I. Introduction
This paper focuses on the solution of linear equation systems , where is a dense, square matrix. In frequency-domain electromagnetics, this problem typically originates from the discretization of the integral form of Maxwell's equations on the surfaces of interest. For large one might use iterative solvers with computational complexities of , where is the condition number of matrix . However, certain problems, e.g. structures with high-quality factor resonances, might yield extremely ill-conditioned system matrices making iterative solves costly as grows.