Abstract

The significance of fluorescence anisotropy in fluorescence intensity and lifetime measurements, and erroneous measurements and interpretations resulting from its disregard, are thoroughly discussed, formulated and quantified. In all fluorescence-related measurements--including excitation and emission spectra, relative fluorescence intensity (FI), fluorescenc life time (FLT), fluorescence resonance energy transfer (FRET), etc., with the exception of fluorescence polarization and anisotropy--it is generally true that the higher the fluorescence anisotropy, the greater the distortion of fluorescence measurements. Quantifiable distortions occur when fluorescence measurements are conducted without considering the influence of fluorescence anisotropy. Here, this influence is described by numerous newly developed mathematical expressions which are simulated and experimentally confirmed utilizing single and binary fluorescent solutions of fluorophores with different spectroscopic characteristics. A marked agreement is shown between the theory and experimental data, clearly indicating the legitimacy of the physical suppositions and the mathematical expressions presented in this paper. Practical and instructive implications are discussed. The following findings are of special applicative importance: 1) the existence of an infinite number of couples of Magic Angles; 2) the deviation between two equally fluorescing particles having different fluorescence anisotropies; 3) the relation between the detected fluorescence intensity and anisotropy when measured under various setups of emission and excitation polarizers; 4) the dependence of the artificial normalized steady-state weight of a single-exponentially decaying fluorophore on its fluorescence anisotropy.

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