{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:VCZHIWZ7LHY2VOZUHK2RWYAQ4D","short_pith_number":"pith:VCZHIWZ7","schema_version":"1.0","canonical_sha256":"a8b2745b3f59f1aabb343ab51b6010e0ef06bfc29dd18521254adf991aeb1b7a","source":{"kind":"arxiv","id":"1802.04237","version":3},"attestation_state":"computed","paper":{"title":"Quantum Spectral Curve and Structure Constants in N=4 SYM: Cusps in the Ladder Limit","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"Andrea Cavagli\\`a, Fedor Levkovich-Maslyuk, Nikolay Gromov","submitted_at":"2018-02-12T18:38:45Z","abstract_excerpt":"We find a massive simplification in the non-perturbative expression for the structure constant of Wilson lines with 3 cusps when expressed in terms of the key Quantum Spectral Curve quantities, namely Q-functions. Our calculation is done for the configuration of 3 cusps lying in the same plane with arbitrary angles in the ladders limit. This provides strong evidence that the Quantum Spectral Curve is not only a highly efficient tool for finding the anomalous dimensions but also encodes correlation functions with all wrapping corrections taken into account to all orders in the `t Hooft coupling"},"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":"1802.04237","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-02-12T18:38:45Z","cross_cats_sorted":["math-ph","math.MP"],"title_canon_sha256":"9966d8e35a534a59386fdd9cf5dec5689db43d3af09d9fa63e4e301f9475ed20","abstract_canon_sha256":"63a296b8adf33725e12fa7a75af66280ec3fe740b1b709b25b5ad9418bb70738"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:00:57.427864Z","signature_b64":"c/yp9hbCxubBFiWutmIkcQW/bX1P96cb+PpoG/DoEFE/5lDkpXo1LqzH+6p0KxEOgJ6v0KkxOdm0TJYvLBFYCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a8b2745b3f59f1aabb343ab51b6010e0ef06bfc29dd18521254adf991aeb1b7a","last_reissued_at":"2026-05-18T00:00:57.427274Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:00:57.427274Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quantum Spectral Curve and Structure Constants in N=4 SYM: Cusps in the Ladder Limit","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"Andrea Cavagli\\`a, Fedor Levkovich-Maslyuk, Nikolay Gromov","submitted_at":"2018-02-12T18:38:45Z","abstract_excerpt":"We find a massive simplification in the non-perturbative expression for the structure constant of Wilson lines with 3 cusps when expressed in terms of the key Quantum Spectral Curve quantities, namely Q-functions. Our calculation is done for the configuration of 3 cusps lying in the same plane with arbitrary angles in the ladders limit. This provides strong evidence that the Quantum Spectral Curve is not only a highly efficient tool for finding the anomalous dimensions but also encodes correlation functions with all wrapping corrections taken into account to all orders in the `t Hooft coupling"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1802.04237","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":"1802.04237","created_at":"2026-05-18T00:00:57.427380+00:00"},{"alias_kind":"arxiv_version","alias_value":"1802.04237v3","created_at":"2026-05-18T00:00:57.427380+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1802.04237","created_at":"2026-05-18T00:00:57.427380+00:00"},{"alias_kind":"pith_short_12","alias_value":"VCZHIWZ7LHY2","created_at":"2026-05-18T12:32:59.047623+00:00"},{"alias_kind":"pith_short_16","alias_value":"VCZHIWZ7LHY2VOZU","created_at":"2026-05-18T12:32:59.047623+00:00"},{"alias_kind":"pith_short_8","alias_value":"VCZHIWZ7","created_at":"2026-05-18T12:32:59.047623+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.15422","citing_title":"Semiclassics at the cusp","ref_index":39,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/VCZHIWZ7LHY2VOZUHK2RWYAQ4D","json":"https://pith.science/pith/VCZHIWZ7LHY2VOZUHK2RWYAQ4D.json","graph_json":"https://pith.science/api/pith-number/VCZHIWZ7LHY2VOZUHK2RWYAQ4D/graph.json","events_json":"https://pith.science/api/pith-number/VCZHIWZ7LHY2VOZUHK2RWYAQ4D/events.json","paper":"https://pith.science/paper/VCZHIWZ7"},"agent_actions":{"view_html":"https://pith.science/pith/VCZHIWZ7LHY2VOZUHK2RWYAQ4D","download_json":"https://pith.science/pith/VCZHIWZ7LHY2VOZUHK2RWYAQ4D.json","view_paper":"https://pith.science/paper/VCZHIWZ7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1802.04237&json=true","fetch_graph":"https://pith.science/api/pith-number/VCZHIWZ7LHY2VOZUHK2RWYAQ4D/graph.json","fetch_events":"https://pith.science/api/pith-number/VCZHIWZ7LHY2VOZUHK2RWYAQ4D/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VCZHIWZ7LHY2VOZUHK2RWYAQ4D/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VCZHIWZ7LHY2VOZUHK2RWYAQ4D/action/storage_attestation","attest_author":"https://pith.science/pith/VCZHIWZ7LHY2VOZUHK2RWYAQ4D/action/author_attestation","sign_citation":"https://pith.science/pith/VCZHIWZ7LHY2VOZUHK2RWYAQ4D/action/citation_signature","submit_replication":"https://pith.science/pith/VCZHIWZ7LHY2VOZUHK2RWYAQ4D/action/replication_record"}},"created_at":"2026-05-18T00:00:57.427380+00:00","updated_at":"2026-05-18T00:00:57.427380+00:00"}