We study the dependence on the charm quark mass of the leading-order low-energy constants of the $\mathrm{\Delta }S=1$ effective Hamiltonian, with the aim of elucidating the role of the charm mass scale in the $\mathrm{\Delta }I=1/2$ rule for $K\to \pi \pi$ decay. To that purpose, finite-volume chiral perturbation theory predictions are matched to QCD simulations, performed in the quenched approximation with overlap fermions and $m_u=m_d=m_s$. Light quark masses range between a few MeV up to around one third of the physical strange mass, while charm masses range between $m_u$ and a few hundred MeV. Novel variance reduction techniques are used to obtain a signal for penguin contractions in correlation functions involving four-fermion operators. The important role played by the subtractions required to construct renormalized amplitudes for $m_c\ne m_u$ is discussed in detail. We find evidence that the moderate enhancement of the $\mathrm{\Delta }I=1/2$ amplitude previously found in the GIM limit $m_c=m_u$ increases only slightly as $m_c$ abandons the light quark regime. Hints of a stronger enhancement for even higher values of $m_c$ are also found, but their confirmation requires a better understanding of the subtraction terms.

• Received 24 June 2014

DOI:https://doi.org/10.1103/PhysRevD.90.094504