Abstract:We calculate the B B parameter, relevant for B 0 -B 0 mixing, from a lattice gauge theory simulation at β = 6.0. The bottom quarks are simulated in the static theory, the light quarks with Wilson fermions. Improved smearing functions produced by a variational technique, most, are used to reduce statistical errors and minimize excited-state contamination of the groundstate signal. We obtain B B (4.33 GeV) = 0.98−18 (systematic) which corresponds to B B = 1.40−26 (systematic) for the oneloop renormalization-sche… Show more
“…In view of this issue, we wish to test the consistency of results from different groups, by listing in table 9 the values for B B (m b ) from refs. 100,162,163 , which were obtained by applying methods (M 1 ), (M 2 ) and (M 3 ) for uniform choices of input parameters. Indeed it turns out that method (M 2 ) systematically produces lower values of B B (m b ).…”
Section: Lattice Results For B B and B Bsmentioning
confidence: 99%
“…Attempts in this direction have been reported in the context of the B parameter B K 84,85 . Lattice results for the B parameter B B have been published recently using the static approximation 100,162,163 and also propagating heavy quarks 114,164,165 . Earlier attempts are discussed in refs.…”
Section: The ∆B = 2 Four-fermion Operator On the Latticementioning
The status of lattice calculations of heavy-light decay constants and of the B parameter B B is reviewed. After describing the lattice approach to heavy quark systems, the main results are discussed, with special emphasis on the systematic errors in present lattice calculations. A detailed analysis of the continuum limit for decay constants is performed. The implications of lattice results on studies of CP violation in the Standard Model are discussed. The status of lattice calculations of heavy-light decay constants and of the B parameter B B is reviewed. After describing the lattice approach to heavy quark systems, the main results are discussed, with special emphasis on the systematic errors in present lattice calculations. A detailed analysis of the continuum limit for decay constants is performed. The implications of lattice results on studies of CP violation in the Standard Model are discussed.
(Submitted to International Journal of Modern Physics A)
“…In view of this issue, we wish to test the consistency of results from different groups, by listing in table 9 the values for B B (m b ) from refs. 100,162,163 , which were obtained by applying methods (M 1 ), (M 2 ) and (M 3 ) for uniform choices of input parameters. Indeed it turns out that method (M 2 ) systematically produces lower values of B B (m b ).…”
Section: Lattice Results For B B and B Bsmentioning
confidence: 99%
“…Attempts in this direction have been reported in the context of the B parameter B K 84,85 . Lattice results for the B parameter B B have been published recently using the static approximation 100,162,163 and also propagating heavy quarks 114,164,165 . Earlier attempts are discussed in refs.…”
Section: The ∆B = 2 Four-fermion Operator On the Latticementioning
The status of lattice calculations of heavy-light decay constants and of the B parameter B B is reviewed. After describing the lattice approach to heavy quark systems, the main results are discussed, with special emphasis on the systematic errors in present lattice calculations. A detailed analysis of the continuum limit for decay constants is performed. The implications of lattice results on studies of CP violation in the Standard Model are discussed. The status of lattice calculations of heavy-light decay constants and of the B parameter B B is reviewed. After describing the lattice approach to heavy quark systems, the main results are discussed, with special emphasis on the systematic errors in present lattice calculations. A detailed analysis of the continuum limit for decay constants is performed. The implications of lattice results on studies of CP violation in the Standard Model are discussed.
(Submitted to International Journal of Modern Physics A)
“…[4], UKQCD coll. [12], Christensen et al [13] and also by JLQCD coll. in NRQCD when their results are extrapolated to the infinite mass limit [14].…”
Section: B-parameters From Numerical Simulations On the Latticementioning
We present recent results for the prediction of the B 0 s −B 0 s lifetime difference from lattice Heavy Quark Effective Theory simulations. In order to get a next-to-leading order result we have calculated the matching between QCD and HQET and the two loop anomalous dimension in the HQET for all the ∆B = 2 operators, in particular for the operators which enter in the width difference. We obtain for the B 0 s −B 0 s lifetime difference, ∆Γ Bs Γ Bs = (5.1 ± 1.9 ± 1.7) × 10 −2 .
“…In particular, the continuum limit has not been taken in any study so far. It turns out, though, that results for B-parameters and ξ are broadly consistent, regardless of whether NRQCD [39,40,26], relativistic heavy quarks [34,38,41] or the static approximation [42][43][44][45] …”
Section: Global Estimates: Strategies and Resultsmentioning
confidence: 99%
“…For the B-parameters B 0B0 , and the ratio ξ, there are not so many results available, and only one recent calculation uses dynamical quarks [26]. It is then clear that MILC [28] CPPACS [27] JLQCD [31] FNAL [30] MILC [29] Rome-II [22] ALPHA [17] UKQCD [34] UKQCD [33] APE [32] CPPACS [37] JLQCD [36] GLOK [35] MILC [28] CPPACS [27] JLQCD [31] FNAL [30] MILC [29] Rome-II [22] UKQCD [34] UKQCD [33] APE [38] JLQCD [26] JLQCD [40] JLQCD [39] SPQR [38,41] UKQCD [34] G+M [44,45] UKQCD [42,45] Kentucky [43] Fig. 2.…”
Section: Global Estimates: Strategies and Resultsmentioning
Abstract. The present status of lattice calculations of , B 0B0 and SU(3) flavour breaking ratios such as / is reviewed. Particular attention is devoted to systematic uncertainties, such as those arising from the lack of simulation data for dynamical quarks with realistic masses, and the related difficulties associated with chiral extrapolations. Global averages for decay constants and mixing parameters are presented (Table 1), and the procedures to obtain them are discussed in detail.
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