Abstract

Using the data sample of an integrated luminosity of 2.93 fb$^{-1}$ taken at the center-of-mass energy of 3.773 GeV, we search for the Majorana neutrino in the lepton number violating decays $D\to K \pi e^+ e^+$. No significant signal is observed, and the upper limits on the branching fraction at the 90\% confidence level are set to be $\mathcal{B}\,(D^0 \to K^- \pi^- e^+ e^+)<2.8\times10^{-6}$, $\mathcal{B}\,(D^+ \to K_S^0 \pi^- e^+ e^+)<3.3\times10^{-6}$ and $\mathcal{B}\,(D^+ \to K^- \pi^0 e^+ e^+)<8.5\times10^{-6}$. The Majorana neutrino is searched for with different mass assumptions ranging from 0.25 to 1.0 GeV/$c^2$ in the decays $D^0\to K^- e^+ \nu_N(\pi^- e^+)$ and $D^+\to K_S^0 e^+ \nu_N(\pi^- e^+)$, and the upper limits on the branching fraction at the 90\% confidence level are extracted to be at the level of $10^{-7} \sim 10^{-6}$, depending on the mass of Majorana neutrino. The constraints on the mixing matrix element $|V_{eN}|^2$ are also evaluated.

Highlights

  • In the Standard Model (SM), due to the absence of a right-handed neutrino component and the requirements of SUð2ÞL gauge invariance and renormalizability, neutrinos are postulated to be massless

  • the observations of neutrino oscillation have shown that neutrinos have a tiny mass

  • which provides the first evidence for physics beyond the SM

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Summary

INTRODUCTION

In the Standard Model (SM), due to the absence of a right-handed neutrino component and the requirements of SUð2ÞL gauge invariance and renormalizability, neutrinos are postulated to be massless. An interesting source of LNV processes is given by exchanging a single Majorana neutrino with a mass on the order of the heavy flavor mass scale, where the Majorana neutrino can be kinematically accessible and produced on shell The effects of such a heavy neutrino with mass in the range 100 MeV=c2 to a few GeV=c2 have been widely searched for in ΔL 1⁄4 2 three-body and fourbody decays of heavy flavor mesons and in τ lepton decays by different experiments, as summarized in Ref. We present the studies of LNV processes with ΔL 1⁄4 2 in D meson decays D0 → K−π−eþeþ, Dþ → K0Sπ−eþeþ and Dþ → K−π0eþeþ Throughout the paper, the charged conjugated modes are always implied implicitly

DETECTOR AND MONTE CARLO SIMULATION
EVENT SELECTION
SIGNAL DETERMINATION
SYSTEMATIC UNCERTAINTIES
RESULTS AND DISCUSSION
Searching for Majorana neutrino
SUMMARY

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