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Continuum limit of B_{K} from 2+1 flavor domain wall QCD

Aoki, Y., Arthur, R., Blum, T., Boyle, P., Brömmel, D., Christ, N., Dawson, C., Izubuchi, T., Jung, C., Kelly, C., Kenway, R., Lightman, M., Mawhinney, R., Ohta, Shigemi, Sachrajda, C., Scholz, E., Soni, A., Sturm, C., Wennekers, J. and Zhou, R. (2011) Continuum limit of B_{K} from 2+1 flavor domain wall QCD Physical Review D, 84, (1), 014503-1-014503-32. (doi:10.1103/PhysRevD.84.014503).

Record type: Article

Abstract

We determine the neutral kaon mixing matrix element BK in the continuum limit with 2+1 flavors of domain wall fermions, using the Iwasaki gauge action at two different lattice spacings. These lattice fermions have near exact chiral symmetry and therefore avoid artificial lattice operator mixing. We introduce a significant improvement to the conventional nonperturbative renormalization (NPR) method in which the bare matrix elements are renormalized nonperturbatively in the regularization invariant momentum scheme (RI-MOM) and are then converted into the MS? scheme using continuum perturbation theory. In addition to RI-MOM, we introduce and implement four nonexceptional intermediate momentum schemes that suppress infrared nonperturbative uncertainties in the renormalization procedure. We compute the conversion factors relating the matrix elements in this family of regularization invariant symmetric momentum schemes (RI-SMOM) and MS? at one-loop order. Comparison of the results obtained using these different intermediate schemes allows for a more reliable estimate of the unknown higher-order contributions and hence for a correspondingly more robust estimate of the systematic error. We also apply a recently proposed approach in which twisted boundary conditions are used to control the Symanzik expansion for off-shell vertex functions leading to a better control of the renormalization in the continuum limit. We control chiral extrapolation errors by considering both the next-to-leading order SU(2) chiral effective theory, and an analytic mass expansion. We obtain BKMS? (3??GeV)=0.529(5)stat(15)?(2)FV(11)NPR. This corresponds to B?KRGI? =0.749(7)stat(21)?(3)FV(15)NPR. Adding all sources of error in quadrature, we obtain B?KRGI? =0.749(27)combined, with an overall combined error of 3.6%.

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Published date: 6 July 2011
Organisations: Theoretical Partical Physics Group

Identifiers

Local EPrints ID: 339265
URI: http://eprints.soton.ac.uk/id/eprint/339265
ISSN: 1550-7998
PURE UUID: 80d20035-baf5-49bd-a212-1aba0600730a

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Date deposited: 28 May 2012 12:56
Last modified: 18 Jul 2017 05:53

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Contributors

Author: Y. Aoki
Author: R. Arthur
Author: T. Blum
Author: P. Boyle
Author: D. Brömmel
Author: N. Christ
Author: C. Dawson
Author: T. Izubuchi
Author: C. Jung
Author: C. Kelly
Author: R. Kenway
Author: M. Lightman
Author: R. Mawhinney
Author: Shigemi Ohta
Author: C. Sachrajda
Author: E. Scholz
Author: A. Soni
Author: C. Sturm
Author: J. Wennekers
Author: R. Zhou

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