We report the results from a study of a partial sample of similar to 2.3 x 10(7) K+/- -> pi(+/-)pi(0)pi(0) decays recorded by the NA48/2 experiment at the CERN SPS, showing an anomaly in the pi(0)pi(0) invariant mass (M-00) distribution in the region around M-00 = 2m(+), where m(+) is the charged pion mass. This anomaly, never observed in previous experiments, can be interpreted as an effect due mainly to the final state charge exchange scattering process pi(+)pi(-) -> pi(0)pi(0) in K+/- -> pi(+/-)pi(+)pi(-) decay [N. Cabibbo, Phys. Rev. Lett. 93 (2004) 121801]. It provides a precise determination of a(0) - a(2), the difference between the pi pi scattering lengths in the isospin I = 0 and I = 2 states. A best fit to a rescattering model [N. Cabibbo, G. Isidori, JHEP 0503 (2005) 21] corrected for isospin symmetry breaking gives (a(0) - a(2))m(+) = 0.268 +/- 0.010(stat) +/- 0.004(syst), with additional external uncertainties of +/- 0.013 from branching ratio and theoretical uncertainties. If the correlation between a(0) and a2 predicted by chiral symmetry is taken into account, this result becomes (a(0) - a(2))m(+) = 0.264 +/- 0.006(stat) +/- 0.004(syst) +/- 0.013(ext). (c) 2005 Elsevier B.V. All rights reserved.

Observation of a cusp-like structure in the pi(0)pi(0) invariant mass distribution from K-+/-->pi(+/-)pi(0)pi(0) decay and determination of the pi pi scattering lengths

COSTANTINI, FLAVIO;GIUDICI, SERGIO;LAMANNA, GIANLUCA;SOZZI, MARCO STANISLAO;
2006-01-01

Abstract

We report the results from a study of a partial sample of similar to 2.3 x 10(7) K+/- -> pi(+/-)pi(0)pi(0) decays recorded by the NA48/2 experiment at the CERN SPS, showing an anomaly in the pi(0)pi(0) invariant mass (M-00) distribution in the region around M-00 = 2m(+), where m(+) is the charged pion mass. This anomaly, never observed in previous experiments, can be interpreted as an effect due mainly to the final state charge exchange scattering process pi(+)pi(-) -> pi(0)pi(0) in K+/- -> pi(+/-)pi(+)pi(-) decay [N. Cabibbo, Phys. Rev. Lett. 93 (2004) 121801]. It provides a precise determination of a(0) - a(2), the difference between the pi pi scattering lengths in the isospin I = 0 and I = 2 states. A best fit to a rescattering model [N. Cabibbo, G. Isidori, JHEP 0503 (2005) 21] corrected for isospin symmetry breaking gives (a(0) - a(2))m(+) = 0.268 +/- 0.010(stat) +/- 0.004(syst), with additional external uncertainties of +/- 0.013 from branching ratio and theoretical uncertainties. If the correlation between a(0) and a2 predicted by chiral symmetry is taken into account, this result becomes (a(0) - a(2))m(+) = 0.264 +/- 0.006(stat) +/- 0.004(syst) +/- 0.013(ext). (c) 2005 Elsevier B.V. All rights reserved.
2006
Batley, Jr; Lazzeroni, C; Munday, Dj; Slater, Mw; Wotton, Sa; Arcidiacono, R; Bocquet, G; Cabibbo, N; Ceccucci, A; Cundy, D; Falaleev, V; Fidecaro, M; Gatignon, L; Gonidec, A; Kubischta, W; Norton, A; Patel, M; Peters, A; Balev, S; Frabetti, Pl; Goudzovski, E; Hristov, P; Kekelidze, V; Kozhuharov, V; Litov, L; Madigozhin, D; Marinova, E; Molokanova, N; Polenkevich, I; Potrebenikov, Y; Stoynev, S; Zinchenko, A; Monnier, E; Swallow, E; Winston, R; Rubin, P; Walker, A; Baldini, W; Ramusino, Ac; Dalpiaz, P; Damiani, C; Fiorini, M; Gianoli, A; Martini, M; Petrucci, F; Savrie, M; Scarpa, M; Wahl, H; Bizzeti, A; Calvetti, M; Celeghini, E; Iacopini, E; Lenti, M; Martelli, F; Ruggiero, G; Veltri, M; Behler, M; Eppard, K; Kleinknecht, K; Marouelli, P; Masetti, L; Moosbrugger, U; Morales, Cm; Renk, B; Wache, M; Wanke, R; Winhart, A; Coward, D; Dabrowski, A; Martin, Tf; Shieh, M; Szleper, M; Velasco, M; Wood, Md; Anzivino, G; Cenci, P; Imbergamo, E; Pepe, A; Petrucci, Mc; Piccini, A; Raggi, M; Valdata Nappi, A; Cerri, C; Collazuol, G; Costantini, Flavio; Dilella, L; Doble, N; Fantechi, R; Fiorini, L; Giudici, Sergio; Lamanna, Gianluca; Mannelli, I; Michetti, A; Pierazzini, G; Sozzi, MARCO STANISLAO; Bloch Devaux, B; Cheshkov, C; Cheze, Jb; De Beer, M; Derre, J; Marel, G; Mazzucato, E; Peyaud, B; Vallage, B; Holder, M; Maier, A; Ziolkowski, M; Bifani, S; Biino, C; Cartiglia, N; Clemencic, M; Lopez, Sg; Marchetto, F; Dibon, H; Jeitler, M; Markytan, M; Mikulec, I; Neuhofer, G; Widhalm, L.
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11568/182055
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