{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:UVRJ24MFA3W3ANW6W7ASNG7OBY","short_pith_number":"pith:UVRJ24MF","schema_version":"1.0","canonical_sha256":"a5629d718506edb036deb7c1269bee0e3464f54b3b5a1e6cda3c6d4b05b4aed1","source":{"kind":"arxiv","id":"1003.1702","version":2},"attestation_state":"computed","paper":{"title":"The Two-Loop Hexagon Wilson Loop in N = 4 SYM","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Claude Duhr, Vittorio Del Duca, Vladimir A. Smirnov","submitted_at":"2010-03-08T19:47:05Z","abstract_excerpt":"In the planar N=4 supersymmetric Yang-Mills theory, the conformal symmetry constrains multi-loop n-edged Wilson loops to be given in terms of the one-loop n-edged Wilson loop, augmented, for n greater than 6, by a function of conformally invariant cross ratios. That function is termed the remainder function. In a recent paper, we have displayed the first analytic computation of the two-loop six-edged Wilson loop, and thus of the corresponding remainder function. Although the calculation was performed in the quasi-multi-Regge kinematics of a pair along the ladder, the Regge exactness of the six"},"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":"1003.1702","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-03-08T19:47:05Z","cross_cats_sorted":[],"title_canon_sha256":"bba6c91dc1fd302723aca67c8af866dfe17a80ae8d0692545a818e4ad66754df","abstract_canon_sha256":"f2dd92c2e1d6368e76a635b4e1b2a47a24c3234cd6fab8953215bbd5aec2fd75"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:33:41.371440Z","signature_b64":"izSTeQx5i2qQdTalqJl+YMQTpaVAxhps9litlVpnGwF191JUaveI8VE+IMzseGBhH1yIrxAJhiXIgOjZL+y+BA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a5629d718506edb036deb7c1269bee0e3464f54b3b5a1e6cda3c6d4b05b4aed1","last_reissued_at":"2026-05-18T02:33:41.370979Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:33:41.370979Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Two-Loop Hexagon Wilson Loop in N = 4 SYM","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Claude Duhr, Vittorio Del Duca, Vladimir A. Smirnov","submitted_at":"2010-03-08T19:47:05Z","abstract_excerpt":"In the planar N=4 supersymmetric Yang-Mills theory, the conformal symmetry constrains multi-loop n-edged Wilson loops to be given in terms of the one-loop n-edged Wilson loop, augmented, for n greater than 6, by a function of conformally invariant cross ratios. That function is termed the remainder function. In a recent paper, we have displayed the first analytic computation of the two-loop six-edged Wilson loop, and thus of the corresponding remainder function. Although the calculation was performed in the quasi-multi-Regge kinematics of a pair along the ladder, the Regge exactness of the six"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1003.1702","kind":"arxiv","version":2},"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":"1003.1702","created_at":"2026-05-18T02:33:41.371041+00:00"},{"alias_kind":"arxiv_version","alias_value":"1003.1702v2","created_at":"2026-05-18T02:33:41.371041+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1003.1702","created_at":"2026-05-18T02:33:41.371041+00:00"},{"alias_kind":"pith_short_12","alias_value":"UVRJ24MFA3W3","created_at":"2026-05-18T12:26:15.391820+00:00"},{"alias_kind":"pith_short_16","alias_value":"UVRJ24MFA3W3ANW6","created_at":"2026-05-18T12:26:15.391820+00:00"},{"alias_kind":"pith_short_8","alias_value":"UVRJ24MF","created_at":"2026-05-18T12:26:15.391820+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/UVRJ24MFA3W3ANW6W7ASNG7OBY","json":"https://pith.science/pith/UVRJ24MFA3W3ANW6W7ASNG7OBY.json","graph_json":"https://pith.science/api/pith-number/UVRJ24MFA3W3ANW6W7ASNG7OBY/graph.json","events_json":"https://pith.science/api/pith-number/UVRJ24MFA3W3ANW6W7ASNG7OBY/events.json","paper":"https://pith.science/paper/UVRJ24MF"},"agent_actions":{"view_html":"https://pith.science/pith/UVRJ24MFA3W3ANW6W7ASNG7OBY","download_json":"https://pith.science/pith/UVRJ24MFA3W3ANW6W7ASNG7OBY.json","view_paper":"https://pith.science/paper/UVRJ24MF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1003.1702&json=true","fetch_graph":"https://pith.science/api/pith-number/UVRJ24MFA3W3ANW6W7ASNG7OBY/graph.json","fetch_events":"https://pith.science/api/pith-number/UVRJ24MFA3W3ANW6W7ASNG7OBY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UVRJ24MFA3W3ANW6W7ASNG7OBY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UVRJ24MFA3W3ANW6W7ASNG7OBY/action/storage_attestation","attest_author":"https://pith.science/pith/UVRJ24MFA3W3ANW6W7ASNG7OBY/action/author_attestation","sign_citation":"https://pith.science/pith/UVRJ24MFA3W3ANW6W7ASNG7OBY/action/citation_signature","submit_replication":"https://pith.science/pith/UVRJ24MFA3W3ANW6W7ASNG7OBY/action/replication_record"}},"created_at":"2026-05-18T02:33:41.371041+00:00","updated_at":"2026-05-18T02:33:41.371041+00:00"}