{"paper":{"title":"QCD and electroweak corrections to WZ scattering at the LHC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Ansgar Denner, Christopher Schwan, Mathieu Pellen, Philipp Maierh\\\"ofer, Stefan Dittmaier","submitted_at":"2019-04-01T14:27:28Z","abstract_excerpt":"We present the first computation of the full next-to-leading-order QCD and electroweak corrections to the WZ scattering process at the LHC. All off-shell, gauge-boson-decay, and interference effects are taken into account for the process $\\mathrm{p} \\mathrm{p} \\to \\mu^+\\mu^-\\mathrm{e}^+\\nu_\\mathrm{e} \\mathrm{j} \\mathrm{j} + X$ at the orders $\\mathcal{O}{\\left( \\alpha_\\mathrm{s} \\alpha^6 \\right)}$ and $\\mathcal{O}{\\left( \\alpha^7 \\right)}$. The electroweak corrections feature the typical Sudakov behaviour towards high energy and amount to $-16\\%$ relative to the electroweak contribution to the "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1904.00882","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"}