_json":"https://pith.science/api/pith-number/DZHGBWVVGQFN2PT2GGFQNPSXWT/events.json","paper":"https://pith.science/paper/DZHGBWVV"},"agent_actions":{"view_html":"https://pith.science/pith/DZHGBWVVGQFN2PT2GGFQNPSXWT","download_json":"https://pith.science/pith/DZHGBWVVGQFN2PT2GGFQNPSXWT.json","view_paper":"https://pith.science/paper/DZHGBWVV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1803.01379&json=true","fetch_graph":"https://pith.science/api/pith-number/DZHGBWVVGQFN2PT2GGFQNPSXWT/graph.json","fetch_events":"https://pith.science/api/pith-number/DZHGBWVVGQFN2PT2GGFQNPSXWT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DZHGBWVVGQFN2PT2GGFQNPSXWT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DZHGBWVVGQFN2PT2GGFQNPSXWT/action/storage_attestation","attest_author":"https://pith.science/pith/DZHGBWVVGQFN2PT2GGFQNPSXWT/action/author_attestation","sign_citation":"https://pith.science/pith/DZHGBWVVGQFN2PT2GGFQNPSXWT/action/citation_signature","submit_replication":"https://pith.science/pith/DZHGBWVVGQFN2PT2GGFQNPSXWT/action/replication_record"}},"created_at":"2026-05-17T23:43:18.185136+00:00","updated_at":"2026-05-17T23:43:18.185136+00:00"}