{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:OKY7FQ62DOSOQAA26MCVSZR75B","short_pith_number":"pith:OKY7FQ62","schema_version":"1.0","canonical_sha256":"72b1f2c3da1ba4e8001af30559663fe851729a945a2f4c65b1bcb80558ff440c","source":{"kind":"arxiv","id":"1610.02914","version":3},"attestation_state":"computed","paper":{"title":"Symmetric Wilson Loops beyond leading order","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Xinyi Chen-Lin","submitted_at":"2016-10-10T13:45:28Z","abstract_excerpt":"We study the circular Wilson loop in the symmetric representation of U(N) in $\\mathcal{N} = 4$ super-Yang-Mills (SYM). In the large N limit, we computed the exponentially-suppressed corrections for strong coupling, which suggests non-perturbative physics in the dual holographic theory. We also computed the next-to-leading order term in 1/N, and the result matches with the exact result from the k-fundamental representation."},"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":"1610.02914","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2016-10-10T13:45:28Z","cross_cats_sorted":[],"title_canon_sha256":"5bbaf92844ba1e167b25245dc6dc60d91b32986ee816976acb93c11d913cd00e","abstract_canon_sha256":"17f4755e6d066a0ea5bd4a3e7edaf1c17111241d7be48444f8789dfb631ad3b4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:53:07.230595Z","signature_b64":"w/oNZNgalJBy2p6aaP5UTENdxwq6CHyZPxV6XsnVVdFPWStsx9Ge8ET8zGg09n1q+Nv0uX71+KZABohYHsG6AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"72b1f2c3da1ba4e8001af30559663fe851729a945a2f4c65b1bcb80558ff440c","last_reissued_at":"2026-05-18T00:53:07.230159Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:53:07.230159Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Symmetric Wilson Loops beyond leading order","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Xinyi Chen-Lin","submitted_at":"2016-10-10T13:45:28Z","abstract_excerpt":"We study the circular Wilson loop in the symmetric representation of U(N) in $\\mathcal{N} = 4$ super-Yang-Mills (SYM). In the large N limit, we computed the exponentially-suppressed corrections for strong coupling, which suggests non-perturbative physics in the dual holographic theory. We also computed the next-to-leading order term in 1/N, and the result matches with the exact result from the k-fundamental representation."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1610.02914","kind":"arxiv","version":3},"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":"1610.02914","created_at":"2026-05-18T00:53:07.230234+00:00"},{"alias_kind":"arxiv_version","alias_value":"1610.02914v3","created_at":"2026-05-18T00:53:07.230234+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1610.02914","created_at":"2026-05-18T00:53:07.230234+00:00"},{"alias_kind":"pith_short_12","alias_value":"OKY7FQ62DOSO","created_at":"2026-05-18T12:30:36.002864+00:00"},{"alias_kind":"pith_short_16","alias_value":"OKY7FQ62DOSOQAA2","created_at":"2026-05-18T12:30:36.002864+00:00"},{"alias_kind":"pith_short_8","alias_value":"OKY7FQ62","created_at":"2026-05-18T12:30:36.002864+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2411.11626","citing_title":"Semiclassical quantization of M5 brane probes wrapped on $\\textrm{AdS}_3\\times S^3$ and defect anomalies","ref_index":74,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/OKY7FQ62DOSOQAA26MCVSZR75B","json":"https://pith.science/pith/OKY7FQ62DOSOQAA26MCVSZR75B.json","graph_json":"https://pith.science/api/pith-number/OKY7FQ62DOSOQAA26MCVSZR75B/graph.json","events_json":"https://pith.science/api/pith-number/OKY7FQ62DOSOQAA26MCVSZR75B/events.json","paper":"https://pith.science/paper/OKY7FQ62"},"agent_actions":{"view_html":"https://pith.science/pith/OKY7FQ62DOSOQAA26MCVSZR75B","download_json":"https://pith.science/pith/OKY7FQ62DOSOQAA26MCVSZR75B.json","view_paper":"https://pith.science/paper/OKY7FQ62","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1610.02914&json=true","fetch_graph":"https://pith.science/api/pith-number/OKY7FQ62DOSOQAA26MCVSZR75B/graph.json","fetch_events":"https://pith.science/api/pith-number/OKY7FQ62DOSOQAA26MCVSZR75B/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OKY7FQ62DOSOQAA26MCVSZR75B/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OKY7FQ62DOSOQAA26MCVSZR75B/action/storage_attestation","attest_author":"https://pith.science/pith/OKY7FQ62DOSOQAA26MCVSZR75B/action/author_attestation","sign_citation":"https://pith.science/pith/OKY7FQ62DOSOQAA26MCVSZR75B/action/citation_signature","submit_replication":"https://pith.science/pith/OKY7FQ62DOSOQAA26MCVSZR75B/action/replication_record"}},"created_at":"2026-05-18T00:53:07.230234+00:00","updated_at":"2026-05-18T00:53:07.230234+00:00"}