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View/Open - ARAN - National University of Ireland, Galway

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Introduction<br />

Figure 1.13: Simulated time domain traces for a fluorophore that exhibits a 1, 5, and 10<br />

ns excited-state lifetime.<br />

be fitted to a sum <strong>of</strong> exponentials:<br />

I(t) =<br />

n<br />

αie −t/τi (1.14)<br />

i=0<br />

where αi is the pre-exponential factor denoting the contribution to the total time-<br />

resolved decay <strong>of</strong> the component with lifetime τi. Figure 1.14 shows situation where<br />

there are two fluorophores with different lifetimes, one short and one long lifetime<br />

component. The fraction <strong>of</strong> the steady state intensity due to each component is<br />

given by:<br />

<br />

fi = αiτi<br />

j<br />

αjτj<br />

(1.15)<br />

For TD experiments, the intensity <strong>of</strong> the decay (I(t)) is convolved with the Instru-<br />

ment Response Function (IRF). The IRF represents the response <strong>of</strong> the measure-<br />

ment system to the excitation pulse and can be generated by recording the output<br />

from a sample that scatters the excitation light or a fluorophore <strong>of</strong> very short life-<br />

time. The convolution <strong>of</strong> the (IRF(t)) and the sample decay results in an observed<br />

26

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