{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2007:NH3F46UA63QFHELPLXEAZFO762","short_pith_number":"pith:NH3F46UA","schema_version":"1.0","canonical_sha256":"69f65e7a80f6e053916f5dc80c95dff6b8a7820e58d29fd4924a921380e617e6","source":{"kind":"arxiv","id":"0709.1026","version":2},"attestation_state":"computed","paper":{"title":"Parton showers from the dipole formalism","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Marko Ternick, Michael Dinsdale, Stefan Weinzierl","submitted_at":"2007-09-07T13:43:46Z","abstract_excerpt":"We present an implementation of a parton shower algorithm for hadron colliders and electron-positron colliders based on the dipole factorisation formulae. The algorithm treats initial-state partons on equal footing with final-state partons. We implemented the algorithm for massless and massive partons."},"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":"0709.1026","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2007-09-07T13:43:46Z","cross_cats_sorted":[],"title_canon_sha256":"face3fdf63164407708ad0eff706de4a11958c2e0aabc9fdb2aed2e230f0bf58","abstract_canon_sha256":"1f05d0fcc1211281ea9c26cd4905764d966e342d219fa55b1f61f8a27e6632d4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:27:44.144498Z","signature_b64":"p6PBHKYtXASMICtzDAeAPHV51YYlqrVRNJBv+bG9lt3XWAOx+CFNaybnRY5n7iplWDTxi3gpFS41Y4/hZTccAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"69f65e7a80f6e053916f5dc80c95dff6b8a7820e58d29fd4924a921380e617e6","last_reissued_at":"2026-07-04T15:27:44.143991Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:27:44.143991Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Parton showers from the dipole formalism","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Marko Ternick, Michael Dinsdale, Stefan Weinzierl","submitted_at":"2007-09-07T13:43:46Z","abstract_excerpt":"We present an implementation of a parton shower algorithm for hadron colliders and electron-positron colliders based on the dipole factorisation formulae. The algorithm treats initial-state partons on equal footing with final-state partons. We implemented the algorithm for massless and massive partons."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0709.1026","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/0709.1026/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":"0709.1026","created_at":"2026-07-04T15:27:44.144062+00:00"},{"alias_kind":"arxiv_version","alias_value":"0709.1026v2","created_at":"2026-07-04T15:27:44.144062+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0709.1026","created_at":"2026-07-04T15:27:44.144062+00:00"},{"alias_kind":"pith_short_12","alias_value":"NH3F46UA63QF","created_at":"2026-07-04T15:27:44.144062+00:00"},{"alias_kind":"pith_short_16","alias_value":"NH3F46UA63QFHELP","created_at":"2026-07-04T15:27:44.144062+00:00"},{"alias_kind":"pith_short_8","alias_value":"NH3F46UA","created_at":"2026-07-04T15:27:44.144062+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":7,"internal_anchor_count":3,"sample":[{"citing_arxiv_id":"2605.02622","citing_title":"Studying the Infrared Behaviour of Improved Logarithmic Accuracy Parton Showers with Herwig","ref_index":45,"is_internal_anchor":true},{"citing_arxiv_id":"2511.19633","citing_title":"An NLO-Matched Initial and Final State Parton Shower on a GPU","ref_index":40,"is_internal_anchor":true},{"citing_arxiv_id":"2511.19633","citing_title":"An NLO-Matched Initial and Final State Parton Shower on a GPU","ref_index":40,"is_internal_anchor":true},{"citing_arxiv_id":"2203.11601","citing_title":"A comprehensive guide to the physics and usage of PYTHIA 8.3","ref_index":116,"is_internal_anchor":false},{"citing_arxiv_id":"1405.0301","citing_title":"The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations","ref_index":178,"is_internal_anchor":false},{"citing_arxiv_id":"0709.2092","citing_title":"Matching NLO QCD computations with Parton Shower simulations: the POWHEG method","ref_index":11,"is_internal_anchor":false},{"citing_arxiv_id":"2605.02622","citing_title":"Studying the Infrared Behaviour of Improved Logarithmic Accuracy Parton Showers with Herwig","ref_index":45,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/NH3F46UA63QFHELPLXEAZFO762","json":"https://pith.science/pith/NH3F46UA63QFHELPLXEAZFO762.json","graph_json":"https://pith.science/api/pith-number/NH3F46UA63QFHELPLXEAZFO762/graph.json","events_json":"https://pith.science/api/pith-number/NH3F46UA63QFHELPLXEAZFO762/events.json","paper":"https://pith.science/paper/NH3F46UA"},"agent_actions":{"view_html":"https://pith.science/pith/NH3F46UA63QFHELPLXEAZFO762","download_json":"https://pith.science/pith/NH3F46UA63QFHELPLXEAZFO762.json","view_paper":"https://pith.science/paper/NH3F46UA","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0709.1026&json=true","fetch_graph":"https://pith.science/api/pith-number/NH3F46UA63QFHELPLXEAZFO762/graph.json","fetch_events":"https://pith.science/api/pith-number/NH3F46UA63QFHELPLXEAZFO762/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NH3F46UA63QFHELPLXEAZFO762/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NH3F46UA63QFHELPLXEAZFO762/action/storage_attestation","attest_author":"https://pith.science/pith/NH3F46UA63QFHELPLXEAZFO762/action/author_attestation","sign_citation":"https://pith.science/pith/NH3F46UA63QFHELPLXEAZFO762/action/citation_signature","submit_replication":"https://pith.science/pith/NH3F46UA63QFHELPLXEAZFO762/action/replication_record"}},"created_at":"2026-07-04T15:27:44.144062+00:00","updated_at":"2026-07-04T15:27:44.144062+00:00"}