Liquid crystalsLiquid crystals (LCs) are typically associated with the development of various LCbased displays (LCDs) such as flat-panel televisions, touchscreen displays, and computer monitors used in our daily lives. Besides massive achievements in the field of LCDs over the last decades, [1] LCs have also attracted attention in a broad range of non-display applications from telecommunication technologies, photonics, sensors, and medicine to self-assembled amphiphilic soap molecules, which are on the borderline between soft condensed matter and nanotechnology. [2][3][4] This class of matter is of great interest mainly due to its fascinating anisotropic properties (i.e., refractive index, viscosity, elastic constant, electric conductivity, or magnetic susceptibility) that can be manipulated via responses to applied external stimuli (i.e., mechanical, electric, magnetic, or even optical stimuli) or their spontaneous self-organization.[1,5] Nowadays, many optical applications benefit from the elastic behavior of LCs (specifically commercial thermotropic LCs) which can be tuned via electric or magnetic fields. The alteration in the orientation of the mesogens in these LCs changes the orientation of the optical axis, resulting in birefringence. Several effects of the anisotropic properties of LCs with polarized light are reproduced from references [6,7] and shown in Figure 1-1.In general, LCs are referred to as intermediate phases or mesophases formed by elongated building blocks or mesogens which can be organic, inorganic, or organometallic compounds. These mesophases are thermodynamically stable and located between the three-dimensional solid crystal and the viscous liquid, which is an isotropic disordered phase. Therefore, LCs are characterized by long-ranged orientational order, which can be combined with long-ranged positional order in one or two dimensions of their long mesogens axis, resulting in direction-dependent physical properties analogous to crystalline solids whereas the ability to flow and long-ranged diffusion is preserved similar to fluids. [8] Although some liquid crystalline properties were observed and described by several researchers more than 100 years ago, thermotropic LCs were not realized until 1888 when Reinitzer[9] discovered this state of matter, which was followed by Lehmann[10] in 1889 who assigned the term 'thermotropic liquid crystals' to these mesophases (the references are in German). [11] In general, two main classes of LCs are distinguished: thermotropic within the layers and at the same time stand parallel to the layer's normal director, the smectic phase is called smectic-B. If the hexagonal order inside the layers exhibits a longrange positional order, the structure will be therefore a three-dimensional crystal. [12] Likewise, the aforementioned LC phases are observed in lyotropic LCs, however, due to the nature of these mesophases, they are formed when the concentration of the anisotropic mesogens is raised to a high enough value. If anisotropic molecular mesogens form lyotr...