“…Since then, the search for new possibilities to exploit the similarities between grooved metal structures and the true SPPs has been an extremely active area of research [5], [6]. For example, graded rectangular [7], thin rectangular [8], and trapezoidal grooved structures [9], [10], among others, have been proposed. The desirable properties of spoof SPPs include: a) low-frequency operation, which can facilitate dispersion [11]; c) high confinement of the fields, which is proportional to δ =(k 2 −k 2 0 ) −1/2 , with k and k 0 the propagating and space momentum, respectively; d) low dispersion, related to the group velocity and derived also from the dispersion relation; e) preservation of the original boundary, which requires shallow grooves; and f) controllability of the former properties, which means that small variations of the groove dimensions can have a significant impact on the characteristics of the SPP waves.…”