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T-odd correlations in polarized top quark decays in the sequential decay t(uparrow) to X_b+W^+(to ell^+ + ν_ell) and in the quasi three-body decay t(uparrow) to X_b+ ell^+ + ν_ell
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T-odd correlations in polarized top quark decays in the sequential decay t(uparrow) to X_b+W^+(to ell^+ + ν_ell) and in the quasi three-body decay t(uparrow) to X_b+ ell^+ + ν_ell
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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 quark decays admit of absorptive one-loop vertex contributions. We analytically calculate the imaginary parts of the relevant four electroweak one-loop triangle vertex diagrams and determine their contributions to the $T$-odd helicity structure functions that appear in the description of polarized top quark decays.
Forward citations
Cited by 2 Pith papers
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CP-odd SMEFT top interactions appear as ΔB and antisymmetric C_A in the tt̄ production density matrix; direct markers beat most QI measures for CP sensitivity at LHC and FCC-ee.
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