Measured ratios of decay rates for R_{K e 3 / K2pi}, R_{K mu3 / K2pi} and R_{K mu3 / Ke3} are presented. These measurements are based on K± decays collected in a dedicated run in 2003 by the NA48/2 experiment at CERN. The results obtained are R_{K e 3 / K2pi} = (0.2496 +- 0.0009 stat +- 0.0004 syst) and R_{K mu3 / K2pi} = (0.1637 +- 0.0006 stat +- 0.0003 syst). Using the PDG average for the K± --> π±π0 normalisation mode, both values are found to be larger than the current values given by the particle data book and lead to a larger magnitude of the |Vus| CKM element than previously accepted. When combined with the latest particle data book value of |Vud|, the result is in agreement with unitarity of the CKM matrix. In addition, a new measured value of R_{K mu3 / Ke3} = (0.656 +- 0.003 stat +- 0.001 syst) is compared to the semi-empirical predictions based on the latest form factor measurements.

Measurements of charged kaon semileptonic decay branching fractions K(+/-) --> pi(0)mu(+/-)v and K(+/-) --> pi(0)e(+/-)v and their ratio

BALDINI, Wander;COTTA RAMUSINO, Angelo;DALPIAZ, Pietro;DAMIANI, Chiara;FIORINI, Massimiliano;GIANOLI, Alberto;MARTINI, Mara;PETRUCCI, Ferruccio Carlo;SAVRIE', Mauro;SCARPA, MARCELLA;
2007

Abstract

Measured ratios of decay rates for R_{K e 3 / K2pi}, R_{K mu3 / K2pi} and R_{K mu3 / Ke3} are presented. These measurements are based on K± decays collected in a dedicated run in 2003 by the NA48/2 experiment at CERN. The results obtained are R_{K e 3 / K2pi} = (0.2496 +- 0.0009 stat +- 0.0004 syst) and R_{K mu3 / K2pi} = (0.1637 +- 0.0006 stat +- 0.0003 syst). Using the PDG average for the K± --> π±π0 normalisation mode, both values are found to be larger than the current values given by the particle data book and lead to a larger magnitude of the |Vus| CKM element than previously accepted. When combined with the latest particle data book value of |Vud|, the result is in agreement with unitarity of the CKM matrix. In addition, a new measured value of R_{K mu3 / Ke3} = (0.656 +- 0.003 stat +- 0.001 syst) is compared to the semi-empirical predictions based on the latest form factor measurements.
2007
J. R., Batley; A. J., Culling; G., Kalmus; C., Lazzeroni; D. J., Munday; M. W., Slater; S. A., Wotton; R., Arcidiacono; G., Bocquet; N., Cabibbo; A., Ceccucci; D., Cundy; V., Falaleev; M., Fidecaro; L., Gatignon; A., Gonidec; W., Kubischta; A., Norton; A., Maier; M., Patel; A., Peters; S., Balev; P. L., Frabetti; E., Goudzovski; P., Hristov; V., Kekelidze; V., Kozhuharov; L., Litov; D., Madigozhin; E., Marinova; N., Molokanova; I., Polenkevich; Y., Potrebenikov; S., Stoynev; A., Zinchenko; E., Monnier; E., Swallow; R., Winston; P., Rubin; A., Walker; Baldini, Wander; COTTA RAMUSINO, Angelo; Dalpiaz, Pietro; Damiani, Chiara; Fiorini, Massimiliano; Gianoli, Alberto; Martini, Mara; Petrucci, Ferruccio Carlo; Savrie', Mauro; Scarpa, Marcella; H., Wahl; A., Bizzeti; M., Calvetti; E., Celeghini; E., Iacopini; M., Lenti; F., Martelli; G., Ruggiero; M., Veltri; M., Behler; K., Eppard; K., Kleinknecht; P., Marouelli; L., Masetti; U., Moosbrugger; C., Morales Morales; B., Renk; M., Wache; R., Wanke; A., Winhart; D., Coward; A., Dabrowski; T., Fonseca Martin; M., Shieh; M., Szleper; M., Velasco; M. D., Wood; G., Anzivino; P., Cenci; E., Imbergamo; A., Nappi; M., Pepe; M. C., Petrucci; M., Piccini; M., Raggi; M., Valdata Nappi; C., Cerri; G., Collazuol; F., Costantini; L., Dilella; N., Doble; R., Fantechi; L., Fiorini; S., Giudici; G., Lamanna; I., Mannelli; A., Michetti; G., Pierazzini; M., Sozzi; B., Bloch Devaux; C., Cheshkov; J. B., Chèze; M., De Beer; J., Derré; G., Marel; E., Mazzucato; B., Peyaud; B., Vallage; M., Holder; M., Ziolkowski; S., Bifani; C., Biino; N., Cartiglia; M., Clemencic; S., Goy Lopez; F., Marchetto; H., Dibon; M., Jeitler; M., Markytan; I., Mikulec; G., Neuhofer; L., Widhalm
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11392/521629
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