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
Summary
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
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