{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:L5JWWHQF5KSPOC6N5TY3F6BPCN","short_pith_number":"pith:L5JWWHQF","schema_version":"1.0","canonical_sha256":"5f536b1e05eaa4f70bcdecf1b2f82f1360c85d69de0cbf07fa27c652c0b637cd","source":{"kind":"arxiv","id":"1409.3187","version":3},"attestation_state":"computed","paper":{"title":"One-loop Structure of Higher Rank Wilson Loops in AdS/CFT","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Alberto Faraggi, Guojun Zhang, James T. Liu, Leopoldo A. Pando Zayas","submitted_at":"2014-09-10T18:42:30Z","abstract_excerpt":"The half-supersymmetric Wilson loop in $\\mathcal N=4$ SYM is arguably the central non-local operator in the AdS/CFT correspondence. On the field theory side, the vacuum expectation values of Wilson loops in arbitrary representations of $SU(N)$ are captured to all orders in perturbation theory by a Gaussian matrix model. Of prominent interest are the $k$-symmetric and $k$-antisymmetric representations, whose gravitational description is given in terms of D3- and D5-branes, respectively, with fluxes in their world volumes. At leading order in $N$ and $\\lambda$ the agreement in both cases is exac"},"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":"1409.3187","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-09-10T18:42:30Z","cross_cats_sorted":[],"title_canon_sha256":"d80eede7718e0834b7965d28d081945949f9fc0b4ff4a92b23b2a199f06d17f4","abstract_canon_sha256":"9476cf6792498cb875b39499617c4bb838695d9cef83ee7c8382fc3d838d22d1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:21:37.929702Z","signature_b64":"aG6jZENBSQw08a/ziMBiDM3f3DqU9JXShKwm1hJjQa2e8sGcfiAqdxzBlzX+5Da5HqOvbZQhMv6/Tzz7ONpaDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5f536b1e05eaa4f70bcdecf1b2f82f1360c85d69de0cbf07fa27c652c0b637cd","last_reissued_at":"2026-05-18T01:21:37.929043Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:21:37.929043Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"One-loop Structure of Higher Rank Wilson Loops in AdS/CFT","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Alberto Faraggi, Guojun Zhang, James T. Liu, Leopoldo A. Pando Zayas","submitted_at":"2014-09-10T18:42:30Z","abstract_excerpt":"The half-supersymmetric Wilson loop in $\\mathcal N=4$ SYM is arguably the central non-local operator in the AdS/CFT correspondence. On the field theory side, the vacuum expectation values of Wilson loops in arbitrary representations of $SU(N)$ are captured to all orders in perturbation theory by a Gaussian matrix model. Of prominent interest are the $k$-symmetric and $k$-antisymmetric representations, whose gravitational description is given in terms of D3- and D5-branes, respectively, with fluxes in their world volumes. At leading order in $N$ and $\\lambda$ the agreement in both cases is exac"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1409.3187","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":"1409.3187","created_at":"2026-05-18T01:21:37.929139+00:00"},{"alias_kind":"arxiv_version","alias_value":"1409.3187v3","created_at":"2026-05-18T01:21:37.929139+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1409.3187","created_at":"2026-05-18T01:21:37.929139+00:00"},{"alias_kind":"pith_short_12","alias_value":"L5JWWHQF5KSP","created_at":"2026-05-18T12:28:35.611951+00:00"},{"alias_kind":"pith_short_16","alias_value":"L5JWWHQF5KSPOC6N","created_at":"2026-05-18T12:28:35.611951+00:00"},{"alias_kind":"pith_short_8","alias_value":"L5JWWHQF","created_at":"2026-05-18T12:28:35.611951+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/L5JWWHQF5KSPOC6N5TY3F6BPCN","json":"https://pith.science/pith/L5JWWHQF5KSPOC6N5TY3F6BPCN.json","graph_json":"https://pith.science/api/pith-number/L5JWWHQF5KSPOC6N5TY3F6BPCN/graph.json","events_json":"https://pith.science/api/pith-number/L5JWWHQF5KSPOC6N5TY3F6BPCN/events.json","paper":"https://pith.science/paper/L5JWWHQF"},"agent_actions":{"view_html":"https://pith.science/pith/L5JWWHQF5KSPOC6N5TY3F6BPCN","download_json":"https://pith.science/pith/L5JWWHQF5KSPOC6N5TY3F6BPCN.json","view_paper":"https://pith.science/paper/L5JWWHQF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1409.3187&json=true","fetch_graph":"https://pith.science/api/pith-number/L5JWWHQF5KSPOC6N5TY3F6BPCN/graph.json","fetch_events":"https://pith.science/api/pith-number/L5JWWHQF5KSPOC6N5TY3F6BPCN/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/L5JWWHQF5KSPOC6N5TY3F6BPCN/action/timestamp_anchor","attest_storage":"https://pith.science/pith/L5JWWHQF5KSPOC6N5TY3F6BPCN/action/storage_attestation","attest_author":"https://pith.science/pith/L5JWWHQF5KSPOC6N5TY3F6BPCN/action/author_attestation","sign_citation":"https://pith.science/pith/L5JWWHQF5KSPOC6N5TY3F6BPCN/action/citation_signature","submit_replication":"https://pith.science/pith/L5JWWHQF5KSPOC6N5TY3F6BPCN/action/replication_record"}},"created_at":"2026-05-18T01:21:37.929139+00:00","updated_at":"2026-05-18T01:21:37.929139+00:00"}