English

RI-(S)MOM to $\overline{\rm MS}$ conversion for $B_K$ at two-loop order

High Energy Physics - Phenomenology 2025-09-04 v2 High Energy Physics - Lattice

Abstract

The Kaon bag parameter B^K {\hat{B}}_K plays a critical role in constraining the parameters of the CKM matrix and in probing physics beyond the Standard Model. In this work, we improve the precision of B^K \hat{B}_K to next-to-next-to-leading order (NNLO) and provide world averages for both 33- and 44-flavour theories. In the course of this, as our main technical development, we carry out the two-loop matching between the RI-(S)MOM and MS\overline{\mathrm{MS}} schemes. Our world averages combine all available lattice data, including conversion between the 3- and 4-flavour theories as appropriate. We obtain the result B^K(f=3)=0.7627(60)\hat B_{K}^{(f=3)} = 0.7627(60), which comprises the complete set of 33- and 44-flavour lattice results and can be used directly in phenomenological applications. The error is dominated by lattice uncertainties and missing higher-order corrections (residual scale dependence). Our averages include a PDG rescaling factor of 1.28 reflecting a mild tension among the lattice inputs after inclusion of NNLO corrections in the scheme conversion and matching across flavour thresholds. Our averages imply an updated value ϵK=2.171(65)pert.(71)non-pert.(153)param.×103|\epsilon_K|=2.171(65)_\text{pert.}(71)_\text{non-pert.}(153)_\text{param.} \times 10^{-3}. We briefly discuss applications of our results to DD-meson mixing.

Cite

@article{arxiv.2411.19861,
  title  = {RI-(S)MOM to $\overline{\rm MS}$ conversion for $B_K$ at two-loop order},
  author = {Martin Gorbahn and Sebastian Jäger and Sandra Kvedaraitė},
  journal= {arXiv preprint arXiv:2411.19861},
  year   = {2025}
}

Comments

33 pages, 11 figures, 9 tables, v2: match published version

R2 v1 2026-06-28T20:17:06.843Z