We present a measurement of the ratio of the decay rates Gamma(K-L -> pi(+)pi(-))/Gamma(K-L -> pi +/- e -/+nu), denoted as Gamma(K2 pi)/Gamma(Ke3). The analysis is based on data taken during a dedicated run in 1999 by the NA48 experiment at the CERN SPS. Using a sample of 47 000 K-2 pi and five million K-e3 decays, we find Gamma(K2 pi)/Gamma(Ke3) = (4.835 +/- 0.022stat. +/- 0.016syst.) x 10(-3). From this we derive the branching ratio of the CP violating decay K-L -> pi(+)pi(-) and the CP violation parameter vertical bar eta+-vertical bar. Excluding the CP conserving direct photon emission component K-L -> pi(+)pi(-)gamma, we obtain the results BR(K-L -> pi(+)pi(-)) = (1.941 +/- 0.019) x 10(-3) and vertical bar eta+-vertical bar = (2.223 +/- 0.012) x 10(-3). (c) 2006 Elsevier B.V. All rights reserved.

Measurement of the ratio Gamma(K-L -> pi(+)pi(-))/Gamma(K-L -> pi(+/-)e(-/+)nu) and extraction of the CP violation parameter vertical bar eta(+-)vertical bar

COSTANTINI, FLAVIO;GIUDICI, SERGIO;SOZZI, MARCO STANISLAO;
2007-01-01

Abstract

We present a measurement of the ratio of the decay rates Gamma(K-L -> pi(+)pi(-))/Gamma(K-L -> pi +/- e -/+nu), denoted as Gamma(K2 pi)/Gamma(Ke3). The analysis is based on data taken during a dedicated run in 1999 by the NA48 experiment at the CERN SPS. Using a sample of 47 000 K-2 pi and five million K-e3 decays, we find Gamma(K2 pi)/Gamma(Ke3) = (4.835 +/- 0.022stat. +/- 0.016syst.) x 10(-3). From this we derive the branching ratio of the CP violating decay K-L -> pi(+)pi(-) and the CP violation parameter vertical bar eta+-vertical bar. Excluding the CP conserving direct photon emission component K-L -> pi(+)pi(-)gamma, we obtain the results BR(K-L -> pi(+)pi(-)) = (1.941 +/- 0.019) x 10(-3) and vertical bar eta+-vertical bar = (2.223 +/- 0.012) x 10(-3). (c) 2006 Elsevier B.V. All rights reserved.
2007
Lai, A; Marras, D; Bevan, A; Dosanjh, Rs; Gershon, Tj; Hay, B; Kalmus, Ge; Lazzeroni, C; Munday, Dj; Olaiya, E; Parker, Ma; White, To; Wotton, Sa; Barr, G; Bocquet, G; Ceccucci, A; Cuhadar Donszelmann, T; Cundy, D; D'Agostini, G; Doble, N; Falaleev, V; Gatignon, L; Gonidec, A; Gorini, B; Govi, G; Grafstrom, P; Kubischta, W; Lacourt, A; Norton, A; Palestini, S; Panzer Steindel, B; Taureg, H; Velasco, M; Wahl, H; Cheshkov, C; Gaponenko, A; Hristov, P; Kekelidze, V; Litov, L; Madigozhin, D; Molokanova, N; Potrebenikov, Y; Stoynev, S; Tatishvili, G; Tkatchev, A; Zinchenko, A; Knowles, I; Martin, V; Sacco, R; Walker, A; Contalbrigo, M; Dalpiaz, P; Duclos, J; Frabetti, Pl; Gianoli, A; Martini, M; Petrucci, F; Savrie, M; Bizzeti, A; Calvetti, M; Collazuol, G; Graziani, G; Iacopini, E; Lenti, M; Martelli, F; Veltri, M; Becker, Hg; Eppard, K; Eppard, M; Fox, H; Kalter, A; Kleinknecht, K; Koch, U; Kopke, L; da Silva, Pl; Marouelli, P; Pellmann, I; Peters, A; Renk, B; Schmidt, Sa; Schonharting, V; Schue, Y; Wanke, R; Winhart, A; Wittgen, M; Chollet, Jc; Fayard, L; Iconomidou Fayard, L; Ocariz, J; Unal, G; Wingerter Seez, I; Anzivino, G; Cenci, P; Imbergamo, E; Lubrano, P; Mestvirishvili, A; Nappi, A; Pepe, A; Piccini, M; Bertanza, L; Carosi, R; Cerri, C; Cirilli, M; Costantini, Flavio; Fantechi, R; Giudici, Sergio; Mannelli, I; Pierazzini, G; Sozzi, MARCO STANISLAO; Cheze, Jb; Cogan, J; De Beer, M; Debu, P; Formica, A; de Cassagnac, Rg; Mazzucato, E; Peyaud, B; Turlay, R; Vallage, B; Holder, M; Maier, A; Ziolkowski, M; Arcidiacono, R; Biino, C; Cartiglia, N; Guida, R; Marchetto, F; Menichetti, E; Pastrone, N; Nassalski, J; Rondio, E; Szleper, M; Wislicki, W; Wronka, S; Dibon, H; Fischer, G; Jeitler, M; Markytan, M; Mikulec, I; Neuhofer, G; Pernicka, M; Taurok, A; Widhalm, L.
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11568/182069
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