TY - JOUR
T1 - The Optimal Strategy for ϵ ′/ϵ in the SM
T2 - International Conference on Kaon Physics 2019, KAON 2019
AU - Buras, Andrzej J.
N1 - Publisher Copyright:
© Published under licence by IOP Publishing Ltd.
PY - 2020/6/2
Y1 - 2020/6/2
N2 - Following the recent analysis done in collaboration with Jason Aebischer and Christoph Bobeth, I summarize the optimal, in our view, strategy for the present evaluation of the ratio ϵ ′/ϵ in the Standard Model. In particular, I emphasize the importance of the correct matching of the long-distance and short-distance contributions to ϵ ′/ϵ, which presently is only achieved by RBC-UKQCD lattice QCD collaboration and by the analytical Dual QCD approach. An important role play also the isospin-breaking and QED effects, which presently are best known from chiral perturbation theory, albeit still with a significant error. Finally, it is essential to include NNLO QCD corrections in order to reduce unphysical renormalization scheme and scale dependences present at the NLO level. Here c in m c ( c ) in the case of QCD penguin contributions and t in m t ( t ) in the case of electroweak penguin contributions play the most important roles. Presently the error on ϵ ′/ϵ is dominated by the uncertainties in the QCDP parameter and the isospin-breaking parameter IMG ALIGN="MIDDLE" ALT="$hat Ω {{\rm{eff}}}$" SRC="JPCS-1526-1-012019eqn-02.gif". We present a table illustrating this.
AB - Following the recent analysis done in collaboration with Jason Aebischer and Christoph Bobeth, I summarize the optimal, in our view, strategy for the present evaluation of the ratio ϵ ′/ϵ in the Standard Model. In particular, I emphasize the importance of the correct matching of the long-distance and short-distance contributions to ϵ ′/ϵ, which presently is only achieved by RBC-UKQCD lattice QCD collaboration and by the analytical Dual QCD approach. An important role play also the isospin-breaking and QED effects, which presently are best known from chiral perturbation theory, albeit still with a significant error. Finally, it is essential to include NNLO QCD corrections in order to reduce unphysical renormalization scheme and scale dependences present at the NLO level. Here c in m c ( c ) in the case of QCD penguin contributions and t in m t ( t ) in the case of electroweak penguin contributions play the most important roles. Presently the error on ϵ ′/ϵ is dominated by the uncertainties in the QCDP parameter and the isospin-breaking parameter IMG ALIGN="MIDDLE" ALT="$hat Ω {{\rm{eff}}}$" SRC="JPCS-1526-1-012019eqn-02.gif". We present a table illustrating this.
UR - http://www.scopus.com/inward/record.url?scp=85086413871&partnerID=8YFLogxK
U2 - 10.1088/1742-6596/1526/1/012019
DO - 10.1088/1742-6596/1526/1/012019
M3 - Conference article
AN - SCOPUS:85086413871
SN - 1742-6588
VL - 1526
JO - Journal of Physics: Conference Series
JF - Journal of Physics: Conference Series
IS - 1
M1 - 012019
Y2 - 10 September 2019 through 13 September 2019
ER -