Abstract

We investigate the possibility that scalar leptoquarks generate consequential effects on the flavor-changing neutral-current decays of charmed hadrons into final states with missing energy carried away by either standard model or sterile neutrinos. We focus on scenarios involving the R2, {tilde{R}}_2 , and {overline{S}}_1 leptoquarks and take into account various pertinent constraints, learning that meson-mixing ones and those inferred from collider searches can be of significance. We find in particular that the branching fractions of charmed meson decays D →, M = π, ρ, and Ds→ and singly charmed baryon decays {Lambda}_c^{+} → and Ξc→ are presently allowed to attain the 10−7-10−6 levels if induced by R2 and that the impact of {tilde{R}}_2 is comparatively much less. In contrast, the contributions of {overline{S}}_1 , which couples to right-handed up-type quarks and the sterile neutrinos, could lead to branching fractions as high as order 10−3. This suggests that these charmed hadron decays might be within reach of the BESIII and Belle II experiments or future super charm-tau factories and could serve as potentially promising probes of leptoquark interactions with sterile neutrinos.

Highlights

  • The foregoing motivates us in this paper to explore these FCNC charm transitions with missing energy in the contexts of relatively simple NP scenarios

  • We investigate the possibility that scalar leptoquarks generate consequential effects on the flavor-changing neutral-current decays of charmed hadrons into final states with missing energy (E/ ) carried away by either standard model or sterile neutrinos

  • This suggests that these charmed hadron decays might be within reach of the BESIII and Belle II experiments or future super charm-tau factories and could serve as potentially promising probes of leptoquark interactions with sterile neutrinos

Read more

Summary

Leptoquark couplings to fermions

Among LQs that can have renormalizable interactions with SM fermions without violating the conservations of baryon and lepton numbers and the SM gauge symmetries, there are four which possess spin 0 and can at tree level contribute to the quark transition c → uE/ where the missing energy is carried away by either SM or sterile neutrinos [7].1. As for the right-handed neutrinos, we assume that there are three of them (N1, N2, and N3) and that they are of Dirac nature. Where Yr2,ljy, yl2r,jy , and yr1,rjy are generally complex elements of the LQ Yukawa matrices, summation over family indices j, y = 1, 2, 3 is implicit, qj (ly) and uj symbolize a lefthanded quark (lepton) doublet and right-handed up-type quark singlet, τ2 is the second Pauli matrix, PL,R = (1 ∓ γ5)/2, and the superscript c indicates charge conjugation. We entertain three distinct possibilities each involving one of the LQs, taken to be heavy, with the couplings specified above

R2 model
S1 model
Conclusions
Findings
A Branching ratio formulas
Full Text
Published version (Free)

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