{"paper":{"title":"$T$-odd correlations in polarized top quark decays in the sequential decay $t(\\uparrow) \\to X_b+W^+(\\to \\ell^+ + \\nu_\\ell)$ and in the quasi three-body decay $t(\\uparrow) \\to X_b+ \\ell^+ + \\nu_\\ell$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"J.G. K\\\"orner, M. Fischer, S. Groote","submitted_at":"2018-02-07T15:48:42Z","abstract_excerpt":"We identify the $T$-odd structure functions that appear in the description of polarized top quark decays in the sequential decay $t(\\uparrow) \\to X_b+W^+(\\to \\ell^+ + \\nu_\\ell)$ (two structure functions) and the quasi-three-body decay $t(\\uparrow) \\to X_b+ \\ell^+ + \\nu_\\ell$ (one structure function). A convenient measure of the magnitude of the $T$-odd structure functions is the contribution of the imaginary part Im $g_R$ of the right-chiral tensor coupling $g_R$ to the $T$-odd structure functions which we work out. Contrary to the case of QCD the NLO electroweak corrections to polarized top q"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1802.02492","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"}