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Principles of Fluorescence Spectroscopy

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414 ADVANCED ANISOTROPY CONCEPTS<br />

Figure 12.1. Model system for an associated anisotropy decay: a mixture <strong>of</strong> tryptophan in solution and in HSA.<br />

Figure 12.2. Simulated associated anisotropy decay simulated for a<br />

mixture <strong>of</strong> fluorophores, τ 1 = 3 ns, θ 1 = 50 ps, τ 2 = 8 ns, θ 2 = 40 ns,<br />

r 01 = r 02 = 0.30. The individual intensity and anisotropy decays are<br />

shown in Figure 12.3.<br />

anisotropy <strong>of</strong> the tryptophan results in a transient decrease<br />

in the measured value <strong>of</strong> r(t). At longer times, the emission<br />

becomes dominated by HSA with its larger anisotropy,<br />

resulting in an increase in r(t).<br />

12.1.1. Theory for Associated Anisotropy Decay<br />

It is useful to compare the equations describing associated<br />

and non-associated anisotropy decays. For a single fluorophore<br />

that displays a multi-exponential intensity and<br />

anisotropy decay the parallel and perpendicular components<br />

<strong>of</strong> the emission are given by<br />

(12.2)<br />

(12.3)<br />

These expressions can be written in terms <strong>of</strong> the multiple<br />

exponential components in I(t) and r(t):<br />

I ||(t) 1<br />

3 ∑ i<br />

I (t) 1<br />

3 ∑ i<br />

I ||(t) 1<br />

I(t)1 2r(t)<br />

3<br />

I(t) 1<br />

I(t)1 r(t)<br />

3<br />

α i exp(t/τ i) [ 1 2 ∑ j<br />

α i exp(t/τ i) [ 1 ∑ j<br />

r 0j exp(t/θ j) ]<br />

r 0j exp(t/θ j) ]<br />

(12.4)<br />

(12.5)

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