such as invisibility cloaking, super focusing, beam steering, sensing, modulating, polarization control, lasing, and nonlinear optics. [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15] One of the potential application of a metasurface platform is to enable strong light-matter coupling, where high-quality (Q) factor resonances are absolutely essential. [16,17] Fano resonances support narrow linewidths with large Q factor values. [18][19][20] The large Q factor of Fano resonant metasurfaces is derived from the enhanced electric field in the subwavelength capacitive gaps of the symmetry-broken resonators. These tightly confined fields could be switched with extremely low-threshold stimulus in the form of electrical or optical stimulus that could drive an active material out of equilibrium in the capacitive gaps. Such prospect of active switching of resonantly confined fields in metasurfaces could be significant for future applications based on light-matter interaction. [21] Early studies on tuning the Fano resonance mainly rely on changing the asymmetry parameter or the coupling distance within the unit cell of the Fano metasurface. [22][23][24] Although significant modulation of the Fano resonances was achieved, they work in passive mode. Therefore, it is important to find alternative design routes for active control of metasurfaces. One possible route is to change the conductivity of the Fano structure, so as to alter the resonance loss. Till date, there have been quite a few reports where the Fano structures were integrated with dynamic materials under external stimulus. [25][26][27][28][29][30][31] For example, an electrically controlled Fano resonance was observed at NIR wavelengths using a graphene-nanoantenna hybrid structure. [30] In addition, by implanting structured silicon patch arrays into asymmetric metallic split-ring resonators, active photoswitching of sharp Fano resonances was realized in the terahertz regime. [31] However, most of them are realized by applying single control stimulus. Active tuning approaches of Fano resonances could be further optimized by incorporating dual control, where a combination of voltage and optical pump could be simultaneously applied. Such dual control would diversify the practical implementation of these devices, as it could bridge the gap between optics and electronics. Graphenesilicon heterostructure could be one such potential system in which Fermi level of graphene responds to applied voltage, [32][33][34][35] while carrier concentration in hybrid system is controlled by Planar metamaterials are extensively studied in recent years due to their potential applications in design of flat optical components, ultrasensitive sensors, lasing spasers, and nonlinear devices. Recent studies have reported dynamic control of photoactive material-based metamaterials through optical excitation. However, most of the previous demonstrations rely on single stimulus control and typically require large fluence and ultrafast pulses of light. Here, graphene is integrated with Fano re...