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“…This prescription has good chiral symmetry properties and leading O(a 2 ) scaling. We extend our previous work [3] by adding a second lattice spacing to quantify discretisation effects and by using both exceptional and non-exceptional kinematics for our intermediate renormalisation schemes.…”
Section: Introductionmentioning
confidence: 98%
“…Their results are shown in Tab.1. There is some tension between these measurements; our previous work [3] used a single lattice spacing, n f = 2 + 1 flavours and renormalised the operators non-perturbatively using the intermediate, exceptional, RI-MOM scheme. The works [4,5] also used the RI-MOM scheme, have n f = 2 and n f = 2 + 1 + 1 flavours respectively and performed an a 2 → 0 extrapolation.…”
Section: Introductionmentioning
confidence: 99%
“…B 5 RBC-UKQCD [3] 0.53(2) 0.43(5) 0.75(9) 0.69(7) 0.47 (6) ETM [4] 0.51(2) 0.47(2) 0.78(4) 0.75(3) 0.60(3) ETM [5] 0.51(2) 0.46(3) 0.79(5) 0.78(5) 0.49(4) SWME [6] 0.52(2) 0.53(2) 0.77(6) 0.98(6) 0.75(8) Recently, several groups have measured a dimensionless prescription of these BSM operators (their bag parameters) in modern, dynamical fermion simulations. Their results are shown in Tab.1.…”
“…This prescription has good chiral symmetry properties and leading O(a 2 ) scaling. We extend our previous work [3] by adding a second lattice spacing to quantify discretisation effects and by using both exceptional and non-exceptional kinematics for our intermediate renormalisation schemes.…”
Section: Introductionmentioning
confidence: 98%
“…Their results are shown in Tab.1. There is some tension between these measurements; our previous work [3] used a single lattice spacing, n f = 2 + 1 flavours and renormalised the operators non-perturbatively using the intermediate, exceptional, RI-MOM scheme. The works [4,5] also used the RI-MOM scheme, have n f = 2 and n f = 2 + 1 + 1 flavours respectively and performed an a 2 → 0 extrapolation.…”
Section: Introductionmentioning
confidence: 99%
“…B 5 RBC-UKQCD [3] 0.53(2) 0.43(5) 0.75(9) 0.69(7) 0.47 (6) ETM [4] 0.51(2) 0.47(2) 0.78(4) 0.75(3) 0.60(3) ETM [5] 0.51(2) 0.46(3) 0.79(5) 0.78(5) 0.49(4) SWME [6] 0.52(2) 0.53(2) 0.77(6) 0.98(6) 0.75(8) Recently, several groups have measured a dimensionless prescription of these BSM operators (their bag parameters) in modern, dynamical fermion simulations. Their results are shown in Tab.1.…”
“…In this talk we present an update on our previous results for the BSM B-parameters [1,2], and compare to those from other collaborations using different fermion discretizations [3,4].…”
We present updated results for kaon B-parameters for operators arising in models of new physics. We use HYP-smeared staggered quarks on the N f = 2 + 1 MILC asqtad lattices. During the last year we have added new ensembles, which has necessitated chiral-continuum fitting with more elaborate fitting functions. We have also corrected an error in a two-loop anomalous dimension used to evolve results between different scales. Our results for the beyond-the-Standard-Model Bparameters have total errors of 5 − 10%. We find that the discrepancy observed last year between our results and those of the RBC/UKQCD and ETM collaborations for some of the B-parameters has been reduced from 4−5 σ to 2−3 σ .
“…Beyond the quenched approximation, these quantities have been computed by RBC-UKQCD, [1,2], by ETM [3,4] and by SWME [5,6]. The renormalisation factors have also been studied by Alpha [7].…”
Abstract. It has been shown that the choice of renormalization scheme is crucial for four-quark operators, in particular for neutral kaon mixing beyond the Standard Model. In the context of SMOM schemes, the choice of projector is not unique and is part of the definition of the renormalisation scheme. I present the non-diagonal Fierz relations which relate some of these projectors.
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