An angle-selective surface (ASS) is defined as a surface that can exhibit angular selectivity allowing EM waves transmits without any reflection at the normal incidence, and with high reflect at oblique incident angles. Furthermore, ASS has potential applications in low sidelobe antenna, high-efficiency energy harvest, spatial filters and anti-jamming communications [1]. At present, researchers have proposed some ways to realize angular selectivity. For example, as early as in 2014, Y. C. Shen et al. [2] proposed that generalized Brewster angle can achieve optical broadband angular selectivity. Additionally, Z. X. Shen et al. [3] used Brewster angle and critical angles to realize a polarization-insensitive angular selectivity. Thus, the implemented angular selectivity relying on the natural or effective dielectric materials, which may extremely limit its applications in most areas. Fortunately, a double-resonance periodic array of ASS was recently proposed by Z. X. Shen et al. [4]. By properly designing the structure and dimensions of frequency-selective surface (FSS) layers, the angular selectivity of TE-polarized incident waves can be achieved. In addition, in order to achieve dual-polarizations ASS, it is generally required to add more degrees of freedom by using a three-layer FSS structure, which causes the ASS structure to have a profile larger than $\lambda$. Thus, the effective reduction of the ASS structure profile, which has good perspectives in the applications.