The KS→π+π−e+e− decay mode was investigated using the data collected in 2002 by the NA48/1 Collaboration. With about 23 k KS→π+π−e+e− events and 59 k normalization decays, the KS→π+π−e+e− branching ratio relative to the one was determined to be . This result was used to set the upper limit |gE1/gBR|<3.0 at 90% CL on the presence, in the decay amplitude, of an E1 direct emission (gE1) term relative to the dominant inner bremsstrahlung (gBR) term. The CP-violating asymmetry in the distribution of KS→π+π−e+e− events, where is the angle between the π+π− and the e+e− decay planes in the kaon centre of mass, was found to be , consistent with zero. These results are in good agreement with a description of the KS→π+π−e+e− decay amplitude dominated by the CP-even inner bremsstrahlung process.

Precision measurement of the ratio BR(KS → π+π-e+e-/ BR(KL →π+π-π0(D))

BALDINI, Wander;DALPIAZ, Pietro;GIANOLI, Alberto;PETRUCCI, Ferruccio Carlo;SAVRIE', Mauro;
2011

Abstract

The KS→π+π−e+e− decay mode was investigated using the data collected in 2002 by the NA48/1 Collaboration. With about 23 k KS→π+π−e+e− events and 59 k normalization decays, the KS→π+π−e+e− branching ratio relative to the one was determined to be . This result was used to set the upper limit |gE1/gBR|<3.0 at 90% CL on the presence, in the decay amplitude, of an E1 direct emission (gE1) term relative to the dominant inner bremsstrahlung (gBR) term. The CP-violating asymmetry in the distribution of KS→π+π−e+e− events, where is the angle between the π+π− and the e+e− decay planes in the kaon centre of mass, was found to be , consistent with zero. These results are in good agreement with a description of the KS→π+π−e+e− decay amplitude dominated by the CP-even inner bremsstrahlung process.
2011
J. R., Batley; G., Kalmus; C., Lazzeroni; D. J., Munday; M., Patel; M. W., Slater; S. A., Wotton; R., Arcidiacono; G., Bocquet; A., Ceccucci; D., Cundy; N., Doble; V., Falaleev; L., Gatignon; A., Gonidec; P., Grafström; W., Kubischta; I., Mikulec; A., Norton; B., Panzer Steindel; P., Rubin; E., Goudzovski; P., Hristov; V., Kekelidze; L., Litov; D., Madigozhin; N., Molokanova; Y., Potrebenikov; S., Stoynev; A., Zinchenko; E., Monnier; E., Swallow; R., Winston; R., Sacco; A., Walker; Baldini, Wander; Dalpiaz, Pietro; P. L., Frabetti; Gianoli, Alberto; M., Martini; Petrucci, Ferruccio Carlo; Savrie', Mauro; M., Scarpa; H., Wahl; A., Bizzeti; M., Calvetti; G., Collazuol; E., Iacopini; M., Lenti; G., Ruggiero; M., Veltri; M., Behler; K., Eppard; M., Eppard; A., Hirstius; K., Kleinknecht; U., Koch; P., Marouelli; L., Masetti; U., Moosbrugger; C., Morales Morales; R., Wanke; A., Winhart; A., Dabrowski; T., Fonseca Martin; M., Velasco; G., Anzivino; P., Cenci; E., Imbergamo; P., Lubrano; A., Nappi; M., Pepe; M. C., Petrucci; M., Piccini; M., Valdata Nappi; C., Cerri; F., Costantini; R., Fantechi; L., Fiorini; S., Giudici; G., Lamanna; I., Mannelli; A., Michetti; G., Pierazzini; M., Sozzi; C., Cheshkov; J. B., Chèze; M., De Beer; P., Debu; J., Derré; G., Gouge; G., Marel; E., Mazzucato; B., Peyaud; B., Vallage; M., Holder; A., Maier; M., Ziolkowski; C., Biino; N., Cartiglia; M., Clemencic; S., Goy Lopez; F., Marchetto; E., Menichetti; N., Pastrone; W., Wislicki; H., Dibon; M., Jeitler; M., Markytan; G., Neuhofer; L., Widhalm
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11392/1653480
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