{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:X26EXM6A4APD2YPBGQXPZAAU5W","short_pith_number":"pith:X26EXM6A","schema_version":"1.0","canonical_sha256":"bebc4bb3c0e01e3d61e1342efc8014ed87ad3f5d8aaa572f1f1943dbe431c18e","source":{"kind":"arxiv","id":"2110.13166","version":1},"attestation_state":"computed","paper":{"title":"The Four-Loop $\\mathcal{N}=4$ SYM Sudakov Form Factor","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Alexander V. Smirnov, Andreas von Manteuffel, Matthias Steinhauser, Robert M. Schabinger, Roman N. Lee, Vladimir A. Smirnov","submitted_at":"2021-10-25T18:00:03Z","abstract_excerpt":"We present the Sudakov form factor in full color $\\mathcal{N}=4$ supersymmetric Yang-Mills theory to four loop order and provide uniformly transcendental results for the relevant master integrals through to weight eight."},"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":"2110.13166","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2021-10-25T18:00:03Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"06af3a2d70292442d026001739511f49faf415b410652031f845ed2c593ec35f","abstract_canon_sha256":"214b9f893c038f16de4d02a9423533ef2bd28d36881b16ce5ab7b720b7888c61"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:55:04.201220Z","signature_b64":"ifqemYRr7jN7eVldPMSjuO4W0/Ty8x7zXLYxnIcLeJ9NlQVRcxPPQCoHcqPP4dnRDz3+Dy+fPJMQD+1MrEjtCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bebc4bb3c0e01e3d61e1342efc8014ed87ad3f5d8aaa572f1f1943dbe431c18e","last_reissued_at":"2026-07-05T03:55:04.200776Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:55:04.200776Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Four-Loop $\\mathcal{N}=4$ SYM Sudakov Form Factor","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Alexander V. Smirnov, Andreas von Manteuffel, Matthias Steinhauser, Robert M. Schabinger, Roman N. Lee, Vladimir A. Smirnov","submitted_at":"2021-10-25T18:00:03Z","abstract_excerpt":"We present the Sudakov form factor in full color $\\mathcal{N}=4$ supersymmetric Yang-Mills theory to four loop order and provide uniformly transcendental results for the relevant master integrals through to weight eight."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2110.13166","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2110.13166/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":"2110.13166","created_at":"2026-07-05T03:55:04.200839+00:00"},{"alias_kind":"arxiv_version","alias_value":"2110.13166v1","created_at":"2026-07-05T03:55:04.200839+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2110.13166","created_at":"2026-07-05T03:55:04.200839+00:00"},{"alias_kind":"pith_short_12","alias_value":"X26EXM6A4APD","created_at":"2026-07-05T03:55:04.200839+00:00"},{"alias_kind":"pith_short_16","alias_value":"X26EXM6A4APD2YPB","created_at":"2026-07-05T03:55:04.200839+00:00"},{"alias_kind":"pith_short_8","alias_value":"X26EXM6A","created_at":"2026-07-05T03:55:04.200839+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.18362","citing_title":"Tracing Transcendentality in Protected Correlators of N=4 SYM","ref_index":25,"is_internal_anchor":false},{"citing_arxiv_id":"2604.02859","citing_title":"The Fate of Ultra-Collinear Modes in On-Shell Massive Sudakov Form Factors","ref_index":31,"is_internal_anchor":false},{"citing_arxiv_id":"2604.21015","citing_title":"Form factors of $\\mathscr{N}=4$ self-dual Yang-Mills from the chiral algebra bootstrap","ref_index":49,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/X26EXM6A4APD2YPBGQXPZAAU5W","json":"https://pith.science/pith/X26EXM6A4APD2YPBGQXPZAAU5W.json","graph_json":"https://pith.science/api/pith-number/X26EXM6A4APD2YPBGQXPZAAU5W/graph.json","events_json":"https://pith.science/api/pith-number/X26EXM6A4APD2YPBGQXPZAAU5W/events.json","paper":"https://pith.science/paper/X26EXM6A"},"agent_actions":{"view_html":"https://pith.science/pith/X26EXM6A4APD2YPBGQXPZAAU5W","download_json":"https://pith.science/pith/X26EXM6A4APD2YPBGQXPZAAU5W.json","view_paper":"https://pith.science/paper/X26EXM6A","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2110.13166&json=true","fetch_graph":"https://pith.science/api/pith-number/X26EXM6A4APD2YPBGQXPZAAU5W/graph.json","fetch_events":"https://pith.science/api/pith-number/X26EXM6A4APD2YPBGQXPZAAU5W/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/X26EXM6A4APD2YPBGQXPZAAU5W/action/timestamp_anchor","attest_storage":"https://pith.science/pith/X26EXM6A4APD2YPBGQXPZAAU5W/action/storage_attestation","attest_author":"https://pith.science/pith/X26EXM6A4APD2YPBGQXPZAAU5W/action/author_attestation","sign_citation":"https://pith.science/pith/X26EXM6A4APD2YPBGQXPZAAU5W/action/citation_signature","submit_replication":"https://pith.science/pith/X26EXM6A4APD2YPBGQXPZAAU5W/action/replication_record"}},"created_at":"2026-07-05T03:55:04.200839+00:00","updated_at":"2026-07-05T03:55:04.200839+00:00"}