{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:DIPT24B3OAAUM4Q7WXRNUDEHQW","short_pith_number":"pith:DIPT24B3","schema_version":"1.0","canonical_sha256":"1a1f3d703b700146721fb5e2da0c8785be5366992f349969d588a1943717cf81","source":{"kind":"arxiv","id":"1007.5313","version":3},"attestation_state":"computed","paper":{"title":"Next-to-leading order QCD predictions for W+W+jj production at the LHC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Giulia Zanderighi, Kirill Melnikov, Raoul Rontsch, Tom Melia","submitted_at":"2010-07-29T20:00:24Z","abstract_excerpt":"Because the LHC is a proton-proton collider, sizable production of two positively charged W-bosons in association with two jets is possible. This process leads to a distinct signature of same sign high-pt leptons, missing energy and jets. We compute the NLO QCD corrections to the QCD-mediated part of pp -> W+W+jj. These corrections reduce the dependence of the production cross-section on the renormalization and factorization scale to about +- 10 percent. We find that a large number of W+W+jj events contain a relatively hard third jet. The presence of this jet should help to either pick up the "},"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":"1007.5313","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-07-29T20:00:24Z","cross_cats_sorted":[],"title_canon_sha256":"d84db5cf39a03e674b3003faa80e6f0eb303e31aec9371f6be49a4e3b2040fb1","abstract_canon_sha256":"0798b1430e2e20ca003f666052e0a5ddc333fe3789d1710a77f87aa463f90d71"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:21:13.664250Z","signature_b64":"OVS3GheVSPPuu9rGGvGig50hMSFYc3+xXJ0FjH3UQLyWRRM5QEb9k58Idg5yczSogyohFoqXOCEaoZ/lcc4FBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1a1f3d703b700146721fb5e2da0c8785be5366992f349969d588a1943717cf81","last_reissued_at":"2026-05-18T04:21:13.663544Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:21:13.663544Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Next-to-leading order QCD predictions for W+W+jj production at the LHC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Giulia Zanderighi, Kirill Melnikov, Raoul Rontsch, Tom Melia","submitted_at":"2010-07-29T20:00:24Z","abstract_excerpt":"Because the LHC is a proton-proton collider, sizable production of two positively charged W-bosons in association with two jets is possible. This process leads to a distinct signature of same sign high-pt leptons, missing energy and jets. We compute the NLO QCD corrections to the QCD-mediated part of pp -> W+W+jj. These corrections reduce the dependence of the production cross-section on the renormalization and factorization scale to about +- 10 percent. We find that a large number of W+W+jj events contain a relatively hard third jet. The presence of this jet should help to either pick up the "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1007.5313","kind":"arxiv","version":3},"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":"1007.5313","created_at":"2026-05-18T04:21:13.663668+00:00"},{"alias_kind":"arxiv_version","alias_value":"1007.5313v3","created_at":"2026-05-18T04:21:13.663668+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1007.5313","created_at":"2026-05-18T04:21:13.663668+00:00"},{"alias_kind":"pith_short_12","alias_value":"DIPT24B3OAAU","created_at":"2026-05-18T12:26:06.534383+00:00"},{"alias_kind":"pith_short_16","alias_value":"DIPT24B3OAAUM4Q7","created_at":"2026-05-18T12:26:06.534383+00:00"},{"alias_kind":"pith_short_8","alias_value":"DIPT24B3","created_at":"2026-05-18T12:26:06.534383+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2606.19999","citing_title":"NLO QCD and EW corrections to semileptonic vector-boson scattering at the LHC","ref_index":15,"is_internal_anchor":true},{"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":266,"is_internal_anchor":false},{"citing_arxiv_id":"2604.18025","citing_title":"Precision calculations for electroweak multi-boson processes","ref_index":20,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/DIPT24B3OAAUM4Q7WXRNUDEHQW","json":"https://pith.science/pith/DIPT24B3OAAUM4Q7WXRNUDEHQW.json","graph_json":"https://pith.science/api/pith-number/DIPT24B3OAAUM4Q7WXRNUDEHQW/graph.json","events_json":"https://pith.science/api/pith-number/DIPT24B3OAAUM4Q7WXRNUDEHQW/events.json","paper":"https://pith.science/paper/DIPT24B3"},"agent_actions":{"view_html":"https://pith.science/pith/DIPT24B3OAAUM4Q7WXRNUDEHQW","download_json":"https://pith.science/pith/DIPT24B3OAAUM4Q7WXRNUDEHQW.json","view_paper":"https://pith.science/paper/DIPT24B3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1007.5313&json=true","fetch_graph":"https://pith.science/api/pith-number/DIPT24B3OAAUM4Q7WXRNUDEHQW/graph.json","fetch_events":"https://pith.science/api/pith-number/DIPT24B3OAAUM4Q7WXRNUDEHQW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DIPT24B3OAAUM4Q7WXRNUDEHQW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DIPT24B3OAAUM4Q7WXRNUDEHQW/action/storage_attestation","attest_author":"https://pith.science/pith/DIPT24B3OAAUM4Q7WXRNUDEHQW/action/author_attestation","sign_citation":"https://pith.science/pith/DIPT24B3OAAUM4Q7WXRNUDEHQW/action/citation_signature","submit_replication":"https://pith.science/pith/DIPT24B3OAAUM4Q7WXRNUDEHQW/action/replication_record"}},"created_at":"2026-05-18T04:21:13.663668+00:00","updated_at":"2026-05-18T04:21:13.663668+00:00"}