2013
DOI: 10.1007/jhep11(2013)084
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Minimally flavored colored scalar in $ \overline{B}\to {D^{{\left( * \right)}}}\tau \overline{\nu} $ and the mass matrices constraints

Abstract: The presence of a colored scalar that is a weak doublet with fractional electric charges of |Q| = 2/3 and |Q| = 5/3 with mass below 1 TeV can provide an explanation of the observed branching ratios in B → D ( * ) τν decays. The required combination of scalar and tensor operators in the effective Hamiltonian for b → cτν is generated through the t-channel exchange. We focus on a scenario with a minimal set of Yukawa couplings that can address a semitauonic puzzle and show that its resolution puts a nontrivial bo… Show more

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Cited by 148 publications
(91 citation statements)
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“…The largest effects in presented LQ model are expected for third generation final states both in flavor conserving decays, as in Z → τ + τ − , which has been shown to have only weak constraining power in ref. [66], as well as in LFV modes Z → τ ± µ ∓ . The latter decay happens due to penguin diagrams with S 3 as well as 1-particle reducible diagrams and is suppressed by a loop factor and small ratio…”
Section: Z → µτ and τ → 3µmentioning
confidence: 96%
“…The largest effects in presented LQ model are expected for third generation final states both in flavor conserving decays, as in Z → τ + τ − , which has been shown to have only weak constraining power in ref. [66], as well as in LFV modes Z → τ ± µ ∓ . The latter decay happens due to penguin diagrams with S 3 as well as 1-particle reducible diagrams and is suppressed by a loop factor and small ratio…”
Section: Z → µτ and τ → 3µmentioning
confidence: 96%
“…Only the first two states have definite baryon and lepton numbers. Among all scalar LQs we will consider only the baryon number conserving state (3, 2, 7/6), which comes with a rich set of couplings that are in general severely constrained by B and K physics [38]. Then, among the two baryon number conserving vector LQs we will focus on the state in the representation (3, 1, 5/3) whose phenomenology is limited to the up-type quarks and charged leptons.…”
Section: Leptoquarksmentioning
confidence: 99%
“…Notice, however, that this model cannot explain R D ( * ) , the fact that was already (implicitly) shown in ref. [31].…”
Section: Introductionmentioning
confidence: 99%