Determination of the branching ratios $\Gamma (K_L \to 3 \pi^0) / \Gamma (K_L \to \pi^+ \pi^- \pi^0)$ and $\Gamma (K_L \to 3 \pi^0) / \Gamma (K_L \to \pi e \nu )$
/ Authors
A. Kreutz, M. Holder, M. Rost, R. Werthenbach, K.J.Peach, H.Blumer, R.Heinz, K.Kleinknecht, P.Mayer, B.Panzer
and 20 more authors
B.Renk, H.Rohrer, A.Wagner, E.Aug'e, D.Fournier, L.Iconomidou-Fayard, O.Perdereau, A.C.Schaffer, L.Serin, L.Bertanza, A.Bigi, P.Calafiura, M.Calvetti, R.Carosi, R.Casali, C.Cerri, I.Mannelli, V.Marzulli, A.Nappi, G.M.Pierazzini
/ Abstract
Improved branching ratios were measured for the $K_L \to 3 \pi^0 $ decay in a neutral beam at the CERN SPS with the NA31 detector: $\Gamma (K_L \to 3 \pi^0) / \Gamma (K_L \to \pi^+ \pi^- \pi^0) = 1.611 \pm 0.037$ and $\Gamma (K_L \to 3 \pi^0) / \Gamma (K_L \to \pi e \nu ) = 0.545 \pm 0.010$. From the first number an upper limit for $\Delta I =5/2$ and $\Delta I = 7/2 $ transitions in neutral kaon decay is derived. Using older results for the Ke3/K$\mu $3 fraction, the 3$\pi^0$ branching ratio is found to be $\Gamma (K_L \to 3 \pi^0 )/ \Gamma_{tot} = (0.211 \pm 0.003)$, about a factor three more precise than from previous experiments.
Journal: arXiv: High Energy Physics - Experiment
DOI: 10.1007/BF01571304