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Principles of Fluorescence Spectroscopy

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148 TIME-DOMAIN LIFETIME MEASUREMENTS<br />

Figure 4.62. Lifetime distribution <strong>of</strong> Annexin V Domain III in the<br />

presence <strong>of</strong> phospholipid at various lipid-to-protein molar ratios<br />

(L/P). The lipid was an 80/20 molar ratio <strong>of</strong> DOPC and DOPS, where<br />

S indicates serine. Revised from [214]. The upper panel shows a<br />

schematic <strong>of</strong> Annexin insertion into membranes. Reprinted with permission<br />

from [218].<br />

4.14. DATA ANALYSIS: MAXIMUM ENTROPY<br />

METHOD<br />

Intensity decays <strong>of</strong> biomolecules are usually multi-exponential<br />

or non-exponential. The decays can be fitted using<br />

the multi-exponential model. However, it is difficult to<br />

obtain an intuitive understanding <strong>of</strong> the results by examining<br />

table <strong>of</strong> α i and τ i values. Analysis <strong>of</strong> the decays in terms<br />

<strong>of</strong> lifetime distribution (Section 4.11.2) is <strong>of</strong>ten useful for<br />

visualizing the decay. However, when using NLLS the lifetime<br />

distribution analysis is usually performed in terms <strong>of</strong><br />

assumed shape functions (eqs. 4.35 and 4.36). Analysis<br />

using the maximum entropy method (MEM) allows recovery<br />

<strong>of</strong> lifetime distributions without assumptions about the<br />

shape <strong>of</strong> the components.<br />

The MEM is mathematically complex 213–216 and the fitting<br />

criteria somewhat subjective. Most <strong>of</strong> the published<br />

analyses were performed using commercial algorithms<br />

which are not completely explained. Nonetheless, the MEM<br />

is now widely utilized and provides insight into complex<br />

intensity decays.<br />

The MEM is based on maximizing a function called<br />

the Skilling-Jaynes entropy function:<br />

∞<br />

α(τ)<br />

S α(τ)<br />

m(τ) α(τ) log<br />

m(τ)<br />

0<br />

dτ<br />

(4.43)<br />

In this expression α(τ) is the recovered distribution and<br />

m(τ) is an assumed starting model that is flat in log τ space.<br />

The MEM method is not used alone, but the fits are performed<br />

while calculating χ R 2 according to eq. 4.22 to<br />

ensure that the recovered distribution is consistent with the<br />

data. In contrast to NLLS there does not appear to be a welldefined<br />

stopping point for the MEM analysis. The analysis<br />

is stopped when χ R 2 does not decrease more than 2% for 20<br />

interactions. The MEM is advantageous because it provides<br />

smooth α(τ) spectra that have enough detail to reveal the<br />

shape <strong>of</strong> the distribution. The MEM method is claimed to<br />

not introduce α(τ) components unless they are needed to fit<br />

the data.<br />

An example <strong>of</strong> an MEM analysis is shown in Figure<br />

4.62 for domain III <strong>of</strong> Annexin V. Annexins are peripheral<br />

membrane proteins that interact with negatively charged<br />

phospholipids. Annexins can become inserted into membranes<br />

(Figure 4.62), so the tryptophan intensity decays are<br />

expected to be dependent on the presence <strong>of</strong> phospholipids.<br />

This domain <strong>of</strong> Annexin V contains a single tryptophan<br />

residue at position 187 (W187). The intensity decays <strong>of</strong><br />

W187 were measured by TCSPC. The excitation source<br />

was synchrotron radiation that appeared as pulses at 13.6<br />

MHz with a pulse width <strong>of</strong> 1.4 ns. 215 The maximum entropy<br />

analysis shows a shift from a dominant component near 0.9<br />

ns in the absence <strong>of</strong> membrane to a longer-lived component

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