{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:N7DV4XZRRZEOJVIB3CJGJBNUJ4","short_pith_number":"pith:N7DV4XZR","schema_version":"1.0","canonical_sha256":"6fc75e5f318e48e4d501d8926485b44f226f1d64f539fef6f88de31c47f387c8","source":{"kind":"arxiv","id":"1311.6738","version":2},"attestation_state":"computed","paper":{"title":"Next-to-leading order QCD corrections to $W^+W^+$ and $W^-W^-$ production in association with two jets","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Dieter Zeppenfeld, Francisco Campanario, Le Duc Ninh, Matthias Kerner","submitted_at":"2013-11-26T17:02:32Z","abstract_excerpt":"We present a study of $W^+W^+jj$ and $W^-W^-jj$ production including leptonic decays in hadron-hadron collisions. The full electroweak and QCD induced contributions and their interferences are calculated at leading order. We find that, for inclusive cuts, the interference effects can be large if the jets are produced with large transverse momentum where, however, the production rate is suppressed. We also discuss the vector-boson-fusion (VBF) cuts and show the validity of the VBF approximation. The NLO QCD corrections to the QCD-induced channels are also calculated. Compared to the previous ca"},"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":"1311.6738","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-11-26T17:02:32Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"3daa497c42290be1d6ba214886cda705a8b07a39e0ec2e7f4682c95cc6f2cb7d","abstract_canon_sha256":"4ff8cbf22ed6ca7ab494ec53aae7e6f25c8c4a1340f3528bb4f0aff108893e58"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:55:57.104442Z","signature_b64":"1qc40ZPHCAeuwHbJrOOsU4IWaKp2WKtdvA12NC2Vrn3fMQrro9gtK8RQOiyXP23FmsAzZA3j7cP0Tx5lfQidDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6fc75e5f318e48e4d501d8926485b44f226f1d64f539fef6f88de31c47f387c8","last_reissued_at":"2026-05-18T02:55:57.103975Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:55:57.103975Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Next-to-leading order QCD corrections to $W^+W^+$ and $W^-W^-$ production in association with two jets","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Dieter Zeppenfeld, Francisco Campanario, Le Duc Ninh, Matthias Kerner","submitted_at":"2013-11-26T17:02:32Z","abstract_excerpt":"We present a study of $W^+W^+jj$ and $W^-W^-jj$ production including leptonic decays in hadron-hadron collisions. The full electroweak and QCD induced contributions and their interferences are calculated at leading order. We find that, for inclusive cuts, the interference effects can be large if the jets are produced with large transverse momentum where, however, the production rate is suppressed. We also discuss the vector-boson-fusion (VBF) cuts and show the validity of the VBF approximation. The NLO QCD corrections to the QCD-induced channels are also calculated. Compared to the previous ca"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1311.6738","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":""},"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":"1311.6738","created_at":"2026-05-18T02:55:57.104040+00:00"},{"alias_kind":"arxiv_version","alias_value":"1311.6738v2","created_at":"2026-05-18T02:55:57.104040+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1311.6738","created_at":"2026-05-18T02:55:57.104040+00:00"},{"alias_kind":"pith_short_12","alias_value":"N7DV4XZRRZEO","created_at":"2026-05-18T12:27:52.871228+00:00"},{"alias_kind":"pith_short_16","alias_value":"N7DV4XZRRZEOJVIB","created_at":"2026-05-18T12:27:52.871228+00:00"},{"alias_kind":"pith_short_8","alias_value":"N7DV4XZR","created_at":"2026-05-18T12:27:52.871228+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"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":267,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/N7DV4XZRRZEOJVIB3CJGJBNUJ4","json":"https://pith.science/pith/N7DV4XZRRZEOJVIB3CJGJBNUJ4.json","graph_json":"https://pith.science/api/pith-number/N7DV4XZRRZEOJVIB3CJGJBNUJ4/graph.json","events_json":"https://pith.science/api/pith-number/N7DV4XZRRZEOJVIB3CJGJBNUJ4/events.json","paper":"https://pith.science/paper/N7DV4XZR"},"agent_actions":{"view_html":"https://pith.science/pith/N7DV4XZRRZEOJVIB3CJGJBNUJ4","download_json":"https://pith.science/pith/N7DV4XZRRZEOJVIB3CJGJBNUJ4.json","view_paper":"https://pith.science/paper/N7DV4XZR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1311.6738&json=true","fetch_graph":"https://pith.science/api/pith-number/N7DV4XZRRZEOJVIB3CJGJBNUJ4/graph.json","fetch_events":"https://pith.science/api/pith-number/N7DV4XZRRZEOJVIB3CJGJBNUJ4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/N7DV4XZRRZEOJVIB3CJGJBNUJ4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/N7DV4XZRRZEOJVIB3CJGJBNUJ4/action/storage_attestation","attest_author":"https://pith.science/pith/N7DV4XZRRZEOJVIB3CJGJBNUJ4/action/author_attestation","sign_citation":"https://pith.science/pith/N7DV4XZRRZEOJVIB3CJGJBNUJ4/action/citation_signature","submit_replication":"https://pith.science/pith/N7DV4XZRRZEOJVIB3CJGJBNUJ4/action/replication_record"}},"created_at":"2026-05-18T02:55:57.104040+00:00","updated_at":"2026-05-18T02:55:57.104040+00:00"}