is strongly dependent on the structural shape and size of the nanoparticle, the polarization of incoming light, and the surrounding dielectric medium. This was shown to provide a promising way to generate, as well as modulate, color in the visible region with high efficiency. [4,8,[11][12][13][14][15] Therefore, plasmonic metasurfaces are attractive for use in high-resolution color displays, counterfeiting elements, and various imaging applications. However, the functionality of the metasurfaces is usually limited, due to their physical design properties, which are fixed once device is fabricated. In order to overcome this limitation, and to realize dynamically controlled devices, a mechanism for strong and tunable light-matter interaction needs to be introduced within a thin layer of active material. This has led to an extensive search for new active materials that offer highly dynamic and tunable responses. [1,[5][6][7][8][9][10][11][12][13] For this goal, liquid crystals (LCs) are promising active materials that exhibit large optical birefringence, ability to control the polarization of incoming light, and most importantly the LC molecules can be efficiently controlled by external electric or magnetic fields, light, and temperature. [16,17] It was shown that LCs possess the highest birefringence compared to any other natural materials over the entire visible-IR-THz-microwave spectrum, together with low power consumption and low operating voltage. Therefore, the LC based active control mechanisms have a significant advantage over other suggested mechanism to develop active metasurface platforms. [4][5][6][7][8][18][19][20][21] Recently, some studies [22][23][24][25][26][27][28][29][30][31][32] have reported on nematic LC enabled metasurfaces that were activated by two different methods. One method was based on the ability to control the LC dielectric constants by external stimuli, which in turn can significantly influence the resonant response of the metasurface. The other approach was based on the ability to rotate the polarization of incoming light by a twisted nematic LC (TN-LC) configuration, and utilize the polarization selectivity of the metasurfaces. Specifically, for color manipulation applications, Olson et al. [22] have employed a TN-LC layer over plasmonic nanorod arrays and demonstrated that the intensity of the plasmonic color pixels can be modulated with an applied voltage. This approach can be used in order to replace the color filters in conventional Bayer pattern, where the combination of three different color pixels is required. Lee et al. [27] proposed an asymmetric lattice nanohole array based electrically tunable Recent demonstrations of metasurfaces show their great potential to realize flat and multifunctional optical elements, viable for many new device applications. Yet, a major frontier in this field is to develop active, tunable, and reconfigurable metasurface platforms. These are highly desirable in modern technologies that require dynamic modulation of light. To achieve this goal, i...