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Principles of Fluorescence Spectroscopy

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PRINCIPLES OF FLUORESCENCE SPECTROSCOPY 101<br />

4.2. BIOPOLYMERS DISPLAY MULTI-EXPONEN-<br />

TIAL OR HETEROGENEOUS DECAYS<br />

At first glance the measurement <strong>of</strong> decay times seems<br />

straightforward (Figure 4.3), so why do these measurements<br />

receive so much attention? Interpretation <strong>of</strong> the data<br />

in Figure 4.3 was relatively simple because the decays were<br />

single exponentials. However, most samples display more<br />

than one decay time. This situation is illustrated by a protein<br />

with two tryptophan residues (Figure 4.4). Suppose that<br />

both residues display lifetimes <strong>of</strong> 5 ns. Then the decay<br />

would be a simple single exponential decay. The decay<br />

would be simple to analyze, but one could not distinguish<br />

between the two tryptophan residues. Now suppose a collisional<br />

quencher is added and that only the residue on<br />

the surface <strong>of</strong> the protein is accessible to quenching.<br />

Assume that the added quencher reduces the lifetime <strong>of</strong><br />

the exposed residue to 1 ns. The intensity decay is now<br />

a double exponential:<br />

I(t) α 1e t/5.0 α 2e t/1.0<br />

(4.7)<br />

In this expression the α i values are called the pre-exponential<br />

factors. For the same fluorophore in different environments,<br />

which usually display the same radiative decay<br />

rates, the values <strong>of</strong> α i represent the fractional amount <strong>of</strong> fluorophore<br />

in each environment. Hence, for the protein<br />

shown in Figure 4.4 one expects α 1 = α 2 = 0.5. The presence<br />

<strong>of</strong> two decay times results in curvature in the plot <strong>of</strong><br />

log I(t) versus time (dashed). The goal <strong>of</strong> the intensity<br />

decay measurements is to recover the decay times (τ i ) and<br />

amplitudes (α i ) from the I(t) measurements.<br />

The presence <strong>of</strong> two decay times can also be detected<br />

using the frequency-domain method. In this case one examines<br />

the frequency response <strong>of</strong> the sample, which consists<br />

<strong>of</strong> a plot <strong>of</strong> phase and modulation on a logarithmic frequency<br />

axis. The longer lifetime tryptophan (τ 1 = 5 ns, solid) and<br />

the shorter lifetime tryptophan (τ 2 = 1 ns, dotted) each display<br />

the curves characteristic <strong>of</strong> a single decay time. In the<br />

presence <strong>of</strong> both decay times (τ 1 = 5 ns and τ 2 = 1 ns,<br />

dashed), the frequency response displays a more complex<br />

shape that is characteristic <strong>of</strong> the heterogeneous or multiexponential<br />

intensity decay. The FD data are used to recover<br />

the individual decay times (τ i ) and amplitudes (α i ) asso-<br />

Figure 4.4. Simulated intensity decays <strong>of</strong> buried (W 1 ) and exposed (W 2 ) tryptophan residues in the absence and presence <strong>of</strong> a collisional quencher.

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