TY - JOUR
T1 - Kaon semileptonic vector form factor and determination of |Vus| using staggered fermions
AU - Bazavov, A.
AU - Bernard, C.
AU - Bouchard, C. M.
AU - Detar, C.
AU - Du, Daping
AU - El-Khadra, A. X.
AU - Foley, J.
AU - Freeland, E. D.
AU - Gámiz, E.
AU - Gottlieb, Steven
AU - Heller, U. M.
AU - Kim, Jongjeong
AU - Kronfeld, A. S.
AU - Laiho, J.
AU - Levkova, L.
AU - Mackenzie, P. B.
AU - Neil, E. T.
AU - Oktay, M. B.
AU - Qiu, Si Wei
AU - Simone, J. N.
AU - Sugar, R.
AU - Toussaint, D.
AU - Van De Water, R. S.
AU - Zhou, Ran
PY - 2013/4/23
Y1 - 2013/4/23
N2 - Using staggered fermions and partially twisted boundary conditions, we calculate the K meson semileptonic decay vector form factor at zero momentum transfer. The highly improved staggered quark formulation is used for the valence quarks, while the sea quarks are simulated with the asqtad action (MILC Collaboration Nf=2+1 configurations). For the chiral and continuum extrapolation, we use two-loop continuum χPT, supplemented by partially quenched staggered χPT at one loop. Our result is f+Kπ(0)=0. 9667±0.0023±0.0033, where the first error is statistical and the second is the sum in quadrature of the systematic uncertainties. This result is the first Nf=2+1 calculation with two lattice spacings and a controlled continuum extrapolation. It is also the most precise result to date for the vector form factor, and, although the central value is larger than previous unquenched lattice calculations, it is compatible with them within errors. Combining our value for f+Kπ(0) with the latest experimental measurements of K semileptonic decays, we obtain |Vus|=0. 2238±0.0009±0.0005, where the first error is from f+Kπ(0) and the second one is experimental. As a byproduct of our calculation, we obtain the combination of low-energy constants (C12r+C34r-(L5r) 2)(Mρ)=(3. 62±1.00)×10-6.
AB - Using staggered fermions and partially twisted boundary conditions, we calculate the K meson semileptonic decay vector form factor at zero momentum transfer. The highly improved staggered quark formulation is used for the valence quarks, while the sea quarks are simulated with the asqtad action (MILC Collaboration Nf=2+1 configurations). For the chiral and continuum extrapolation, we use two-loop continuum χPT, supplemented by partially quenched staggered χPT at one loop. Our result is f+Kπ(0)=0. 9667±0.0023±0.0033, where the first error is statistical and the second is the sum in quadrature of the systematic uncertainties. This result is the first Nf=2+1 calculation with two lattice spacings and a controlled continuum extrapolation. It is also the most precise result to date for the vector form factor, and, although the central value is larger than previous unquenched lattice calculations, it is compatible with them within errors. Combining our value for f+Kπ(0) with the latest experimental measurements of K semileptonic decays, we obtain |Vus|=0. 2238±0.0009±0.0005, where the first error is from f+Kπ(0) and the second one is experimental. As a byproduct of our calculation, we obtain the combination of low-energy constants (C12r+C34r-(L5r) 2)(Mρ)=(3. 62±1.00)×10-6.
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U2 - 10.1103/PhysRevD.87.073012
DO - 10.1103/PhysRevD.87.073012
M3 - Article
AN - SCOPUS:84877152692
SN - 1550-7998
VL - 87
JO - Physical Review D - Particles, Fields, Gravitation and Cosmology
JF - Physical Review D - Particles, Fields, Gravitation and Cosmology
IS - 7
M1 - 073012
ER -