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Principles of Fluorescence Spectroscopy

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174 FREQUENCY-DOMAIN LIFETIME MEASUREMENTS<br />

Figure 5.19. Frequency response for IR-144 in ethanol (open symbols)<br />

and DOTCI in ethanol (filled symbols). Best one-component fits<br />

to each data are indicated by the lines. IR-144 and DOTCI were excited<br />

with laser diodes at 790 and 670 nm, respectively. Revised and<br />

reprinted with permission from [79], Copyright © 1992, American<br />

Chemical Society.<br />

complex laser source can be replaced with laser diodes, 78–79<br />

and light-emitting diodes. 80–86 Frequency-domain measurements<br />

have also been accomplished with electroluminescent<br />

devices, 87 and even a modulated deuterium lamp. 88<br />

Given the rapid advances with pulsed LDs and LEDs these<br />

devices are likely to be the dominant excitation source for<br />

FD measurements in the near future.<br />

5.5.1. Laser Diode Excitation<br />

The output <strong>of</strong> laser diodes can be modulated up to several<br />

GHz. Hence, laser diodes can be used for FD excitation<br />

without the use <strong>of</strong> a modulator. Data are shown in Figure<br />

5.19 for two laser dyes—IR-144 and DOTCI—which were<br />

excited with 791- or 670-nm laser diodes, respectively (Figure<br />

5.19). Frequency-doubled laser diodes have also been<br />

used to obtain shorter excitation wavelengths near 400<br />

nm. 89 However, the need for frequency-doubled LDs has<br />

diminished given the availability <strong>of</strong> LDs and LEDs with<br />

fundamental outputs ranging from 280 to 820 nm.<br />

5.5.2. LED Excitation<br />

It is now known that LEDs can be modulated to several<br />

hundred MHz. 85–86 Hence, LEDs are becoming an alternative<br />

to modulated arc lamps. The modulated output <strong>of</strong> a<br />

390-nm LED output was used to measure the 3.2-ns decay<br />

time <strong>of</strong> green fluorescent protein (not shown) and the 11.8ns<br />

lifetime <strong>of</strong> 9-cyanoanthracene 85 (Figure 5.20).<br />

The use <strong>of</strong> a simple light source such as an LED is likely<br />

to find use in analytical chemistry and clinical chemistry.<br />

84–85 This is illustrated in Figure 5.21 for the potassi-<br />

Figure 5.20. Intensity decay <strong>of</strong> 9-cyanoanthracene in ethanol using<br />

the 390-nm output <strong>of</strong> a UV LED as the excitation source. Revised<br />

from [85].<br />

um-sensitive probe CD 222. This probe has a lifetime <strong>of</strong><br />

0.15 ns in the absence <strong>of</strong> potassium and 0.67 ns in the presence<br />

<strong>of</strong> bound potassium. The frequency response could be<br />

measured up to 300 MHz using a modulated UV LED at<br />

373 nm. The possibility <strong>of</strong> measuring nanosecond decay<br />

times using modulated LEDs, and the availability <strong>of</strong> a wide<br />

range <strong>of</strong> wavelengths, suggests these light sources will be<br />

used for low-cost FD instruments in the near future.<br />

Another application <strong>of</strong> LEDs will be for excitation <strong>of</strong><br />

the longer-lived metal–ligand complexes (Chapter 20). The<br />

LEDs are ideal because the 450-nm output is centered on<br />

the 450-nm charge-transfer absorption <strong>of</strong> the ruthenium<br />

complexes. The shorter wavelengths are suitable for excitation<br />

<strong>of</strong> the higher-quantum-yield rhenium complexes (Figure<br />

5.22). In this case the entire frequency response <strong>of</strong><br />

[Re(dpphen)(CO) 3 ) (4-COOHPy)] + was measured in the<br />

absence (10.24 :s) or presence <strong>of</strong> oxygen (598 ns). 84<br />

Figure 5.21. Frequency response <strong>of</strong> the potassium probe CD 222<br />

measured with a 373-nm LED ("). From [84].

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