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Principles of Fluorescence Spectroscopy

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146 TIME-DOMAIN LIFETIME MEASUREMENTS<br />

Figure 4.58. Intensity decay <strong>of</strong> green fluorescence protein. From<br />

[207].<br />

GFPs are widely used as a tag to follow gene expression.<br />

The intensity decay <strong>of</strong> GFP was measured with 365-nm<br />

excitation, a 1.25-MHz repetition rate, and magic-angle<br />

polarizer conditions. 207 The emission was detected above<br />

500 nm, using an MCP PMT.<br />

The intensity decay <strong>of</strong> GFP could be well fit to a single<br />

exponential (Figure 4.58). The value <strong>of</strong> χ R 2 is slightly elevated,<br />

and not consistent with a single exponential model.<br />

However, the value <strong>of</strong> χ R 2 was not decreased by including a<br />

second decay time (χ R 2 = 1.18). Examination <strong>of</strong> the deviations<br />

(lower panel) reveals the presence <strong>of</strong> systematic oscillations<br />

for which a second decay time does not improve the<br />

fit. The failure <strong>of</strong> χ R 2 to decrease is typically an indication<br />

<strong>of</strong> systematic error as the origin <strong>of</strong> the elevated value <strong>of</strong> χ R 2.<br />

4.13.3. Picosecond Decay Time<br />

The measurement <strong>of</strong> picosecond decay times remains challenging<br />

even with the most modern instruments for TCSPC.<br />

Figure 4.59 shows a schematic for a state-<strong>of</strong>-the-art instrument.<br />

208 The primary source <strong>of</strong> excitation is a Ti:sapphire<br />

laser, which is pumped by a continuous argon ion laser. The<br />

repetition rate is decreased as needed by a pulse picker<br />

(PP). Additional excitation wavelengths are obtained using<br />

a harmonic generator (HG) for frequency doubling or<br />

tripling, or an optical parameter oscillator (OPO). The pulse<br />

Figure 4.59. Intensity decay <strong>of</strong> DASPI in methanol. The upper panel<br />

shows a schematic <strong>of</strong> the instrument with a Ti:sapphire-OPO pump<br />

source at 543 nm and an R3809U MPC PMT. DASPI is 2-[2-[3dimethylamino)phenyl]-ethyl]-N-methyl<br />

pyridinium iodide (DASPI).<br />

Revised from [208].<br />

widths were near 1 ps. This instrument has an R3809U<br />

MCP PMT that has one <strong>of</strong> the smallest available transient<br />

time spreads.<br />

The lower panel in Figure 4.59 shows the intensity<br />

decay <strong>of</strong> DASPI in methanol. DASPI has a very short decay<br />

time in this solvent. The intensity decay is not much wider<br />

than the IRF, which has an FWHM below 28 ps. The decay<br />

time recovered for DASPI is 27.5 ps. Comparison <strong>of</strong> the<br />

IRF and intensity decay <strong>of</strong> DASPI shows the need for<br />

deconvolution. In spite <strong>of</strong> the complex pr<strong>of</strong>ile <strong>of</strong> these<br />

curves, they are consistent with a single-exponential decay<br />

<strong>of</strong> DASPI with a 27.5 ps lifetime.<br />

4.13.4. Chlorophyll Aggregates in Hexane<br />

The intensity decay for the tryptophan residues in the tet<br />

repressor was relatively close to a single exponential. Intensity<br />

decays can be much more heterogeneous. One example

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