Abstract

We report on the first realistic \emph{ab initio} calculation of a hadronic weak decay, that of the amplitude A2A_2 for a kaon to decay into two π-mesons with isospin 2. We find ReA2=(1.436±0.063stat±0.258syst) 10−8 GeVA_2=(1.436\pm 0.063_{\textrm{stat}}\pm 0.258_{\textrm{syst}})\,10^{-8}\,\textrm{GeV} in good agreement with the experimental result and for the hitherto unknown imaginary part we find {Im} A2=−(6.83±0.51stat±1.30syst) 10−13 GeV\,A_2=-(6.83 \pm 0.51_{\textrm{stat}} \pm 1.30_{\textrm{syst}})\,10^{-13}\,{\rm GeV}. Moreover combining our result for Im\,A2A_2 with experimental values of Re\,A2A_2, Re\,A0A_0 and ε′/εε^\prime/ε, we obtain the following value for the unknown ratio Im\,A0A_0/Re\,A0A_0 within the Standard Model: Im A0/Re A0=−1.63(19)stat(20)syst×10−4\mathrm{Im}\,A_0/\mathrm{Re}\,A_0=-1.63(19)_{\mathrm{stat}}(20)_{\mathrm{syst}}\times10^{-4}. One consequence of these results is that the contribution from Im\,A2A_2 to the direct CP violation parameter ε′ε^{\prime} (the so-called Electroweak Penguin, EWP, contribution) is Re(ε′/ε)EWP=−(6.52±0.49stat±1.24syst)×10−4(ε^\prime/ε)_{\mathrm{EWP}} = -(6.52 \pm 0.49_{\textrm{stat}} \pm 1.24_{\textrm{syst}}) \times 10^{-4}. We explain why this calculation of A2A_2 represents a major milestone for lattice QCD and discuss the exciting prospects for a full quantitative understanding of CP-violation in kaon decays.

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