I. Introduction
Modern interconnect structures are becoming ever more miniaturized and complex, operating up to very high frequencies for which the corresponding wavelengths are comparable to their longitudinal dimension. However, as the dimensions of their cross Section most often remain sufficiently small with respect to the smallest wavelength of the transported signals, it is still possible to describe these interconnects using frequency-dependent, per unit-of-length (p.u.l.), RLGC transmission line parameters [1] derived from a suitable quasi-transverse magnetic (quasi-TM) electromagnetic analysis, as thoroughly motivated and validated in [2] and [3]. The quasi-TM regime implies that the longitudinal component of the magnetic field remains negligible. Moreover, the broadband nature of the signals, with frequency components ranging from dc to several tens of GHz, necessitates an analysis that accounts for current crowding, conductor losses, and the skin effect in the cross Section as these phenomena change dramatically over the considered frequency range.