Abstract

The CKM matrix element ∣Vus∣|V_{us}| can be extracted from the experimental measurement of semileptonic K→πK\toπ decays. The determination depends on theory input for the corresponding vector form factor in QCD. We present a preliminary update on our efforts to compute it in Nf=2+1N_f=2+1 lattice QCD using domain wall fermions for several lattice spacings and with a lightest pion mass of about 170 MeV170\,\mathrm{MeV}. By using partially twisted boundary conditions we avoid systematic errors associated with an interpolation of the form factor in momentum-transfer, while simulated pion masses near the physical point reduce the systematic error due to the chiral extrapolation.

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