TY - JOUR
T1 - Precision computation of the kaon bag parameter
AU - Dürr, S.
AU - Fodor, Z.
AU - Hoelbling, C.
AU - Katz, S. D.
AU - Krieg, S.
AU - Kurth, T.
AU - Lellouch, L.
AU - Lippert, T.
AU - McNeile, C.
AU - Portelli, A.
AU - Szabó, K. K.
N1 - Funding Information:
We thank Jérôme Charles, Robert Harlander and Steve Sharpe for helpful discussions. Computations were performed using HPC resources from FZ Jülich and from GENCI-[IDRIS/CCRT] (grant 52275) and clusters at Wuppertal and CPT. This work is supported in part by EU grants I3HP , FP7/2007-2013/ERC No. 208740 , MRTN-CT-2006-035482 (FLAVIAnet) , DFG grants FO 502/2 , SFB-TR 55 , by CNRS grants GDR 2921 and PICS 4707 .
PY - 2011/11/24
Y1 - 2011/11/24
N2 - Indirect CP violation in K→ππ decays plays a central role in constraining the flavor structure of the Standard Model (SM) and in the search for new physics. For many years the leading uncertainty in the SM prediction of this phenomenon was the one associated with the nonperturbative strong interaction dynamics in this process. Here we present a fully controlled lattice QCD calculation of these effects, which are described by the neutral kaon mixing parameter BK. We use a two step HEX smeared clover-improved Wilson action, with four lattice spacings from a≈0.054 fm to a≈0.093 fm and pion masses at and even below the physical value. Nonperturbative renormalization is performed in the RI-MOM scheme, where we find that operator mixing induced by chiral symmetry breaking is very small. Using fully nonperturbative continuum running, we obtain our main result BKRI(3.5 GeV)=0.531(6)stat(2)sys. A perturbative 2-loop conversion yields BKMS-NDR(2 GeV)=0.564(6)stat(3)sys(6)PT and B̂K=0.773(8)stat(3)sys(8)PT, which is in good agreement with current results from fits to experimental data.
AB - Indirect CP violation in K→ππ decays plays a central role in constraining the flavor structure of the Standard Model (SM) and in the search for new physics. For many years the leading uncertainty in the SM prediction of this phenomenon was the one associated with the nonperturbative strong interaction dynamics in this process. Here we present a fully controlled lattice QCD calculation of these effects, which are described by the neutral kaon mixing parameter BK. We use a two step HEX smeared clover-improved Wilson action, with four lattice spacings from a≈0.054 fm to a≈0.093 fm and pion masses at and even below the physical value. Nonperturbative renormalization is performed in the RI-MOM scheme, where we find that operator mixing induced by chiral symmetry breaking is very small. Using fully nonperturbative continuum running, we obtain our main result BKRI(3.5 GeV)=0.531(6)stat(2)sys. A perturbative 2-loop conversion yields BKMS-NDR(2 GeV)=0.564(6)stat(3)sys(6)PT and B̂K=0.773(8)stat(3)sys(8)PT, which is in good agreement with current results from fits to experimental data.
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U2 - 10.1016/j.physletb.2011.10.043
DO - 10.1016/j.physletb.2011.10.043
M3 - Article
AN - SCOPUS:80955151655
SN - 0370-2693
VL - 705
SP - 477
EP - 481
JO - Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physics
JF - Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physics
IS - 5
ER -