I. Introduction
In recent years, the antenna literature has seen a resurgence of work centered around the theory of characteristic modes (TCM). Originally formulated by Garbacz in 1971 [1], the method was revisited and reformulated by Harrington and Mautz [2], [3]. Using the method-of-moments impedance matrix [4] of a perfectly conducting structure, one can use TCM to generate a set of modal currents with convenient properties. These modes are characterized entirely by the shape of the object, independent of any excitation. TCM has been the subject of application-focused review papers [5], [6] attempting to refine the popular understanding of the method and expand on what it offers the larger antenna engineering field. More recently, characteristic modes have been used in devising broadband equivalent circuit models of antennas [7], automated design resonant single- and multiband antennas [8], as well as enabling modal considerations of the antenna -factor [9], [10].