“…Numerous structures of photoconductive antennas have been proposed, which were based on the incorporation of optical nano antennas [17], fractal geometries [18], gammadion-type structure [19], tapered helix monopole [20], hexagonal nano-antenna [21], interdigitated metallic dipole nanoantenna [22]- [24], 3D plasmon contact electrodes [25], nano-structured electrodes [26], thin-film plasma electrode [27], rectangular metal dipole nanoantenna [28], bow-tie metallic dipole nanoantenna [28], plasmon contact electrodes [29], [30], SRR-loaded antennas [31], and arrays of bowtie and four-leaf-clover-shaped antennas [32]. Further, several numerical models have been proposed for understanding the dynamics of these photoconductive antennas, such as full-wave numerical technique based on Maxwell and hydrodynamic transport equations [33], semiconductor carrier transport and migration models [22], [34], time-domain numerical modeling [35], numerical solution of induced current based on Monte Carlo simulation [36], finite element method [27], [37], and three-dimensional full-wave model [38].…”