{"paper":{"title":"A precise characterisation of the top quark electro-weak vertices at the ILC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-ex","authors_text":"E. Ros, F. Richard, I. Garc\\`ia Garc\\`ia, J. Rou\\\"en\\'e, M. Boronat, M. Perell\\'o, M.S. Amjad, M. Vos, P. Doublet, P. Ruiz Femenia, R. P\\\"oschl, S. Bilokin, T. Frisson","submitted_at":"2015-05-22T10:37:24Z","abstract_excerpt":"Top quark production in the process $e^+e^- \\to t\\bar{t}$ at a future linear electron positron collider with polarised beams is a powerful tool to determine indirectly the scale of new physics. The presented study, based on a detailed simulation of the ILD detector concept, assumes a centre-of-mass energy of $\\sqrt{s}=500\\,$GeV and a luminosity of $\\mathcal{L}=500\\,{\\rm fb}^{-1}$ equally shared between the incoming beam polarisations of $\\mathcal{P}_{e^-}, \\mathcal{P}_{e^+} =\\pm0.8,\\mp0.3$. Events are selected in which the top pair decays semi-leptonically and the cross sections and the forwar"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1505.06020","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"}