{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:FREHTSWYGJIS75EEEWOITKN6J4","short_pith_number":"pith:FREHTSWY","schema_version":"1.0","canonical_sha256":"2c4879cad832512ff484259c89a9be4f1dd94ac8b326a33aa9276593b206d414","source":{"kind":"arxiv","id":"hep-th/0512336","version":2},"attestation_state":"computed","paper":{"title":"Twistor diagrams for all tree amplitudes in gauge theory: a helicity-independent formalism","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Andrew Hodges","submitted_at":"2005-12-29T13:00:18Z","abstract_excerpt":"We give a new formalism for pure gauge-theoretic scattering at tree-amplitude level. We first describe a generalization of the Britto-Cachazo-Feng recursion relation in which a significant restriction is removed. We then use twistor diagrams to express all tree amplitudes in a form independent of helicity. A formal procedure involving anticommuting elements is required. We illustrate the results with specific calculations of interest, up to 8 interacting fields."},"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":"hep-th/0512336","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2005-12-29T13:00:18Z","cross_cats_sorted":[],"title_canon_sha256":"bfc3d9a0ce9357bb509a692e6b4ae6af90c888dd24a9e7e7adff16f716b2261f","abstract_canon_sha256":"81c0e2308f6963da297f31c3b1913efe3dab478f748659ed6c646aa3db84a478"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:52:11.403015Z","signature_b64":"HO7OrN5paq3BmGHg2M9l6Ccx1qdqEZHDM5lbfkquswasFB/53SYi5SCC5RvN+s9V0TBHhoY5QzCd2fDiuv8cCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2c4879cad832512ff484259c89a9be4f1dd94ac8b326a33aa9276593b206d414","last_reissued_at":"2026-07-04T14:52:11.402632Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:52:11.402632Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Twistor diagrams for all tree amplitudes in gauge theory: a helicity-independent formalism","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Andrew Hodges","submitted_at":"2005-12-29T13:00:18Z","abstract_excerpt":"We give a new formalism for pure gauge-theoretic scattering at tree-amplitude level. We first describe a generalization of the Britto-Cachazo-Feng recursion relation in which a significant restriction is removed. We then use twistor diagrams to express all tree amplitudes in a form independent of helicity. A formal procedure involving anticommuting elements is required. We illustrate the results with specific calculations of interest, up to 8 interacting fields."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0512336","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-th/0512336/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":"hep-th/0512336","created_at":"2026-07-04T14:52:11.402694+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0512336v2","created_at":"2026-07-04T14:52:11.402694+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0512336","created_at":"2026-07-04T14:52:11.402694+00:00"},{"alias_kind":"pith_short_12","alias_value":"FREHTSWYGJIS","created_at":"2026-07-04T14:52:11.402694+00:00"},{"alias_kind":"pith_short_16","alias_value":"FREHTSWYGJIS75EE","created_at":"2026-07-04T14:52:11.402694+00:00"},{"alias_kind":"pith_short_8","alias_value":"FREHTSWY","created_at":"2026-07-04T14:52:11.402694+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2506.05460","citing_title":"Generating Hodges' Graviton MHV Formula with an $Lw_{1+\\infty}$ Ward Identity","ref_index":17,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/FREHTSWYGJIS75EEEWOITKN6J4","json":"https://pith.science/pith/FREHTSWYGJIS75EEEWOITKN6J4.json","graph_json":"https://pith.science/api/pith-number/FREHTSWYGJIS75EEEWOITKN6J4/graph.json","events_json":"https://pith.science/api/pith-number/FREHTSWYGJIS75EEEWOITKN6J4/events.json","paper":"https://pith.science/paper/FREHTSWY"},"agent_actions":{"view_html":"https://pith.science/pith/FREHTSWYGJIS75EEEWOITKN6J4","download_json":"https://pith.science/pith/FREHTSWYGJIS75EEEWOITKN6J4.json","view_paper":"https://pith.science/paper/FREHTSWY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0512336&json=true","fetch_graph":"https://pith.science/api/pith-number/FREHTSWYGJIS75EEEWOITKN6J4/graph.json","fetch_events":"https://pith.science/api/pith-number/FREHTSWYGJIS75EEEWOITKN6J4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FREHTSWYGJIS75EEEWOITKN6J4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FREHTSWYGJIS75EEEWOITKN6J4/action/storage_attestation","attest_author":"https://pith.science/pith/FREHTSWYGJIS75EEEWOITKN6J4/action/author_attestation","sign_citation":"https://pith.science/pith/FREHTSWYGJIS75EEEWOITKN6J4/action/citation_signature","submit_replication":"https://pith.science/pith/FREHTSWYGJIS75EEEWOITKN6J4/action/replication_record"}},"created_at":"2026-07-04T14:52:11.402694+00:00","updated_at":"2026-07-04T14:52:11.402694+00:00"}