reflection, exhibits photonic localization in the band gap determined by the period in the case of normal incidence. [6] Similarly, a helical superstructure composed of chiral chromophores leads to absorption differences between left-and right-handed CPL, referred to as the Cotton effect, owing to the asymmetry of chiral chromophores or that of achiral chromophores induced by a chiral system. [7] Chiro-optical characteristics in helical supramolecular assemblies and superstructures have attracted tremendous attention in the past decade, especially in self-organized mesogenic helical soft matter, which is an emerging scientific frontier in chemistry, functional materials, soft matter physics, biological medicine, and even sensor physics. Mesogenic soft matter, defined as soft condensed matter with molecules containing single or multiple anisotropic mesogen moieties, is distinct from common soft condensed matter in terms of molecular arrangement, interaction, and specific optical chirality, although the "soft" characteristic is still maintained. A primary reason for the softness is related to the responses of this type of matter to multiple external stimuli, such as electric fields, heat, light, mechanical forces, and even acoustic fields. [8] The control and manipulation of such soft materials by light is always more desirable than that of other stimuli due to the prominent advantages of non-contact, wireless, remote, and high-resolution control, which enable numerous unprecedented chiro-optical applications. [9] Optically, another fascinating feature of these materials is their molecular self-organization behavior, which can establish an ordered and regular arrangement with a structural parameter (≈µm) much larger than the single-molecule scale (≈nm) through the weak non-covalent molecular interaction, rather than the chemical bonds that normally exist in