ranging from the nanometer to micrometer scale. The performance of solar cells is strongly correlated to the morphology within the OPV fi lm, and optimizing it is essential. Typically, a fi ner intermixture between the blend donor and acceptor components benefi ts exciton dissociation and charge carrier generation, while a coarse more phase pure and highly crystalline morphology is benefi cial to charge transport and reduced recombination of free charge carriers.A common approach to optimizing BHJ morphology is the introduction of liquid additives to the casting solution. These include 1,8-diiodooctane (DIO), 1,8-octanedithiol (ODT), and 1-chloronaphtalene (CN). [8][9][10][11][12] These additives have a surprising diversity of impacts on the fi lm structure; they can increase domain sizes when the morphology is too intimately mixed and they can reduce domain sizes when the morphology is too coarse. [ 10,[13][14][15] The benefi cial morphology changes caused by the additives were originally attributed to selective solvation of the fullerene, [ 8 ] but recent studies have established that the working mechanisms for additives are far more diverse. [ 16,17 ] We and others have used in-situ grazing incidence X-ray diffraction (GIXD), grazing incidence small angle X-ray scattering (GISAXS), and optical studies to gain insight into the real-time structure evolution of spin-coated and blade-coated BHJs. [ 16,[18][19][20][21][22][23][24] It was shown that additives can impact the structure evolution of polymer-fullerene BHJs by decreasing the solvent quality and directly or indirectly plasticizing the crystallizing material, which generally results in higher crystallinity and a modifi ed nanometer-scale domain structure. Although in-situ X-ray scattering methods have tremendously advanced our understanding of BHJ structure evolution, their contrast mechanisms are limited. GIXD requires long range order, and defi nitive GISAXS requires serendipitous contrast between the BHJ components and all the formulation liquids. The GIXD requirement for long range order is particularly problematic for low-crystallinity BHJ systems for which diffraction intensity is limited and morphology evolution must be discussed based on the evolution of the amorphous halo of either of the blend components. [ 19 ] To augment our toolkit for in-situ structure evolution measurements, we have developed steady state photoluminescence