{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:IXJ2RUMLZ4ASLYAEOIFUOQ5EOX","short_pith_number":"pith:IXJ2RUML","schema_version":"1.0","canonical_sha256":"45d3a8d18bcf0125e004720b4743a475d59bc08655dc3be4980fadc49c3b87b9","source":{"kind":"arxiv","id":"1010.1498","version":1},"attestation_state":"computed","paper":{"title":"A Note on Dual MHV Diagrams in N=4 SYM","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Andreas Brandhuber, Bill Spence, Gabriele Travaglini, Gang Yang","submitted_at":"2010-10-07T18:00:44Z","abstract_excerpt":"Recently a reformulation of the MHV diagram method in N=4 supersymmetric Yang-Mills theory in momentum twistor space was presented and was shown to be equivalent to the perturbative expansion of the expectation value of a supersymmetric Wilson loop in momentum twistor space. In this note we present related explicit Feynman rules in dual momentum space, which should have the interpretation of Wilson loop diagrams in dual momentum space. We show that these novel rules are completely equivalent to ordinary spacetime MHV rules and can be naturally viewed as their graph dual representation."},"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":"1010.1498","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-10-07T18:00:44Z","cross_cats_sorted":[],"title_canon_sha256":"0d6e042a6e32ac6b1c1e9e5d41de2a2a3bc1bda35043df07b4d0b1ad50e46de2","abstract_canon_sha256":"32bc427bd76d7a959e622f31f0f9b14a8ffdfd80c924ab39591f2b73654e2803"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:25:49.198533Z","signature_b64":"mxDs4b5csL+430hHuZ2xNGA7FUsadZtpy2Dwb7yfXnTTg050twsg9XTc9y9qxENebXgckBEVNtaseSXTz9k1CA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"45d3a8d18bcf0125e004720b4743a475d59bc08655dc3be4980fadc49c3b87b9","last_reissued_at":"2026-05-18T04:25:49.197796Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:25:49.197796Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A Note on Dual MHV Diagrams in N=4 SYM","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Andreas Brandhuber, Bill Spence, Gabriele Travaglini, Gang Yang","submitted_at":"2010-10-07T18:00:44Z","abstract_excerpt":"Recently a reformulation of the MHV diagram method in N=4 supersymmetric Yang-Mills theory in momentum twistor space was presented and was shown to be equivalent to the perturbative expansion of the expectation value of a supersymmetric Wilson loop in momentum twistor space. In this note we present related explicit Feynman rules in dual momentum space, which should have the interpretation of Wilson loop diagrams in dual momentum space. We show that these novel rules are completely equivalent to ordinary spacetime MHV rules and can be naturally viewed as their graph dual representation."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1010.1498","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":"1010.1498","created_at":"2026-05-18T04:25:49.197911+00:00"},{"alias_kind":"arxiv_version","alias_value":"1010.1498v1","created_at":"2026-05-18T04:25:49.197911+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1010.1498","created_at":"2026-05-18T04:25:49.197911+00:00"},{"alias_kind":"pith_short_12","alias_value":"IXJ2RUMLZ4AS","created_at":"2026-05-18T12:26:09.077623+00:00"},{"alias_kind":"pith_short_16","alias_value":"IXJ2RUMLZ4ASLYAE","created_at":"2026-05-18T12:26:09.077623+00:00"},{"alias_kind":"pith_short_8","alias_value":"IXJ2RUML","created_at":"2026-05-18T12:26:09.077623+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/IXJ2RUMLZ4ASLYAEOIFUOQ5EOX","json":"https://pith.science/pith/IXJ2RUMLZ4ASLYAEOIFUOQ5EOX.json","graph_json":"https://pith.science/api/pith-number/IXJ2RUMLZ4ASLYAEOIFUOQ5EOX/graph.json","events_json":"https://pith.science/api/pith-number/IXJ2RUMLZ4ASLYAEOIFUOQ5EOX/events.json","paper":"https://pith.science/paper/IXJ2RUML"},"agent_actions":{"view_html":"https://pith.science/pith/IXJ2RUMLZ4ASLYAEOIFUOQ5EOX","download_json":"https://pith.science/pith/IXJ2RUMLZ4ASLYAEOIFUOQ5EOX.json","view_paper":"https://pith.science/paper/IXJ2RUML","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1010.1498&json=true","fetch_graph":"https://pith.science/api/pith-number/IXJ2RUMLZ4ASLYAEOIFUOQ5EOX/graph.json","fetch_events":"https://pith.science/api/pith-number/IXJ2RUMLZ4ASLYAEOIFUOQ5EOX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/IXJ2RUMLZ4ASLYAEOIFUOQ5EOX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/IXJ2RUMLZ4ASLYAEOIFUOQ5EOX/action/storage_attestation","attest_author":"https://pith.science/pith/IXJ2RUMLZ4ASLYAEOIFUOQ5EOX/action/author_attestation","sign_citation":"https://pith.science/pith/IXJ2RUMLZ4ASLYAEOIFUOQ5EOX/action/citation_signature","submit_replication":"https://pith.science/pith/IXJ2RUMLZ4ASLYAEOIFUOQ5EOX/action/replication_record"}},"created_at":"2026-05-18T04:25:49.197911+00:00","updated_at":"2026-05-18T04:25:49.197911+00:00"}