{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:CL5L37NJFPIAFHXJORKIXVAVW6","short_pith_number":"pith:CL5L37NJ","schema_version":"1.0","canonical_sha256":"12fabdfda92bd0029ee974548bd415b790039155acb4eb4bbceb9b27f68e8030","source":{"kind":"arxiv","id":"1107.5702","version":1},"attestation_state":"computed","paper":{"title":"Correlation function of null polygonal Wilson loops with local operators","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A.A. Tseytlin, E.I. Buchbinder, L.F. Alday","submitted_at":"2011-07-28T12:54:01Z","abstract_excerpt":"We consider the correlator <W_n O(x)> of a light-like polygonal Wilson loop with n cusps with a local operator (like the dilaton or the chiral primary scalar) in planar N =4 super Yang-Mills theory. As a consequence of conformal symmetry, the main part of such correlator is a function F of 3n-11 conformal ratios. The first non-trivial case is n=4 when F depends on just one conformal ratio \\zeta. This makes the corresponding correlator one of the simplest non-trivial observables that one would like to compute for generic values of the `t Hooft coupling \\lambda. We compute F(\\zeta,\\lambda) at le"},"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":"1107.5702","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-07-28T12:54:01Z","cross_cats_sorted":[],"title_canon_sha256":"d259d72514a3d37ada64cfa2e8b0c611642d3e80ed3258879bbc41b84da0c697","abstract_canon_sha256":"c57da1d22f7167a34353c188059a62cbb3f95171f3d3f3e87f87728f49784577"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:01:08.390258Z","signature_b64":"OwWNHp613mJ9cfQ+Blev79z6ovz1ho3ggnlAg2wPeIn+GOEsVod/fXjNzOqTKhGtI1+kfpOGyc43QsUMtVRtDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"12fabdfda92bd0029ee974548bd415b790039155acb4eb4bbceb9b27f68e8030","last_reissued_at":"2026-05-18T02:01:08.389684Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:01:08.389684Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Correlation function of null polygonal Wilson loops with local operators","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A.A. Tseytlin, E.I. Buchbinder, L.F. Alday","submitted_at":"2011-07-28T12:54:01Z","abstract_excerpt":"We consider the correlator <W_n O(x)> of a light-like polygonal Wilson loop with n cusps with a local operator (like the dilaton or the chiral primary scalar) in planar N =4 super Yang-Mills theory. As a consequence of conformal symmetry, the main part of such correlator is a function F of 3n-11 conformal ratios. The first non-trivial case is n=4 when F depends on just one conformal ratio \\zeta. This makes the corresponding correlator one of the simplest non-trivial observables that one would like to compute for generic values of the `t Hooft coupling \\lambda. We compute F(\\zeta,\\lambda) at le"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1107.5702","kind":"arxiv","version":1},"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":"1107.5702","created_at":"2026-05-18T02:01:08.389786+00:00"},{"alias_kind":"arxiv_version","alias_value":"1107.5702v1","created_at":"2026-05-18T02:01:08.389786+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1107.5702","created_at":"2026-05-18T02:01:08.389786+00:00"},{"alias_kind":"pith_short_12","alias_value":"CL5L37NJFPIA","created_at":"2026-05-18T12:26:26.731475+00:00"},{"alias_kind":"pith_short_16","alias_value":"CL5L37NJFPIAFHXJ","created_at":"2026-05-18T12:26:26.731475+00:00"},{"alias_kind":"pith_short_8","alias_value":"CL5L37NJ","created_at":"2026-05-18T12:26:26.731475+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.22683","citing_title":"Landau Analysis of One-Cycle Negative Geometries","ref_index":58,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/CL5L37NJFPIAFHXJORKIXVAVW6","json":"https://pith.science/pith/CL5L37NJFPIAFHXJORKIXVAVW6.json","graph_json":"https://pith.science/api/pith-number/CL5L37NJFPIAFHXJORKIXVAVW6/graph.json","events_json":"https://pith.science/api/pith-number/CL5L37NJFPIAFHXJORKIXVAVW6/events.json","paper":"https://pith.science/paper/CL5L37NJ"},"agent_actions":{"view_html":"https://pith.science/pith/CL5L37NJFPIAFHXJORKIXVAVW6","download_json":"https://pith.science/pith/CL5L37NJFPIAFHXJORKIXVAVW6.json","view_paper":"https://pith.science/paper/CL5L37NJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1107.5702&json=true","fetch_graph":"https://pith.science/api/pith-number/CL5L37NJFPIAFHXJORKIXVAVW6/graph.json","fetch_events":"https://pith.science/api/pith-number/CL5L37NJFPIAFHXJORKIXVAVW6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CL5L37NJFPIAFHXJORKIXVAVW6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CL5L37NJFPIAFHXJORKIXVAVW6/action/storage_attestation","attest_author":"https://pith.science/pith/CL5L37NJFPIAFHXJORKIXVAVW6/action/author_attestation","sign_citation":"https://pith.science/pith/CL5L37NJFPIAFHXJORKIXVAVW6/action/citation_signature","submit_replication":"https://pith.science/pith/CL5L37NJFPIAFHXJORKIXVAVW6/action/replication_record"}},"created_at":"2026-05-18T02:01:08.389786+00:00","updated_at":"2026-05-18T02:01:08.389786+00:00"}