摘要： Dye-sensitized solar cells (DSSCs) are existing to be a promising alternative to conventional silicon solar cells owing to its ease of fabrication, low cost, along with the additional features like flexible devices and building integrated photovoltaic system [1]. In general, DSSC architecture comprised of semiconducting photoanode, counter electrode (catalyst), and an electrolyte [2, 3]. In DSSC, the quantity of light caught by the dye-sensitized photoanode has a strong influence on the overall performance because the electrons are generated directly from the excited dye molecules by the irradiated sunlight. One of the primary key tasks is to boost the performance of the device by enriching the photon absorption in DSSCs such as the introduction of a tandem structure and the introduction of a light-scattering effect. Among these developments, the light-scattering effect had more attention than others because of an easy method for enhancing light absorption [4–7]. The simple theory of light scattering effect was introduced by Usami [8] in 1997, stating that a new photoelectrode structure consisting of top layer made up of a large sized particle film on the below layer made up of a small sized particle film; the light scattered by the top layer triggered an increase in the light absorption. In initial days, several studies had been focused on the analysis of the light-scattering effect in the DSSCs by using various simulation methods based on the Monte Carlo model, Mie theory, and the many-flux model. Subsequently, the light-scattering effect had been widely used as an important technique to develop the performance of DSSCs [9]. So, the introduction of light scattering and light scattering materials are explained in the following sections.