Abstract

The NA48/2 and NA62-$R_K$ experiments at the CERN SPS collected large samples of charged kaon decays in flight in 2003--07. The data analysis is still on-going (with over 20 publications produced so far); the recent results from these experiments are presented. A new upper limit on the rate of a lepton number violating decay $K^\pm\to\pi^\mp\mu^\pm\mu^\pm$ is reported: $\mathcal{B} < 8.6\times 10^{-11}$ at 90\% CL. Searches for heavy sterile neutrino $N_4$ and neutral scalar resonances ($\chi$) in $K^\pm\to\pi\mu\mu$ decays are reported. Upper limits on the products $\mathcal{B}(K^\pm\to\mu^\pm N_4)\mathcal{B}(N_4\to\pi^\mp\mu^\pm)$ and $\mathcal{B}(K^\pm\to\pi^\pm \chi)\mathcal{B}(\chi\to\mu^+\mu^-)$ are set in the range $10^{-10}$ to $10^{-9}$ for resonance lifetimes up to 100~ps. A preliminary measurement of the electromagnetic transition form factor slope of the $\pi^0$ from $1.05\times 10^6$ fully reconstructed $\pi^0\to\gamma e^+e^-$ decays is presented: the obtained result $a = (3.70 \pm 0.53_\text{stat} \pm 0.36_\text{syst})\times 10^{-2}$ represents the first observation of a non-zero slope in the time-like region of momentum transfer.

Highlights

  • The NA48/2 experiment at the CERN SPS collected a large sample of charged kaon decays in 2003– 04

  • The NA48/2 and NA62-RK experiments used simultaneous K+ and K− beams produced by 400 GeV/c primary CERN SPS protons impinging on a beryllium target

  • Searches for the Lepton number violation (LNV) K± → π∓μ±μ± decay and resonances in K± → πμμ decays using the 2003–04 data sample collected by the NA48/2 experiment at CERN are presented

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Summary

Introduction

The NA48/2 experiment at the CERN SPS collected a large sample of charged kaon decays in 2003– 04 (corresponding to about 2 × 1011 K± decays in the vacuum decay volume). Particle identification is performed using the ratio E/p of the energy deposit measured in the LKr calorimeter to the momentum reconstructed in the spectrometer, as well as the response of the downstream muon detector. In the LNV channel, a blind analysis is performed, with the selection optimized and the background simulation validated in the control mass region defined as Mπμμ < 480 MeV/c2, where Mπμμ is the reconstructed invariant mass of the pion and the two muons.

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