The decay rate of K-L --> pi(o)gammagamma has been measured with the NA48 detector at the CERN SPS. A total of 2558 K-L --> pi(o)gammagamma candidates have been observed with a residual background of 3.2%. The branching ratio is determined to be (1.36 +/- 0.03((stat)) +/- 0.03((syst)) +/- 0.03((norm))) x 10(-6) and the vector coupling constant a(v) = -0.46 +/- 0.03((stat)) +/- 0.04((syst)). This result suggests that the CP-violation effects are dominating in the K-L --> pi(o)e(+)e(-) decay. An upper limit for the K-L --> pi(o)gammagamma decay rate in the two photon mass region m(gammagamma) < m(&pi;)o is also given. (C) 2002 Published by Elsevier Science B.V.

Precise measurement of the decay K-L ->pi(0)gamma gamma

COSTANTINI, FLAVIO;GIUDICI, SERGIO;SOZZI, MARCO STANISLAO;
2002-01-01

Abstract

The decay rate of K-L --> pi(o)gammagamma has been measured with the NA48 detector at the CERN SPS. A total of 2558 K-L --> pi(o)gammagamma candidates have been observed with a residual background of 3.2%. The branching ratio is determined to be (1.36 +/- 0.03((stat)) +/- 0.03((syst)) +/- 0.03((norm))) x 10(-6) and the vector coupling constant a(v) = -0.46 +/- 0.03((stat)) +/- 0.04((syst)). This result suggests that the CP-violation effects are dominating in the K-L --> pi(o)e(+)e(-) decay. An upper limit for the K-L --> pi(o)gammagamma decay rate in the two photon mass region m(gammagamma) < m(π)o is also given. (C) 2002 Published by Elsevier Science B.V.
2002
Lai, A; Marras, D; Bevan, A; Dosanjh, Rs; Gershon, Tj; Hay, B; Kalmus, Ge; Lazzeroni, C; Munday, Dj; Needham, Md; 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; Lenti, M; Luitz, S; Mikulec, I; Norton, A; Palestini, S; Panzer Steindel, B; Tatishvili, G; Taureg, H; Velasco, M; Wahl, H; Cheshkov, C; Hristov, P; Kekelidze, V; Madigojine, D; Molokanova, N; Potrebenikov, Y; 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; Veltri, M; Becker, Hg; Eppard, M; Fox, H; Holtz, K; Kalter, A; Kleinknecht, K; Koch, U; Kopke, L; da Silva, Pl; Maruelli, 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, M; Piccini, M; Carosi, R; Casali, 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; Clemencic, M; Marchetto, F; Menichetti, E; Pastrone, N; Nassalski, J; Rondio, E; Szleper, M; Wislicki, W; Wronka, S; Dibon, H; Fischer, G; Jeitler, M; Markytan, M; 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/11568/178351
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