21–25 May 2007
Laboratori Nazionali di Frascati dell'INFN
Europe/Rome timezone

Measurement of the CP violation parameter $|\eta_{+-}|$ and the charge asymmetry in $K^\pm \to 3\pi$ decays by NA48 and NA48/2

22 May 2007, 12:20
20m
High Energy Building - Aula Bruno Touschek (Laboratori Nazionali di Frascati dell'INFN)

High Energy Building - Aula Bruno Touschek

Laboratori Nazionali di Frascati dell'INFN

Via E. Fermi, 40 00044 Frascati
Non leptonic/ radiative decays Session II

Speaker

Dr Andreas Winhart (Institut fuer Physik, Universitaet Mainz)

Description

The main goal of the NA48 experiment at the CERN SPS has been the search for direct CP violation (CPV) in kaon decays. The observable $\eta_{+-}$ is related to the parameters of indirect and direct CPV ($\eta_{+-} = \varepsilon + \varepsilon^\prime$) and defined as the CP violating amplitude ratio of the neutral kaon decaying into two charged pions: $\eta_{+-} = A(K_L \to \pi^+\pi^-)/A(K_S \to \pi^+\pi^-)$. NA48 has determined $|\eta_{+-}|$ via the measurement of the ratio of decay rates $\Gamma(K_L \to \pi^+\pi^-)/\Gamma(K_L \to \pi e \nu)$. The data were taken during a dedicated run in 1999 using a pure $K_L$ beam. The analysis is based on 47000 $K_L \to \pi^+\pi^-$ and five million $K_L \to \pi e \nu$ decays. Complementary with $\varepsilon^\prime/\varepsilon$, the observable in the charged kaons sector is the asymmetry $A_g = (g^+ - g^-)/(g^+ + g^-)$ of the linear slope parameter $g$ in the Dalitz plot of $K^\pm \to 3\pi$ decays. Any non-zero value of $A_g$ would reflect evidence for direct CPV. SM predictions for the charge asymmetry give an upper limit of a few $10^{-5}$, while theoretical calculations involving processes beyond the SM do not exclude substantial enhancements of $A_g$. The NA48/2 experiment used simultaneous $K^+/K^-$ beams, and from the data samples taken in 2003 and 2004, $3.11 \times 10^9 K^\pm \to \pi^\pm\pi^+\pi^-$ and $9.13 \times 10^7 K^\pm \to \pi^\pm\pi^0\pi^0$ were selected. The charge asymmetry parameter $A_g$ was determined with a total uncertainty of $\sim 2\times 10^{-4}$ for each mode, ten times more accurate than previous measurements.

Primary author

Dr Andreas Winhart (Institut fuer Physik, Universitaet Mainz)

Presentation materials