“…For all PV systems, optical loss is a major factor that hinders the attainment of the Shockley–Queisser limit: (1) a certain amount of sunlight is reflected off the cell surface, (2) absorbed by the inactive layer of the PV module, or (3) incompletely trapped inside the semiconductor . All these phenomena reduce the photocurrent that can be achieved in cells. − To overcome the limitations, a strategy to reduce the inactive area of the solar cell and efficient light delivery to the active area is highly required, eliminating losses from nonradiative recombination or incomplete absorption. , The incorporation of properly designed nanostructures to control the flow of light reduces the aforementioned optical losses and mitigates optical absorption, increasing the photocurrent, particularly through encapsulation layers. − Encapsulation is the final step in the modularization of solar cells, and it covers the surface of the cell and controls the transmission properties of the incident light to promote maximum conversion in the primary cell without affecting its intrinsic behavior . Based on the design of the photonic structure to deliver sunlight into the active area, structural approaches such as the use of prisms, randomly scattered pyramid structures, , tapered structures, , diffraction gratings, , correlating nanostructure, and periodic/nonperiodic array , have been reported.…”