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Principles of Fluorescence Spectroscopy

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PRINCIPLES OF FLUORESCENCE SPECTROSCOPY 119<br />

Figure 4.25. Transit time spread for an MCP PMT (R3809U) and a<br />

miniature PMT (R7400 series in a H7422 module). Revised from [90].<br />

anywhere on the photocathode are detected. In contrast, the<br />

active area <strong>of</strong> an avalanche photodiode is usually less than<br />

1 mm 2 , and less than 10 :m x 10 :m for a high-speed APD.<br />

It is therefore difficult to focus the fluorescence onto the<br />

APD, so the sensitivity is too low for most measurements.<br />

Another disadvantage is the relatively long tail following<br />

each pulse, the extent <strong>of</strong> which depends on wavelength. The<br />

presence <strong>of</strong> a wavelength-dependent tail can create problems<br />

in data analysis since the instrument response function<br />

will depend on wavelength. Methods have been developed<br />

to actively quench the tail. Values <strong>of</strong> the full width at half<br />

Figure 4.26. Compact PMTs and modules containing the PMTs. The<br />

diameter <strong>of</strong> the PMT is 16 mm. The width <strong>of</strong> the PMT modules is 25<br />

nm. Courtesy <strong>of</strong> William Cieslik, Hamamatsu Photonics Systems.<br />

maxima have been reported from 20 to 400 ps, and APDs<br />

have been successfully used in TCSPC. 98–105<br />

APDs are now routinely used for TCSPC, especially in<br />

applications where the emission can be tightly focused,<br />

such as single-molecule detection (SMD) and fluorescencecorrelation<br />

spectroscopy (FCS). TCSPC measurements can<br />

be performed at the same time as SMD and FCS experiments.<br />

APDs have high quantum efficiencies at real wavelengths,<br />

and are the detector <strong>of</strong> choice for these applications.<br />

4.6.5. Color Effects in Detectors<br />

When performing lifetime measurements, one generally<br />

compares the response <strong>of</strong> a fluorescent sample with that <strong>of</strong><br />

a zero decay time scattering sample. Because <strong>of</strong> the Stokes<br />

shift <strong>of</strong> the sample, the wavelengths are different when<br />

measuring the sample and the impulse response function.<br />

The timing characteristics <strong>of</strong> a PMT can depend on wavelength.<br />

Color effects were significant with the older-style<br />

tubes, such as the linear-focused 56 DVVP and the sidewindow<br />

tubes. 106–111 The time response <strong>of</strong> PMTs can also<br />

depend on which region <strong>of</strong> the photocathode is illuminated.<br />

Color effects are almost nonexistent in MCP PMTs 80 and do<br />

not appear to be a problem with the compact PMTs.<br />

Methods are available to correct for such color effects.<br />

There are two general approaches, one <strong>of</strong> which is to use a<br />

standard with a very short lifetime. 112–113 The standard<br />

should emit at the wavelength used to measure the sample.<br />

Because <strong>of</strong> the short decay time one assumes that the measured<br />

response is the instrument response function. Because

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