I. Introduction
In the information age, wireless optical switching (WOS) technology has significantly advanced optical communication and established a robust foundation for high-performance information interaction and processing [1], [2]. Traditional WOS units, such as Micro-Electro-Mechanical Systems (MEMS) [3], are inadequate for future large-scale WOS due to their complex serial control and high energy consumption from external voltages. Consequently, researchers are focusing on reconfigurable metasurfaces (R-MTSs) to design WOS units [4], [5], [6]. R-MTSs consist of two-dimensional arrays of metamaterials with subwavelength-scale dimensions. By tailoring the parameters of meta-units, the interaction between surrounding electromagnetic waves and incident light fields can be induced [7], [8], thereby eliciting local resonances and effecting changes in amplitude and phase gradients to enable agile manipulation of light waves [9], [10], [11]. This facilitates functionalities such as spin-orbit angular momentum conversion [12], anomalous reflection beam deflection [13], reconfigurable optical switching [14], and broadband angular spectrum differentiation [15].