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Determination of the branching ratios $\Gamma(K_{L} \to 3\pi^{0}) / \Gamma(K_{L} \to \pi^{+}\pi^{-}\pi^{0})$ and $\Gamma(K_{L} \to 3\pi^{0}) / \Gamma(K_{L} \to \pi e\nu)$
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 t...
Autores principales: | , , , , , , , , , , , , , , , , , , , , , , , , , , , , , |
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Lenguaje: | eng |
Publicado: |
1994
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Acceso en línea: | https://dx.doi.org/10.1007/BF01571304 http://cds.cern.ch/record/270327 |
_version_ | 1780887060129775616 |
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author | Kreutz, A. Holder, M. Rost, M. Werthenbach, R. Peach, K.J. Blumer, H. Heinz, R. Kleinknecht, K. Mayer, P. Panzer, B. Renk, B. Rohrer, H. Wagner, A. Auge, E. Fournier, D. Iconomidou-Fayard, L. Perdereau, O. Schaffer, A.C. Serin, L. Bertanza, L. Bigi, A. Calafiura, P. Calvetti, M. Carosi, R. Casali, R. Cerri, C. Mannelli, I. Marzulli, V. Nappi, A. Pierazzini, G.M. |
author_facet | Kreutz, A. Holder, M. Rost, M. Werthenbach, R. Peach, K.J. Blumer, H. Heinz, R. Kleinknecht, K. Mayer, P. Panzer, B. Renk, B. Rohrer, H. Wagner, A. Auge, E. Fournier, D. Iconomidou-Fayard, L. Perdereau, O. Schaffer, A.C. Serin, L. Bertanza, L. Bigi, A. Calafiura, P. Calvetti, M. Carosi, R. Casali, R. Cerri, C. Mannelli, I. Marzulli, V. Nappi, A. Pierazzini, G.M. |
author_sort | Kreutz, A. |
collection | CERN |
description | 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.\\[1ex] |
id | cern-270327 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 1994 |
record_format | invenio |
spelling | cern-2703272019-09-30T06:29:59Zdoi:10.1007/BF01571304http://cds.cern.ch/record/270327engKreutz, A.Holder, M.Rost, M.Werthenbach, R.Peach, K.J.Blumer, H.Heinz, R.Kleinknecht, K.Mayer, P.Panzer, B.Renk, B.Rohrer, H.Wagner, A.Auge, E.Fournier, D.Iconomidou-Fayard, L.Perdereau, O.Schaffer, A.C.Serin, L.Bertanza, L.Bigi, A.Calafiura, P.Calvetti, M.Carosi, R.Casali, R.Cerri, C.Mannelli, I.Marzulli, V.Nappi, A.Pierazzini, G.M.Determination of the branching ratios $\Gamma(K_{L} \to 3\pi^{0}) / \Gamma(K_{L} \to \pi^{+}\pi^{-}\pi^{0})$ and $\Gamma(K_{L} \to 3\pi^{0}) / \Gamma(K_{L} \to \pi e\nu)$Particle Physics - ExperimentImproved 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.\\[1ex]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.hep-ex/9409003SI-94-05oai:cds.cern.ch:2703271994-09-21 |
spellingShingle | Particle Physics - Experiment Kreutz, A. Holder, M. Rost, M. Werthenbach, R. Peach, K.J. Blumer, H. Heinz, R. Kleinknecht, K. Mayer, P. Panzer, B. Renk, B. Rohrer, H. Wagner, A. Auge, E. Fournier, D. Iconomidou-Fayard, L. Perdereau, O. Schaffer, A.C. Serin, L. Bertanza, L. Bigi, A. Calafiura, P. Calvetti, M. Carosi, R. Casali, R. Cerri, C. Mannelli, I. Marzulli, V. Nappi, A. Pierazzini, G.M. Determination of the branching ratios $\Gamma(K_{L} \to 3\pi^{0}) / \Gamma(K_{L} \to \pi^{+}\pi^{-}\pi^{0})$ and $\Gamma(K_{L} \to 3\pi^{0}) / \Gamma(K_{L} \to \pi e\nu)$ |
title | Determination of the branching ratios $\Gamma(K_{L} \to 3\pi^{0}) / \Gamma(K_{L} \to \pi^{+}\pi^{-}\pi^{0})$ and $\Gamma(K_{L} \to 3\pi^{0}) / \Gamma(K_{L} \to \pi e\nu)$ |
title_full | Determination of the branching ratios $\Gamma(K_{L} \to 3\pi^{0}) / \Gamma(K_{L} \to \pi^{+}\pi^{-}\pi^{0})$ and $\Gamma(K_{L} \to 3\pi^{0}) / \Gamma(K_{L} \to \pi e\nu)$ |
title_fullStr | Determination of the branching ratios $\Gamma(K_{L} \to 3\pi^{0}) / \Gamma(K_{L} \to \pi^{+}\pi^{-}\pi^{0})$ and $\Gamma(K_{L} \to 3\pi^{0}) / \Gamma(K_{L} \to \pi e\nu)$ |
title_full_unstemmed | Determination of the branching ratios $\Gamma(K_{L} \to 3\pi^{0}) / \Gamma(K_{L} \to \pi^{+}\pi^{-}\pi^{0})$ and $\Gamma(K_{L} \to 3\pi^{0}) / \Gamma(K_{L} \to \pi e\nu)$ |
title_short | Determination of the branching ratios $\Gamma(K_{L} \to 3\pi^{0}) / \Gamma(K_{L} \to \pi^{+}\pi^{-}\pi^{0})$ and $\Gamma(K_{L} \to 3\pi^{0}) / \Gamma(K_{L} \to \pi e\nu)$ |
title_sort | determination of the branching ratios $\gamma(k_{l} \to 3\pi^{0}) / \gamma(k_{l} \to \pi^{+}\pi^{-}\pi^{0})$ and $\gamma(k_{l} \to 3\pi^{0}) / \gamma(k_{l} \to \pi e\nu)$ |
topic | Particle Physics - Experiment |
url | https://dx.doi.org/10.1007/BF01571304 http://cds.cern.ch/record/270327 |
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