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Principles of Fluorescence Spectroscopy

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PRINCIPLES OF FLUORESCENCE SPECTROSCOPY 465<br />

Figure 13.32. Membrane fusion detection by RET. Top: Homotransfer<br />

and self-quenching. Bottom: RET for a D–A pair.<br />

ized around gramicidin then RET to the dansyl acceptor<br />

would exceed the calculated values.<br />

13.8.2. Membrane Fusion and Lipid Exchange<br />

Energy transfer has been widely used to study fusion and/or<br />

aggregation <strong>of</strong> membranes. These experiments are shown<br />

schematically in Figure 13.32. Suppose a lipid vesicle contains<br />

a high concentration <strong>of</strong> a fluorophore that undergoes<br />

homo-RET (Figure 13.32). Initially the membrane will be<br />

dimly fluorescent because <strong>of</strong> self-quenching (top). If this<br />

vesicle fuses with another unlabeled vesicle the extent <strong>of</strong><br />

self-quenching will decrease and the emission intensity will<br />

increase. An alternative approach is to use RET between a<br />

donor and acceptor (bottom). In this case the vesicles<br />

labeled with each type <strong>of</strong> fluorophore will appear with different<br />

colors. Upon fusion the color will change. Depending<br />

upon the concentrations <strong>of</strong> donor and acceptor in the<br />

membranes, the extent <strong>of</strong> RET could be small, in which<br />

case the color <strong>of</strong> the fused vesicles would be a simple mixture<br />

<strong>of</strong> the two colors. If the probe concentration results in<br />

efficient RET then the fused vesicles will have the color <strong>of</strong><br />

the acceptor.<br />

As seen from Figure 13.28 the acceptor density does<br />

not need to be large. Any process that dilutes the donor and<br />

acceptors from the initially labeled vesicles will result in<br />

less energy transfer and increased donor emission. For<br />

example, if the D–A-labeled vesicles fuse with an unlabeled<br />

vesicle, the acceptor becomes more dilute and the donor<br />

intensity increases. Alternatively, the donor may display a<br />

modest water solubility adequate to allow exchange<br />

between vesicles. Then some <strong>of</strong> the donors will migrate to<br />

the acceptor-free vesicles and again the donor fluorescence<br />

will increase. It is also possible to trap a water-soluble fluorophore–quencher<br />

pair inside the vesicles. Upon fusion<br />

the quencher can be diluted and/or released. A wide variety<br />

<strong>of</strong> different procedures have been proposed, 73–79 but most<br />

rely on these simple proximity considerations.<br />

RET has been used to obtain images <strong>of</strong> membranes as<br />

they fuse together. Figure 13.33 shows images <strong>of</strong> giant unilamellar<br />

vesicles (GUVs) that were labeled either with a<br />

cyanine dye DiO (left, green) or a rhodamine dye Rh–PE<br />

(right, orange). 80 The two types <strong>of</strong> vesicles contained oppositely<br />

charged lipids, which resulted in rapid fusion. The<br />

GUVs were brought together by electrophoretic migration<br />

in a fluid channel. The images were obtained with a color<br />

CCD camera, so they are real color images. Prior to contact<br />

between the GUVs, the DiO-labeled vesicle is bright and<br />

the Rh–PE-labeled vesicle dark. Rh–PE is dark because it<br />

absorbs weakly at the excitation wavelength <strong>of</strong> near 450<br />

nm. As the vesicles make contact and fuse, a bright orange<br />

signal appears, which is due to Rh–PE. Eventually the<br />

entire vesicle surface becomes orange. The green emission<br />

from DiO is mostly quenched due to RET to Rh–PE.<br />

13.9. EFFECT OF τ 2 ON RET<br />

While the effect <strong>of</strong> κ 2 in energy transfer is frequently discussed,<br />

81–82 there are relatively few experimental<br />

results. 83–86 Most <strong>of</strong> the experimental results are measurements<br />

with a single κ 2 value, rather than a systematic<br />

dependence <strong>of</strong> k T (r) or κ 2 . However, the experimental<br />

results show that the value <strong>of</strong> κ 2 does affect the rate <strong>of</strong> energy<br />

transfer. Figure 13.34 shows the chemical structure <strong>of</strong><br />

two donor–acceptor pairs. The anthracene donor was linked<br />

either in plane with the porphyrin acceptor (κ 2 = 4) or in the<br />

axial position (κ 2 = 0) The transition moment <strong>of</strong> the<br />

anthracene is along the short axis <strong>of</strong> the molecule. Emission<br />

spectra <strong>of</strong> these D–A pairs were compared to a donor control<br />

molecule. For the axial anthracene (κ 2 = 0) there is<br />

almost no RET to the porphyrin. For the in-plane<br />

anthracene with κ 2 = 4 there is almost no emission showing<br />

RET is rapid for these colinear transitions. These results<br />

show that orientation can have a dramatic effect on the RET<br />

efficiency. However, these D–A pairs are rather rigidly<br />

linked and a smaller effect is expected if the acceptor had<br />

more mobility relative to the porphyrin ring.

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