Abstract

We present new results for the amplitude A2A_2 for a kaon to decay into two pions with isospin I=2I=2: ReA2=1.50(4)stat(14)syst×10−8A_2 = 1.50(4)_\mathrm{stat}(14)_\mathrm{syst}\times 10^{-8} GeV; ImA2=−6.99(20)stat(84)syst×10−13A_2 = -6.99(20)_\mathrm{stat}(84)_\mathrm{syst}\times 10^{-13} GeV. These results were obtained from two ensembles generated at physical quark masses (in the isospin limit) with inverse lattice spacings a−1=1.728(4)a^{-1}=1.728(4) GeV and 2.358(7)2.358(7) GeV. We are therefore able to perform a continuum extrapolation and hence largely to remove the dominant systematic uncertainty from our earlier results, that due to lattice artefacts. The only previous lattice computation of K→ππK\toππ decays at physical kinematics was performed using an ensemble at a single, rather coarse, value of the lattice spacing (a−1≃1.37(1)a^{-1}\simeq 1.37(1) GeV). We confirm the observation that there is a significant cancellation between the two dominant contributions to ReA2A_2 which we suggest is an important ingredient in understanding the ΔI=1/2ΔI=1/2 rule, ReA0A_0/ReA2≃22.5A_2\simeq 22.5, where the subscript denotes the total isospin of the two-pion final state. Our result for A2A_2 implies that the electroweak penguin contribution to ε′/εε^\prime/ε is Re(ε′/ε)EWP=−(6.6±1.0)×10−4ε^\prime/ε)_\textrm{EWP}=-(6.6\pm 1.0)\times 10^{-4}.

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