{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2008:44LHRQVLOZKUAMNZPPWMXDQZUE","short_pith_number":"pith:44LHRQVL","schema_version":"1.0","canonical_sha256":"e71678c2ab76554031b97beccb8e19a12ec64c2e523cb0471da12fa3bc931e50","source":{"kind":"arxiv","id":"0805.4802","version":1},"attestation_state":"computed","paper":{"title":"NLO vector-boson production matched with shower in POWHEG","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Carlo Oleari, Emanuele Re, Paolo Nason, Simone Alioli","submitted_at":"2008-05-30T16:51:15Z","abstract_excerpt":"We present a next-to-leading-order calculation of W/Z production interfaced to shower Monte Carlo, implemented according to the POWHEG method. Finite width effects, Z/gamma interference and angular correlations of decay products are included. A detailed comparison with MC@NLO and PYTHIA is carried out."},"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":"0805.4802","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2008-05-30T16:51:15Z","cross_cats_sorted":[],"title_canon_sha256":"7f5102733c7a049e97d886a99c041b89f5a56c31b7ecfb4d67dc76429713ee60","abstract_canon_sha256":"cb911a733aa28e17499204b39234b7b8993a5eec0fc0833099b112f74af164d4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:30:12.803139Z","signature_b64":"RhlBW7hxJDdKHdywShHxR3VV4Y11Vho3nVDtKySU2UAWkGqSwx++DDMnNWUuzuEasosYYxiw5SzJpx9bIu8sCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e71678c2ab76554031b97beccb8e19a12ec64c2e523cb0471da12fa3bc931e50","last_reissued_at":"2026-07-04T15:30:12.802609Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:30:12.802609Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"NLO vector-boson production matched with shower in POWHEG","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Carlo Oleari, Emanuele Re, Paolo Nason, Simone Alioli","submitted_at":"2008-05-30T16:51:15Z","abstract_excerpt":"We present a next-to-leading-order calculation of W/Z production interfaced to shower Monte Carlo, implemented according to the POWHEG method. Finite width effects, Z/gamma interference and angular correlations of decay products are included. A detailed comparison with MC@NLO and PYTHIA is carried out."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0805.4802","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/0805.4802/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":"0805.4802","created_at":"2026-07-04T15:30:12.802672+00:00"},{"alias_kind":"arxiv_version","alias_value":"0805.4802v1","created_at":"2026-07-04T15:30:12.802672+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0805.4802","created_at":"2026-07-04T15:30:12.802672+00:00"},{"alias_kind":"pith_short_12","alias_value":"44LHRQVLOZKU","created_at":"2026-07-04T15:30:12.802672+00:00"},{"alias_kind":"pith_short_16","alias_value":"44LHRQVLOZKUAMNZ","created_at":"2026-07-04T15:30:12.802672+00:00"},{"alias_kind":"pith_short_8","alias_value":"44LHRQVL","created_at":"2026-07-04T15:30:12.802672+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":12,"internal_anchor_count":7,"sample":[{"citing_arxiv_id":"2605.26462","citing_title":"Search for a new heavy scalar resonance decaying to a pair of Z bosons in the four-lepton final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","ref_index":26,"is_internal_anchor":true},{"citing_arxiv_id":"2605.25103","citing_title":"Search for low-mass resonances decaying to $\\tau\\tau$ and measurement of the $\\Upsilon$ $\\to$ $\\tau\\tau$ decay in proton-proton collisions at $\\sqrt{s}$ = 13.6 TeV","ref_index":44,"is_internal_anchor":true},{"citing_arxiv_id":"1907.02029","citing_title":"Towards a W boson mass measurement with LHCb","ref_index":10,"is_internal_anchor":true},{"citing_arxiv_id":"2605.20015","citing_title":"Search for soft unclustered energy patterns containing muons in the final state in $pp$ collisions at $\\sqrt{s}$ = 13 TeV with the ATLAS detector","ref_index":42,"is_internal_anchor":true},{"citing_arxiv_id":"2605.15396","citing_title":"First measurements of vector boson scattering in W$^\\pm$W$^{\\pm}$ and WZ production in all-leptonic final states at $\\sqrt{s}$ = 13.6 TeV","ref_index":52,"is_internal_anchor":true},{"citing_arxiv_id":"2509.13759","citing_title":"Measurement of the $W$-boson angular coefficients and transverse momentum in $pp$ collisions at $\\sqrt{s}=$ 13 TeV with the ATLAS detector","ref_index":42,"is_internal_anchor":true},{"citing_arxiv_id":"2509.12012","citing_title":"DeepMET: Improving missing transverse momentum estimation with a deep neural network","ref_index":24,"is_internal_anchor":true},{"citing_arxiv_id":"1002.2581","citing_title":"A general framework for implementing NLO calculations in shower Monte Carlo programs: the POWHEG BOX","ref_index":7,"is_internal_anchor":false},{"citing_arxiv_id":"2604.26124","citing_title":"Recent Developments in IR-Improved Amplitude-Based Resummation in Precision High Energy Collider Physics","ref_index":23,"is_internal_anchor":false},{"citing_arxiv_id":"2604.21670","citing_title":"Effective field theory interpretation of ATLAS measurements involving the Higgs boson, electroweak bosons and the top quark","ref_index":93,"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":231,"is_internal_anchor":false},{"citing_arxiv_id":"2604.12706","citing_title":"Measurement of the $W$-boson production cross-sections in $pp$ collisions at $\\sqrt{s}$ = 13 TeV in the forward region","ref_index":74,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/44LHRQVLOZKUAMNZPPWMXDQZUE","json":"https://pith.science/pith/44LHRQVLOZKUAMNZPPWMXDQZUE.json","graph_json":"https://pith.science/api/pith-number/44LHRQVLOZKUAMNZPPWMXDQZUE/graph.json","events_json":"https://pith.science/api/pith-number/44LHRQVLOZKUAMNZPPWMXDQZUE/events.json","paper":"https://pith.science/paper/44LHRQVL"},"agent_actions":{"view_html":"https://pith.science/pith/44LHRQVLOZKUAMNZPPWMXDQZUE","download_json":"https://pith.science/pith/44LHRQVLOZKUAMNZPPWMXDQZUE.json","view_paper":"https://pith.science/paper/44LHRQVL","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0805.4802&json=true","fetch_graph":"https://pith.science/api/pith-number/44LHRQVLOZKUAMNZPPWMXDQZUE/graph.json","fetch_events":"https://pith.science/api/pith-number/44LHRQVLOZKUAMNZPPWMXDQZUE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/44LHRQVLOZKUAMNZPPWMXDQZUE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/44LHRQVLOZKUAMNZPPWMXDQZUE/action/storage_attestation","attest_author":"https://pith.science/pith/44LHRQVLOZKUAMNZPPWMXDQZUE/action/author_attestation","sign_citation":"https://pith.science/pith/44LHRQVLOZKUAMNZPPWMXDQZUE/action/citation_signature","submit_replication":"https://pith.science/pith/44LHRQVLOZKUAMNZPPWMXDQZUE/action/replication_record"}},"created_at":"2026-07-04T15:30:12.802672+00:00","updated_at":"2026-07-04T15:30:12.802672+00:00"}