Flavor changing neutral current decays tcXt\to c X (X=γ,g,Z,HX=\gamma,\,g,\, Z,\, H) and tcˉt\to c\bar \ell\ell (=μ,τ\ell=\mu,\,\tau) via scalar leptoquarks

Jul 12, 2019
24 pages
Published in:
  • Eur.Phys.J.C 79 (2019) 8, 700
  • Published: Aug 21, 2019
e-Print:

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Abstract: (Springer)
The flavor changing neutral current decays tcXt\rightarrow c X ( X=γ,g,Z,HX=\gamma ,\,g,\, Z,\, H ) and tcˉt\rightarrow c{{\bar{\ell }}}\ell ( =μ,τ\ell =\mu ,\,\tau ) are studied in a renormalizable scalar leptoquark (LQ) model with no proton decay, where a scalar SU(2) doublet with hypercharge Y=7/6Y=7/6 is added to the standard model, yielding a non-chiral LQ Ω5/3\varOmega _{5/3} . Analytical results for the one-loop (tree-level) contributions of a scalar LQ to the fifjXf_i\rightarrow f_j X ( fifjfˉmflf_i\rightarrow f_j {\bar{f}}_m f_l ) decays, with fa=qa,af_a=q_a, \ell _a , are presented. We consider the scenario where Ω5/3\varOmega _{5/3} couples to the fermions of the second and third families, with its right- and left-handed couplings obeying λRui/λLui=O(ϵ)\lambda _R^{\ell u_i}/\lambda _L^{\ell u_i}=O(\epsilon ) , where ϵ\epsilon parametrizes the relative size between these couplings. The allowed parameter space is then found via the current constraints on the muon (g2)(g-2) , the τμγ\tau \rightarrow \mu \gamma decay, the LHC Higgs boson data, and the direct LQ searches at the LHC. For mΩ5/3=1m_{\varOmega _{5/3}}=1 TeV and ϵ=103\epsilon =10^{-3} , we find that the tcXt\rightarrow c X branching ratios are of similar size and can be as large as 10810^{-8} in a tiny area of the parameter space, whereas Br(tcτˉτ){\mathrm{Br}}(t\rightarrow c{{\bar{\tau }}}\tau ) [ Br(tcμˉμ){\mathrm{Br}}(t\rightarrow c{{\bar{\mu }}}\mu ) ] can be up to 10610^{-6} ( 10710^{-7} ).
Note:
  • 24 pags, 10 figures, 1 table
  • leptoquark: scalar
  • leptoquark: mass
  • charge: 5/3
  • neutral current: flavor changing
  • top: decay
  • top: branching ratio
  • decay: flavor changing
  • tau: radiative decay
  • p: decay
  • coupling: left-handed