We propose an integrability approach for planar three-point functions at finite coupling in \mathcal{N}=2 superconformal field theories obtained by \mathbb{Z}_K orbifolds of \mathcal{N}=4 super Yang-Mills (SYM). Generalizing the hexagon formalism for \mathcal{N}=4 SYM, we reproduce the structure constants of Coulomb branch operators, previously obtained by supersymmetric localization as exact functions of the 't Hooft coupling. Our analysis explains the common physical origin of Fredholm kernels in integrability and localization, and hints at structures after the resummation in the hexagon formalism.
