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Principles of Fluorescence Spectroscopy

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812 FLUORESCENCE CORRELATION SPECTROSCOPY<br />

Figure 24.20. Confocal fluorescence images <strong>of</strong> giant unilamellar vesicles (GUVs) labeled with a cyanine (DiI-C 20 ) or a Bodipy (Bodipy-PC)-labeled<br />

lipid. The lipid compositions are shown under the images. In the upper black and white images DiI-C 20 is on the left and Bodipy-PC on the right. The<br />

bars indicate 10 µm. Revised from [67].<br />

revealed the phenomenon <strong>of</strong> anomalous subdiffusion <strong>of</strong><br />

membrane-bound proteins where the G(τ) curve is spread<br />

out over a larger range <strong>of</strong> τ values. 63–66<br />

24.5.1. Biophysical Studies <strong>of</strong> Lateral Diffusion<br />

in Membranes<br />

The ability <strong>of</strong> FCS to measure widely different diffusion<br />

coefficients has been useful in studies <strong>of</strong> lateral diffusion in<br />

membranes. Giant unilamellar vesicles (GUVs) about 35<br />

µM in diameter were used to allow observation <strong>of</strong> specific<br />

regions <strong>of</strong> the membranes. Figure 24.20 shows confocal<br />

fluorescence microscopy images <strong>of</strong> GUVs that were labeled<br />

with two lipophilic dyes: DiI-C 20 and Bodipy-PC. 67 For<br />

these images the GUVs were composed <strong>of</strong> two phospholipids:<br />

dilauroyl phosphatidylcholine (DLPC) and dipalmitoyl<br />

phosphatidylcholine (DPPC). At room temperature<br />

DLPC bilayers are in the fluid state and DPPC bilayers in<br />

the solid state. Because <strong>of</strong> the difference in length <strong>of</strong> the<br />

acyl side chain, C12 for lauroyl and C16 for palmitoyl,<br />

bilayers containing both lipids show lateral phase separation.<br />

This does not mean that each phase is composed only<br />

<strong>of</strong> DLPC or DPPC but rather that two phases exist: a fluid<br />

phase rich in DLPC and a solid phase rich in DPPC.<br />

The images in Figure 24.20 were taken through two<br />

different emission filters to select for the shorter-wavelength<br />

emission <strong>of</strong> Bodipy-PC (shown as green) or the<br />

longer-wavelength emission <strong>of</strong> DiI-C 20 (shown as red). To<br />

obtain the confocal images the GUVs were labeled with<br />

both probes at relatively high concentrations. When the<br />

GUV contains only DLPC both probes are distributed<br />

homogeneously (left). When the GUVs contain a mixture <strong>of</strong><br />

DLPC and DPPC one finds liquid domains rich in Bodipy-<br />

PC and solid domains rich in DiI-C 20 . As the mole fraction<br />

<strong>of</strong> DPPC increases the extent <strong>of</strong> the solid phase containing<br />

DiI-C 20 increases (middle and right). GUVs similar to those<br />

shown in Figure 24.20 were studied by FCS. For FCS the<br />

GUVs were labeled with only one probe DiI-C 20 at a lower<br />

concentration to allow observation <strong>of</strong> only a few probe molecules.<br />

For this system we expect the diffusion to be two<br />

dimensional with different diffusion coefficients in each<br />

phase. Assuming the probe brightness is the same in both<br />

phases the autocorrelation function becomes<br />

G(τ) C FD F(τ) C SD S(τ)<br />

V eff(C F C S) 2<br />

(24.33)<br />

where F and S refer to the fluid and solid phases, respectively,<br />

and the diffusion correlation function in each phase is<br />

given by<br />

D i(τ) ( 1 4D iτ<br />

s 2 ) 1<br />

(24.34)

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