{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:5UEITHKTLNJRQE6LACMSLE7M5M","short_pith_number":"pith:5UEITHKT","schema_version":"1.0","canonical_sha256":"ed08899d535b531813cb00992593eceb1a18dbfbbce2e630858a9c69665efedd","source":{"kind":"arxiv","id":"2110.13106","version":5},"attestation_state":"computed","paper":{"title":"Modular invariant holographic correlators for $\\mathcal{N}=4$ SYM with general gauge group","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Luis F. Alday, Shai M. Chester, Tobias Hansen","submitted_at":"2021-10-25T16:58:05Z","abstract_excerpt":"We study the stress tensor four-point function for $\\mathcal{N}=4$ SYM with gauge group $G=SU(N)$, $SO(2N+1)$, $SO(2N)$ or $USp(2N)$ at large $N$. When $G=SU(N)$, the theory is dual to type IIB string theory on $AdS_5\\times S^5$ with complexified string coupling $\\tau_s$, while for the other cases it is dual to the orbifold theory on $AdS_5\\times S^5/\\mathbb{Z}_2$. In all cases we use the analytic bootstrap and constraints from localization to compute 1-loop and higher derivative tree level corrections to the leading supergravity approximation of the correlator. We give perturbative evidence t"},"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":"2110.13106","kind":"arxiv","version":5},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2021-10-25T16:58:05Z","cross_cats_sorted":[],"title_canon_sha256":"a3152cd932b647e210e825b609d4fc253728f321f18186bab51fb2e4ff3a5ca6","abstract_canon_sha256":"cd6a2c7ada212564416f8c8b2afd6ca2f3f9bf397516c2a525bc9de955d494c4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:43:59.567286Z","signature_b64":"KUK3FiTBcyoi5zDUvdcnoi2ISJVzkVW9EkP+EHklQtBTATK/YbUZ0jrXANoUE/U43k2EWdji4wFcI9aXhg9rCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ed08899d535b531813cb00992593eceb1a18dbfbbce2e630858a9c69665efedd","last_reissued_at":"2026-07-05T03:43:59.566777Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:43:59.566777Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Modular invariant holographic correlators for $\\mathcal{N}=4$ SYM with general gauge group","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Luis F. Alday, Shai M. Chester, Tobias Hansen","submitted_at":"2021-10-25T16:58:05Z","abstract_excerpt":"We study the stress tensor four-point function for $\\mathcal{N}=4$ SYM with gauge group $G=SU(N)$, $SO(2N+1)$, $SO(2N)$ or $USp(2N)$ at large $N$. When $G=SU(N)$, the theory is dual to type IIB string theory on $AdS_5\\times S^5$ with complexified string coupling $\\tau_s$, while for the other cases it is dual to the orbifold theory on $AdS_5\\times S^5/\\mathbb{Z}_2$. In all cases we use the analytic bootstrap and constraints from localization to compute 1-loop and higher derivative tree level corrections to the leading supergravity approximation of the correlator. We give perturbative evidence t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2110.13106","kind":"arxiv","version":5},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2110.13106/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2110.13106","created_at":"2026-07-05T03:43:59.566823+00:00"},{"alias_kind":"arxiv_version","alias_value":"2110.13106v5","created_at":"2026-07-05T03:43:59.566823+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2110.13106","created_at":"2026-07-05T03:43:59.566823+00:00"},{"alias_kind":"pith_short_12","alias_value":"5UEITHKTLNJR","created_at":"2026-07-05T03:43:59.566823+00:00"},{"alias_kind":"pith_short_16","alias_value":"5UEITHKTLNJRQE6L","created_at":"2026-07-05T03:43:59.566823+00:00"},{"alias_kind":"pith_short_8","alias_value":"5UEITHKT","created_at":"2026-07-05T03:43:59.566823+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2507.12533","citing_title":"$20'$ Five-Point Function of $\\mathcal{N}=4$ SYM and Stringy Corrections","ref_index":36,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/5UEITHKTLNJRQE6LACMSLE7M5M","json":"https://pith.science/pith/5UEITHKTLNJRQE6LACMSLE7M5M.json","graph_json":"https://pith.science/api/pith-number/5UEITHKTLNJRQE6LACMSLE7M5M/graph.json","events_json":"https://pith.science/api/pith-number/5UEITHKTLNJRQE6LACMSLE7M5M/events.json","paper":"https://pith.science/paper/5UEITHKT"},"agent_actions":{"view_html":"https://pith.science/pith/5UEITHKTLNJRQE6LACMSLE7M5M","download_json":"https://pith.science/pith/5UEITHKTLNJRQE6LACMSLE7M5M.json","view_paper":"https://pith.science/paper/5UEITHKT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2110.13106&json=true","fetch_graph":"https://pith.science/api/pith-number/5UEITHKTLNJRQE6LACMSLE7M5M/graph.json","fetch_events":"https://pith.science/api/pith-number/5UEITHKTLNJRQE6LACMSLE7M5M/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5UEITHKTLNJRQE6LACMSLE7M5M/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5UEITHKTLNJRQE6LACMSLE7M5M/action/storage_attestation","attest_author":"https://pith.science/pith/5UEITHKTLNJRQE6LACMSLE7M5M/action/author_attestation","sign_citation":"https://pith.science/pith/5UEITHKTLNJRQE6LACMSLE7M5M/action/citation_signature","submit_replication":"https://pith.science/pith/5UEITHKTLNJRQE6LACMSLE7M5M/action/replication_record"}},"created_at":"2026-07-05T03:43:59.566823+00:00","updated_at":"2026-07-05T03:43:59.566823+00:00"}