Abstract

We revisit the possibilities of accommodating the experimental indications of the lepton flavor universality violation in $b$-hadron decays in the minimal scenarios in which the Standard Model is extended by the presence of a single $\mathcal{O}(1\,\mathrm{TeV})$ leptoquark state. To do so we combine the most recent low energy flavor physics constraints, including $R_{K^{(\ast)}}^\mathrm{exp}$ and $R_{D^{(\ast)}}^\mathrm{exp}$, and combine them with the bounds on the leptoquark masses and their couplings to quarks and leptons as inferred from the direct searches at the LHC and the studies of the large $p_T$ tails of the $pp\to \ell\ell$ differential cross section. We find that none of the scalar leptoquarks of $m_\mathrm{LQ} \simeq 1\div 2$ TeV can accommodate the $B$-anomalies alone. Only the vector leptoquark, known as $U_1$, can provide a viable solution which, in the minimal setup, provides an interesting prediction, i.e. a lower bound to the lepton flavor violating $b\to s\mu^\pm\tau^\mp$ decay modes, such as $\mathcal{B}(B\to K\mu\tau) \gtrsim 0.7\times 10^{-7}$.

Highlights

  • In Ref. [1] we made a comprehensive phenomenological analysis of the new physics (NP) scenarios in which the Standard Model (SM) is extended minimally by a single Oð1 TeVÞ leptoquark state

  • In this work we revisited our previous phenomenological study and examined the viability of the scenarios in which the SM is extended by only one Oð1 TeVÞ LQ after comparing them to the most recent experimental results, in addition to those already discussed in our Ref. [1]

  • Besides the low-energy observables, we exploit the most recent experimental improvements regarding the direct searches and the high pT considerations of the pp → ll differential cross section studied at the LHC

Read more

Summary

INTRODUCTION

In Ref. [1] we made a comprehensive phenomenological analysis of the new physics (NP) scenarios in which the Standard Model (SM) is extended minimally by a single Oð1 TeVÞ leptoquark state. BðBs → μμÞ 1⁄4 ð2.70 Æ 0.36Þ × 10−9; ð4Þ to which we include the most recent update of the LHCb result BðBs → μμÞ 1⁄4 ð3.09þ−00..4448Þ × 10−9 [7], 1We combined the errors in quadrature before symmetrizing them. (iii) Experimental indications of LFUV have been observed in the b → clνl decays, and in. In the following we will use the above experimental improvements, combine them with theoretical expressions used in Ref. [1] and references therein, or with the improved expressions which will be properly referred to in the body of this letter organized as follows: In Sec. II we update the effective field theory (EFT) analysis of the transitions b → sμμ and b → cτνto determine the effective coefficients that can accommodate the latest experimental results for RKðÃÞ and RDðÃÞ.

RK and RKÃ
RD and RDÃ
LHC CONSTRAINTS
Direct searches
Bounds from indirect high-pT searches
WHICH LEPTOQUARK?
CONCLUSIONS
Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.