$K \to \pi$ matrix elements of the chromomagnetic operator on the lattice

TL;DR

This paper presents the first lattice QCD calculation of the $K o mbda$ matrix elements of the chromomagnetic operator, providing new non-perturbative results crucial for understanding $mbda$ transitions beyond the Standard Model.

Contribution

It introduces a novel lattice QCD computation of the chromomagnetic operator's matrix elements, including non-perturbative mixing coefficients, with results that challenge previous model estimates.

Findings

Calculated $B_{CMO}^{K mbda}$ at physical point: 0.273(70)

Determined $B_{CMO}$ in SU(3) chiral limit: 0.072(22)

Results are significantly smaller than previous model estimates.

Abstract

We present the results of the first lattice QCD calculation of the $K \to \pi$ matrix elements of the chromomagnetic operator $O_{CM} = g\, \bar s\, \sigma_{\mu\nu} G_{\mu\nu} d$, which appears in the effective Hamiltonian describing $\Delta S = 1$ transitions in and beyond the Standard Model. Having dimension 5, the chromomagnetic operator is characterized by a rich pattern of mixing with operators of equal and lower dimensionality. The multiplicative renormalization factor as well as the mixing coefficients with the operators of equal dimension have been computed at one loop in perturbation theory. The power divergent coefficients controlling the mixing with operators of lower dimension have been determined non-perturbatively, by imposing suitable subtraction conditions. The numerical simulations have been carried out using the gauge field configurations produced by the European Twisted Mass Collaboration with $N_f = 2+1+1$ dynamical quarks at three values of the lattice spacing. Our result for the B-parameter of the chromomagnetic operator at the physical pion and kaon point is $B_{CMO}^{K \pi} = 0.273 ~ (70)$, while in the SU(3) chiral limit we obtain $B_{CMO} = 0.072 ~ (22)$. Our findings are significantly smaller than the model-dependent estimate $B_{CMO} \sim 1 - 4$, currently used in phenomenological analyses, and improve the uncertainty on this important phenomenological quantity.