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Principles of Fluorescence Spectroscopy

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172 FREQUENCY-DOMAIN LIFETIME MEASUREMENTS<br />

Figure 5.14. Frequency-domain intensity decay data for GFPuv in<br />

0.05 M phosphate buffer, pH = 7, for one-photon excitation at 400 nm,<br />

and for two-photon excitation at 800 nm. From [72].<br />

Figure 5.15. The frequency responses shift to higher frequencies<br />

with increasing amounts <strong>of</strong> chloride, indicating a<br />

decrease in lifetime. One can use the data to calculate the<br />

decay times at each chloride concentration. These lifetimes<br />

are 25.5, 11.3, 5.3, and 2.7 ns, for 0, 10, 30, and 70 mM<br />

chloride, respectively (Problem 5.1).<br />

5.4.5. Intensity Decay <strong>of</strong> NADH<br />

Reduced nicotinamide adenine dinucleotide (NADH) is<br />

known to display a subnanosecond decay time near 0.4 ns.<br />

Figure 5.15. Frequency-domain intensity decays <strong>of</strong> SPQ in the presence<br />

<strong>of</strong> 0, 10, 40, and 70 mM chloride.<br />

Figure 5.16. Frequency response <strong>of</strong> NADH dissolved in 0.02 M Tris<br />

(pH 8) 25°C. The excitation wavelength was 325 nm from an HeCd<br />

laser, which was modulated with an electrooptic modulator. The emission<br />

filter was a Corning 0-52. For the two-component analysis f 1 =<br />

0.57 and f 2 = 0.43. Revised and reprinted from [2], Copyright © 1985,<br />

with permission from Elsevier Science.<br />

Its intensity decay is complex, with decay times near 0.3<br />

and 0.8 ns. 77 Frequency-domain data for NADH are shown<br />

in Figure 5.16. The presence <strong>of</strong> more than one lifetime is<br />

immediately evident from the failure <strong>of</strong> the single exponential<br />

fit (– – –) and the systematic deviations ("). Use <strong>of</strong> the<br />

two decay time model resulted in a 50-fold decrease <strong>of</strong> χ R 2.<br />

The frequency-domain data for NADH illustrate a limitation<br />

<strong>of</strong> the commercially available instruments. An upper<br />

frequency <strong>of</strong> 200 MHz is too low to determine the entire<br />

frequency response <strong>of</strong> NADH or other subnanosecond<br />

intensity decays. For this reason FD instruments were<br />

developed to allow measurements at higher modulation frequencies.<br />

5.4.6. Effect <strong>of</strong> Scattered Light<br />

A critical component <strong>of</strong> any frequency-domain or timedomain<br />

experiment should be collection <strong>of</strong> emission spectra.<br />

One possible artifact is illustrated in Figure 5.17, which<br />

shows the emission spectrum <strong>of</strong> 9,10-diphenylanthracene<br />

(DPA) in a solution that also scattered light. 69 9,10-<br />

Diphenylanthracene was dissolved in ethanol that contained<br />

a small amount <strong>of</strong> Ludox scatterer. When the emission is

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