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Microscopy-based analysis of Förster Resonance Energy Transfer (FRET) permits assessment of interactions between proteins in live cells. It provides spatial and temporal information, including information on where in the cell and in which subcellular compartment the interaction takes place and if this interaction changes over time.
Theodor Förster laid the theoretical foundation of FRET in 19481. FRET is a radiationless transfer of energy from an excited donor to an acceptor molecule and depends upon the distance of the molecules and the relative orientation of their transition dipoles as well as the overlap between the donor emission and acceptor absorption spectra. The rate of energy transfer is inversely proportional to the sixth power of the donor-acceptor distance. Thus, FRET can be used to measure molecular proximity in the range of 1-10 nm.
FRET competes with other de-excitation processes of the donor molecule and results in the so-called donor-quenching and sensitized emission of the acceptor. Donor-quenching is a reduction of the number of emitted donor photons, while sensitized emission is an increase in emitted acceptor photons. Many microscopic FRET analyses use fluorescence intensity measurements, including acceptor photobleaching2, donor photobleaching2, or FRET-sensitized photobleaching of the acceptor3.
Here, a step-by-step experimental protocol and mathematical algorithm are presented to quantify FRET using donor quenching and acceptor sensitized emission4,5, a method often referred to as ratiometric FRET. Many protocols on how to approximate sensitized emission have been published, few have quantified the absolute FRET efficiency6,7,8,9. The quantification of FRET efficiencies in the living cell requires determining (i) the crosstalk (spectral spill-over, or bleed-through) of the fluorescent proteins and, also (ii) the detection efficiency of the microscopic setup. While crosstalk can be assessed by imaging cells expressing only one of the fluorophores, the assessment of the relative detection efficiency of the donor and acceptor fluorescence is more complicated. It requires the knowledge of at least the ratio of the number of donor and acceptor molecules giving rise to the measured signals. The number of fluorophores expressed in live cells varies, however, from cell to cell and is unknown. The so-called α factor characterizes the relative signal strengths from a single excited donor and acceptor molecule. Knowledge of the factor is a prerequisite for quantitative ratiometric FRET measurements in samples with variable acceptor-to-donor molecule ratios as encountered during live-cell imaging with fluorescent proteins. Using a 1-to-1 donor-acceptor fusion protein as a calibration probe permits the determination of the α factor and also serves as a positive control. This genetically coupled probe is expressed by cells in unknown total amounts but in a fixed and known relative amount of one-to-one. The following protocol lays out how to construct the 1-to-1 probe and how to use it for quantification of FRET efficiency. A spreadsheet that includes all formulae can be found in the supplement and can be used by the readers to enter their own measurements in the respective columns as outlined below.
While the protocol uses the GFP-Cherry donor/ acceptor pair, the presented approach can be performed with any other FRET pair. The Supplementary File 1 provides details on cyan-yellow pairs.