Nanoparticles (NP) can modify fluorophore fluorescence in solution through multiple pathways that include fluorescence inner filter effect (IFE), dynamic and static quenching, surface enhancement, and fluorophore quantum yield variation associated with structural and conformational modifications induced by NP binding. The combined contribution of the latter three effects is termed the collective near-field effect because (1) they affect only fluorophore fluorescence in molecules close to the NPs, and (2) it is impossible to differentiate these effects with steady-state fluorescence measurements. A generalized model (F 0 corr /F NP corr = (1 + K[NP])/(1 + K[NP]S) was developed for the determination of the NP collective near-field effect S on the fluorophore fluorescence in the surface-adsorbed molecules. The popular Stern−Volmer equation (F 0 corr /F NP corr = (1 + K[NP]) used in current fluorescence studies of NP interfacial interactions is a special case of this generalized model, valid only under situations in which the surfacebound molecules are completely fluorescence inactive (S = 0). In addition, we excluded the possibility of NPs inducing significant dynamic fluorescence quenching under realistic experimental conditions on the basis of a simple back-of-the-envelope calculation. Furthermore, using an external reference fluorescence IFE correction method developed in this work, we demonstrated that gold nanoparticles (AuNPs) only slightly attenuate, but do not completely quench the fluorescence signal of the protein, bovine serum albumin (BSA), on AuNP. This result undermines the reliability of the BSA/AuNP binding constants calculated using the Stern−Volmer equation in earlier studies of BSA/AuNP interfacial interactions. The methodology and insights provided in this work should be of general importance for fluorescence study of nanoparticle interfacial interactions.
■ INTRODUCTIONThe effect of nanoparticles (NP) on fluorophore fluorescence can be highly complicated depending on the types of NP and the structure of fluorophore-containing molecules. Taking protein tryptophan fluorescence on plasmonic gold NPs (AuNPs) as examples, both fluorescence enhancement and quenching have been proposed in the literature, 1−9 and there are large discrepancies in the degree of fluorescence enhancement or quenching factors. One common belief is that AuNPs induce static or dynamic fluorescence quenching. 9−17 Such quenching is commonly modeled with the Stern−Volmer equation to estimate the AuNP/protein binding rate or binding affinity constants.Despite its popularity, the general applicability of the Stern− Volmer equation for fluorophore interactions with NPs is highly questionable. Indeed, the Stern−Volmer equation is applicable only in situations in which fluorophore fluorescence is completely quenched in the dynamic and static fluorophore/ quencher complex. Such a scenario is unlikely to occur for general NPs such as silica, graphene, two-dimensional nanosheets, or plasmonic AuNPs. Using protein binding to AuNPs as an ...