I. Introduction
In recent years, a lot of interest has been attracted by artificial surfaces able to provide electromagnetic properties that one cannot find in nature [1], [2]. Such structures, commonly referred to as metasurfaces (MTSs), can be employed in a wide range of frequencies, from microwaves [3] to optics [4]. Although MTSs may also be used to tailor the transmission of space waves [4], [5], they have found a vast number of applications in the control of surface-wave (SW) wavefronts [6], [7] and the design of aperture antennas [8]–[14]. At microwave frequencies, MTSs may be implemented as dense textures of subwavelength elements (typically , with being the free-space wavelength) printed on a grounded dielectric slab [10]. The resulting number of printed patches is generally around 104 for devices with a diameter. Indeed, MTS antennas [11] generally consist of circular apertures, where an SW launcher [15] is used to excite the structure. This paper will focus on circular apertures, bearing in mind that a proper stretching of the proposed basis functions may enable the treatment of elliptical ones [12], [16], [17].