“…Among these include the luminophore PLQY, optical density of luminophores, GG of the LSC system, Stokes shift of the luminophore absorption/PL profiles, trapping efficiency of the emitted PL, reabsorption probability by the luminophore species, attenuation and bulk/surface scattering by the host waveguide, and the quantum efficiency of the photovoltaic cell collector . Previous studies have highlighted the most important parameters for LSC optical and conversion efficiency; PLQY, PL trapping, optical density, and GG are observed to be highly influential for a given luminophore and LSC system type. − While some parameters need to be maximized ( e.g ., PLQY) or minimized ( e.g ., attenuation in the waveguide), others attain optimal values that strongly depend on the entire LSC design, complicating the process ( e.g ., optical density, GG). , In addition, there exist numerous pathways for photon loss intrinsic to the LSC design. Consequently, the single-junction LSC conversion efficiency remains limited to below 10%, with the current record achieving 7.1% under 1 sun illumination …”