Circularly polarized (CP) light has garnered significant attention due to its extensive applications across fields such as optoelectronic devices, spintronics, optical communication of spin information, and optical sensing and imaging. The ability to generate and control CP light is essential, as the handedness-left-(LCP) or right-circularly polarized (RCP)plays a distinct role in modulating light-matter interactions. Organic materials structured at the micro-or nanoscale and capable of direct CP light generation within laser systems offer substantial potential, not only in device applications but also as powerful platforms for exploring chiral light-matter interactions. Organic compounds composed of chiral molecules exhibit intrinsic photophysical properties such as circular dichroism (CD) and circularly polarized luminescence (CPL), which are the differential absorption and emission of left-and right-handed light. Despite their potential for generating CP light, most small molecules exhibit weak CD, leading to low dissymmetry factors (g lum < 10 -3 ) in the visible range. While larger dissymmetry factors (greater than 0.2) can be achieved through advanced fabrication methods, these systems very rarely produce a coherent and highly polarized luminescence which would be necessary for stimulated CP-emission. The prospect of coherent CP laser light, which can reach intensities over 10 8 times greater than fluorescence, remains particularly compelling.