Abstract

We study the discovery prospect of different three body lepton number violating~(LNV) meson decays $M_{1}^{-}\to\ell_{1}^{-}\ell_{2}^{-}M_{2}^{+}$ in the framework of right handed~(RH) neutrino extended Standard Model~(SM). We consider a number of ongoing experiments, such as, NA62 and LHCb at CERN, Belle II at SuperKEK, as well as at the proposed future experiments, SHiP, MATHUSLA and FCC-ee. The RH Majorana neutrino $N$ mediating these meson decays provides a resonant enhancement of the rates, if the mass of $N$ lies in the range $(100\, \text{MeV}-6\, \text{GeV})$. We consider the effect of parent mesons velocity, as well as, the effect of finite detector size. Using the expected upper limits on the number of events for the LNV decay modes, $M_{1}^{-} \to\ell_1^{-}\ell_2^{-}\pi^{+}$~($M_{1}=B, B_c,D, D_{s}\,\text{and}\,K$), we analyze the sensitivity reach of the mixing angles $|V_{e N}|^{2}$, $|V_{\mu N}|^{2}$, $|V_{\tau N}|^{2}$, $|V_{e N}V_{\mu N}|$, $|V_{e N}V_{\tau N}|$ and $|V_{\mu N}V_{\tau N}|$ as a function of heavy neutrino mass $M_{N}$. We show that, inclusion of parent meson velocity can account to a large difference for active-sterile mixing, specially for $D$, $D_s$ meson decay at SHiP and $K$ meson decay at NA62. Taking into account the velocity of the $D_s$ meson, the future beam dump experiment SHiP can probe $|V_{eN}|^2 \sim 10^{-9}$. For RH neutrino mass in between 2 - 5 GeV, MATHUSLA can provide best sensitivity reach of active-sterile mixings.

Highlights

  • The discovery of neutrino oscillations [1] in a series of oscillation experiments has confirmed that neutrinos have nonzero masses and nonzero mixings

  • We show that inclusion of parent meson velocity can account to a large difference for active-sterile mixing, especially for D, Ds meson decay at SHiP and K meson decay at NA62

  • We have shown the projected sensitivities in the mass-mixing plane for the heavy neutrinos produced from the W=Z decays (M-HL-Large Hadron Collider (LHC)-WZ) and B=D meson decays (M-HL-LHC-BD) for electron, muon and tau lepton at the HL-LHC in Figs. 11, 12 and 13, respectively

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Summary

INTRODUCTION

The discovery of neutrino oscillations [1] in a series of oscillation experiments has confirmed that neutrinos have nonzero masses and nonzero mixings. RH neutrinos have been searched for in the laboratory experiment through peak searches in leptonic decays of pions and kaons [49,50] Another interesting probe for Majorana neutrinos of hundreds of MeV–few GeV masses and their mixings are the lepton number violating (LNV) rare meson decay processes, such as M−1 → l−1 l−2 πþ [50,51,52,53,54,55,56,57,58,59,60,61,62,63,64,65,66]. In the Appendix, we provide details of the RH neutrino decay width calculations

THE MODEL
PROCESS
TOTAL DECAY WIDTH OF N
Þ2 þM2N
PARENT MESON VELOCITY AND FINITE DETECTOR SIZE EFFECT
SIGNAL EVENTS
INPUT FOR DIFFERENT EXPERIMENTS
MATHUSLA
Belle II
FCC-ee
VIII. RESULTS
COMBINED SENSITIVITY REACH FROM MESON DECAYS AND COMPARISON WITH
CONCLUSION
P ðxνl νlV0Þ
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