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2011 QCD and High Energy Interactions - Rencontres de Moriond ...

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STUDY OF Ke4 DECAYS IN THE NA48/2 EXPERIMENT AT CERN<br />

B. BLOCH-DEVAUX<br />

Department of Physics, Università <strong>de</strong>gli Studi di Torino,<br />

via P.Giuria 1, 10125 Torino, Italy<br />

Large samples of kaon <strong>de</strong>cays have been collected in 2003 − 2004 by the NA48/2 collaboration<br />

in the charged (K ± → π + π − e ± ν) <strong>and</strong> neutral (K ± → π 0 π 0 e ± ν) Ke4 mo<strong>de</strong>s. In the charged<br />

mo<strong>de</strong>, form factors have been extensively studied from a sample of more than one million<br />

<strong>de</strong>cays <strong>and</strong> a preliminary branching ratio measurement is reported here. In the neutral mo<strong>de</strong>,<br />

a sample of 44 000 <strong>de</strong>cays has been analyzed <strong>and</strong> provi<strong>de</strong>s a new branching ratio value with<br />

1 − 2% precision, a factor of ten improvement with respect to the current knowledge. Both<br />

mo<strong>de</strong>s contribute to the study of low energy <strong>QCD</strong> <strong>and</strong> are powerful tests of Chiral Perturbation<br />

Theory predictions.<br />

1 Introduction<br />

Kaon <strong>de</strong>cays have been i<strong>de</strong>ntified as a perfect laboratory to study low energy strong interaction.<br />

Semileptonic four-body <strong>de</strong>cays are of particular interest because of the small number of hadrons<br />

in the final state which are related to the study of ππ interaction. The <strong>de</strong>velopment of chiral<br />

perturbation theory (ChPT) 1 over more than 30 years has reached a competitive precision level<br />

in its predictions of both ππ scattering lengths values <strong>and</strong> form factors appearing in the weak<br />

hadronic current of the Ke4 <strong>de</strong>cay matrix element. The global analysis of ππ, πK <strong>and</strong> Ke4 data<br />

allows the <strong>de</strong>termination of the Low <strong>Energy</strong> Constants (LEC) of ChPT at Leading <strong>and</strong> Next<br />

to Leading Or<strong>de</strong>rs (LO,NLO,NNLO) 2,3 <strong>and</strong> subsequent predictions of form factors <strong>and</strong> <strong>de</strong>cay<br />

rates. Current experimental measurements 4 <strong>and</strong> NA48/2 improved sensitivity are shown in<br />

Table 1. The possibility to study high statistics samples collected concurrently by NA48/2 in<br />

several mo<strong>de</strong>s will bring improved inputs <strong>and</strong> will allow stronger tests of ChPT predictions.<br />

Table 1: Number of analyzed Ke4 events, measured <strong>de</strong>cay rates <strong>and</strong> NA48/2 improvements for the two reported<br />

mo<strong>de</strong>s. Relative errors are given within parentheses.<br />

2 Kinematics<br />

Decay mo<strong>de</strong> PDG 2010 This measurement<br />

K + → π + π − e + νe 418 000 3304 ± 81 (2.4%) 1.11 10 6 28 (0.8%)<br />

K + → π 0 π 0 e + νe 37 1777 ± 323 (18.2%) 44 000 34 (1.6%)<br />

The Ke4 <strong>de</strong>cay is fully <strong>de</strong>scribed by the five kinematic Cabibbo-Maksymowicz variables 7 : two<br />

invariant masses Sπ = M 2 ππ <strong>and</strong> Se = M 2 eν <strong>and</strong> three angles θπ, θe <strong>and</strong> φ. Form factors can be <strong>de</strong>veloped<br />

in a partial wave expansion 8 . Limiting the expansion to S- <strong>and</strong> P- wave <strong>and</strong> consi<strong>de</strong>ring

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