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182      FLUORESCENCE MICROSCOPY

                                                                      Stokes shift










                                            A                                            E



                                                  Absorbance                  Emission




                                             350    400    450    500    550    600    650
                                                             Wavelength (nm)

                                Figure 11-3
                                Normalized absorption and fluorescence emission spectra of fluorescein-conjugated IgG.
                                Both spectra span a wide range of wavelengths. Fluorescein has an absorption/excitation
                                peak at 492 nm, but is also stimulated by ultraviolet wavelengths. Fluorescein emission has
                                a peak at 520 nm and looks yellow-green to the eye, but actually fluoresces at wavelengths
                                ranging from blue to red. The difference in nanometers between the excitation and emission
                                maxima is called the Stokes shift.


                                quenching molecules, and others. This fact explains why the fluorescence of a dye such
                                as fluorescein varies depending on whether it is free in solution or conjugated to a pro-
                                tein or other macromolecule.


                                PROPERTIES OF FLUORESCENT DYES


                                The excitation and emission spectra of fluorescent molecules are commonly observed to
                                overlap. The difference in wavelength or energy between the excitation and emitted fluo-
                                rescent photons is called the Stokes shift. In practice, the Stokes shift is the difference
                                between the excitation and emission maxima (Fig. 11-3). Depending on the particular
                                fluorescent molecule, the shift can range from just a few to several hundred nanometers.
                                The Stokes shift for fluorescein is  20 nm, while that for porphyrins is over 200 nm.
                                Dyes exhibiting a large Stokes shift are advantageous in fluorescence microscopy,
                                because the bands of excitation and fluorescence wavelengths are easier to isolate using
                                interference filters. Another important criterion for dye selection is the molar extinction
                                coefficient, which describes the potential of a fluorochrome to absorb photon quanta,
                                and is given in units of absorbance (optical density) at a reference wavelength (usually
                                the absorption maximum) under specified conditions. The quantum efficiency (QE) of
                                fluorescence emission is the fraction of absorbed photon quanta that is re-emitted by a
                                fluorochrome as fluorescent photons. QE varies greatly between different fluo-
                                rochromes and for a single fluorochrome under different conditions. For soluble fluo-
                                rescein dye at alkaline pH, the quantum efficiency can be as high as 0.9—an extremely
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