{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:K5AFR5O7GPTYWHG5FY5DYBGPJ5","short_pith_number":"pith:K5AFR5O7","schema_version":"1.0","canonical_sha256":"574058f5df33e78b1cdd2e3a3c04cf4f53a8d6ac7f6412da49811b95bb8f8d9c","source":{"kind":"arxiv","id":"1201.6073","version":1},"attestation_state":"computed","paper":{"title":"Conformal anomaly of super Wilson loop","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A. V. Belitsky","submitted_at":"2012-01-29T20:01:25Z","abstract_excerpt":"Classically supersymmetric Wilson loop on a null polygonal contour possesses all symmetries required to match it onto non-MHV amplitudes in maximally supersymmetric Yang-Mills theory. However, to define it quantum mechanically, one is forced to regularize it since perturbative loop diagrams are not well-defined due to presence of ultraviolet divergences stemming from integration in the vicinity of the cusps. A regularization that is adopted by practitioners by allowing one to use spinor helicity formalism, on the one hand, and systematically go to higher orders of perturbation theory is based "},"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":"1201.6073","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-01-29T20:01:25Z","cross_cats_sorted":[],"title_canon_sha256":"3ceb85b1d715e57fa73698e62ad96abf6f8988abab76b5cbc839f1dc5c26a008","abstract_canon_sha256":"0c11ea1908befc915e6ee116dd6078db90f280fbb7ac429ee921efbecf982eb9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:58:38.455871Z","signature_b64":"eI8oF2OnZHZScIiVY9d2T6f0Z1dU23+vuXushILsAdq4RDBOwDCJWKNRPeUk339CEzeOGJLLYnezHYdOlhzLAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"574058f5df33e78b1cdd2e3a3c04cf4f53a8d6ac7f6412da49811b95bb8f8d9c","last_reissued_at":"2026-05-18T01:58:38.455093Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:58:38.455093Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Conformal anomaly of super Wilson loop","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A. V. Belitsky","submitted_at":"2012-01-29T20:01:25Z","abstract_excerpt":"Classically supersymmetric Wilson loop on a null polygonal contour possesses all symmetries required to match it onto non-MHV amplitudes in maximally supersymmetric Yang-Mills theory. However, to define it quantum mechanically, one is forced to regularize it since perturbative loop diagrams are not well-defined due to presence of ultraviolet divergences stemming from integration in the vicinity of the cusps. A regularization that is adopted by practitioners by allowing one to use spinor helicity formalism, on the one hand, and systematically go to higher orders of perturbation theory is based "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1201.6073","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":""},"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":"1201.6073","created_at":"2026-05-18T01:58:38.455219+00:00"},{"alias_kind":"arxiv_version","alias_value":"1201.6073v1","created_at":"2026-05-18T01:58:38.455219+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1201.6073","created_at":"2026-05-18T01:58:38.455219+00:00"},{"alias_kind":"pith_short_12","alias_value":"K5AFR5O7GPTY","created_at":"2026-05-18T12:27:11.947152+00:00"},{"alias_kind":"pith_short_16","alias_value":"K5AFR5O7GPTYWHG5","created_at":"2026-05-18T12:27:11.947152+00:00"},{"alias_kind":"pith_short_8","alias_value":"K5AFR5O7","created_at":"2026-05-18T12:27:11.947152+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/K5AFR5O7GPTYWHG5FY5DYBGPJ5","json":"https://pith.science/pith/K5AFR5O7GPTYWHG5FY5DYBGPJ5.json","graph_json":"https://pith.science/api/pith-number/K5AFR5O7GPTYWHG5FY5DYBGPJ5/graph.json","events_json":"https://pith.science/api/pith-number/K5AFR5O7GPTYWHG5FY5DYBGPJ5/events.json","paper":"https://pith.science/paper/K5AFR5O7"},"agent_actions":{"view_html":"https://pith.science/pith/K5AFR5O7GPTYWHG5FY5DYBGPJ5","download_json":"https://pith.science/pith/K5AFR5O7GPTYWHG5FY5DYBGPJ5.json","view_paper":"https://pith.science/paper/K5AFR5O7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1201.6073&json=true","fetch_graph":"https://pith.science/api/pith-number/K5AFR5O7GPTYWHG5FY5DYBGPJ5/graph.json","fetch_events":"https://pith.science/api/pith-number/K5AFR5O7GPTYWHG5FY5DYBGPJ5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/K5AFR5O7GPTYWHG5FY5DYBGPJ5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/K5AFR5O7GPTYWHG5FY5DYBGPJ5/action/storage_attestation","attest_author":"https://pith.science/pith/K5AFR5O7GPTYWHG5FY5DYBGPJ5/action/author_attestation","sign_citation":"https://pith.science/pith/K5AFR5O7GPTYWHG5FY5DYBGPJ5/action/citation_signature","submit_replication":"https://pith.science/pith/K5AFR5O7GPTYWHG5FY5DYBGPJ5/action/replication_record"}},"created_at":"2026-05-18T01:58:38.455219+00:00","updated_at":"2026-05-18T01:58:38.455219+00:00"}