{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:WQLPIH3ASLLNGZOFFJKPM4PNN5","short_pith_number":"pith:WQLPIH3A","schema_version":"1.0","canonical_sha256":"b416f41f6092d6d365c52a54f671ed6f51d3231ce852027eb891bfd30107642d","source":{"kind":"arxiv","id":"1607.00763","version":1},"attestation_state":"computed","paper":{"title":"On the maximal use of Monte Carlo samples: re-weighting events at NLO accuracy","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Olivier Mattelaer","submitted_at":"2016-07-04T08:19:35Z","abstract_excerpt":"Accurate Monte Carlo simulations for high-energy events at CERN's Large Hadron Collider, are very expensive, both from the computing and storage points of view. We describe a method that allows to consistently re-use parton-level samples accurate up to NLO in QCD under different theoretical hypotheses. We implement it in MadGraph5_aMC@NLO and show its validation by applying it to several cases of practical interest for the search of new physics at the LHC."},"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":"1607.00763","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-07-04T08:19:35Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"4eec8d21da070c3e7aa62060a17d7bfd0eb28c23bb7ca00cf6296b028e82845e","abstract_canon_sha256":"f8370fcf095e1cbc6250c4a7e596ae7dc40bb87a03c0aafa7be5207fd69e6dde"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:54:35.801578Z","signature_b64":"kKYZizJLt5QKJVxn6YWRQi4VroTWe7gAh6Xv5KleQ3m1MhyFWFXi17DDOmQpoZTBf3IfaaijqAIvMvBppTrvDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b416f41f6092d6d365c52a54f671ed6f51d3231ce852027eb891bfd30107642d","last_reissued_at":"2026-05-18T00:54:35.800955Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:54:35.800955Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"On the maximal use of Monte Carlo samples: re-weighting events at NLO accuracy","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Olivier Mattelaer","submitted_at":"2016-07-04T08:19:35Z","abstract_excerpt":"Accurate Monte Carlo simulations for high-energy events at CERN's Large Hadron Collider, are very expensive, both from the computing and storage points of view. We describe a method that allows to consistently re-use parton-level samples accurate up to NLO in QCD under different theoretical hypotheses. We implement it in MadGraph5_aMC@NLO and show its validation by applying it to several cases of practical interest for the search of new physics at the LHC."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1607.00763","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":"1607.00763","created_at":"2026-05-18T00:54:35.801028+00:00"},{"alias_kind":"arxiv_version","alias_value":"1607.00763v1","created_at":"2026-05-18T00:54:35.801028+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1607.00763","created_at":"2026-05-18T00:54:35.801028+00:00"},{"alias_kind":"pith_short_12","alias_value":"WQLPIH3ASLLN","created_at":"2026-05-18T12:30:51.357362+00:00"},{"alias_kind":"pith_short_16","alias_value":"WQLPIH3ASLLNGZOF","created_at":"2026-05-18T12:30:51.357362+00:00"},{"alias_kind":"pith_short_8","alias_value":"WQLPIH3A","created_at":"2026-05-18T12:30:51.357362+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":4,"sample":[{"citing_arxiv_id":"2411.00096","citing_title":"Why detect forward muons at a muon collider","ref_index":84,"is_internal_anchor":true},{"citing_arxiv_id":"2504.05919","citing_title":"Measurement of high-mass $t\\bar{t}\\ell^{+}\\ell^{-}$ production and lepton flavour universality-inspired effective field theory interpretations at $\\sqrt{s}=13$ TeV with the ATLAS detector","ref_index":72,"is_internal_anchor":true},{"citing_arxiv_id":"2605.16036","citing_title":"The Monte Carlo Ecosystem in High-Energy Physics: A Primer","ref_index":277,"is_internal_anchor":true},{"citing_arxiv_id":"2510.17730","citing_title":"Automated computation of spin-density matrices and quantum observables for collider physics","ref_index":146,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/WQLPIH3ASLLNGZOFFJKPM4PNN5","json":"https://pith.science/pith/WQLPIH3ASLLNGZOFFJKPM4PNN5.json","graph_json":"https://pith.science/api/pith-number/WQLPIH3ASLLNGZOFFJKPM4PNN5/graph.json","events_json":"https://pith.science/api/pith-number/WQLPIH3ASLLNGZOFFJKPM4PNN5/events.json","paper":"https://pith.science/paper/WQLPIH3A"},"agent_actions":{"view_html":"https://pith.science/pith/WQLPIH3ASLLNGZOFFJKPM4PNN5","download_json":"https://pith.science/pith/WQLPIH3ASLLNGZOFFJKPM4PNN5.json","view_paper":"https://pith.science/paper/WQLPIH3A","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1607.00763&json=true","fetch_graph":"https://pith.science/api/pith-number/WQLPIH3ASLLNGZOFFJKPM4PNN5/graph.json","fetch_events":"https://pith.science/api/pith-number/WQLPIH3ASLLNGZOFFJKPM4PNN5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WQLPIH3ASLLNGZOFFJKPM4PNN5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WQLPIH3ASLLNGZOFFJKPM4PNN5/action/storage_attestation","attest_author":"https://pith.science/pith/WQLPIH3ASLLNGZOFFJKPM4PNN5/action/author_attestation","sign_citation":"https://pith.science/pith/WQLPIH3ASLLNGZOFFJKPM4PNN5/action/citation_signature","submit_replication":"https://pith.science/pith/WQLPIH3ASLLNGZOFFJKPM4PNN5/action/replication_record"}},"created_at":"2026-05-18T00:54:35.801028+00:00","updated_at":"2026-05-18T00:54:35.801028+00:00"}