22.07.2013 Views

Principles of Fluorescence Spectroscopy

Principles of Fluorescence Spectroscopy

Principles of Fluorescence Spectroscopy

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

PRINCIPLES OF FLUORESCENCE SPECTROSCOPY 145<br />

Figure 4.56. Global lifetime χ R 2 surface for the three-component mixture<br />

<strong>of</strong> In, AA, and 2-AP. From [187].<br />

length global analysis the uncertainties are significant. For<br />

instance, the value <strong>of</strong> the 4.1-ns lifetime can range from<br />

about 3.2 to 5.5 ns and still be consistent with the data.<br />

4.13. APPLICATIONS OF TCSPC<br />

The concepts described in the preceding sections can be<br />

made more understandable by examination <strong>of</strong> some specific<br />

examples.<br />

4.13.1. Intensity Decay for a Single Tryptophan<br />

Protein<br />

The tet repressor controls the gene in Gram-negative bacteria<br />

that provides resistance to the antibiotic tetracycline. 206<br />

This protein usually contains two tryptophans, but a mutant<br />

protein was engineered that contains a single tryptophan<br />

residue at position 43. Intensity decays are shown in Figure<br />

4.57. The light source was a frequency-doubled R6G dye<br />

laser at 590 nm, frequency doubled to 295 nm. The dye<br />

laser was cavity dumped at 80 kHz. The excitation was vertically<br />

polarized and the emission detected through a polarizer<br />

set 54.7E from the vertical. The use <strong>of</strong> magic-angle<br />

polarization conditions is essential in this case because the<br />

protein can be expected to rotate on a timescale comparable<br />

to the intensity decay. A Schott WG 320 filter was used in<br />

front <strong>of</strong> the monochromator to prevent scattered light from<br />

entering the monochromator, which was set at 360 nm.<br />

The emission was detected with an XP-2020 PMT.<br />

This PMT shows a wavelength-dependent time response<br />

and an afterpulse. To avoid color effects the authors used a<br />

Figure 4.57. Intensity decay <strong>of</strong> trp-43 in the tet repressor protein F75<br />

TetR at 360 nm. The calibration is 108 ps/channel. Revised and<br />

reprinted with permission from [206]. Copyright © 1992, American<br />

Chemical Society.<br />

short-lifetime reference that shifted the wavelength to the<br />

measurement wavelength with minimal time delay. 112 This<br />

was accomplished with a solution <strong>of</strong> p-terphenyl highly<br />

quenched by CCl 4 . The fact that the measurements were<br />

performed with a dynode PMT is evident from the width <strong>of</strong><br />

the impulse response function, which appears to be near<br />

500 ps. Some <strong>of</strong> this width may be contributed from the<br />

short lifetime standard.<br />

The intensity decay was fit to the one, two, and three<br />

exponential models, resulting in χ R 2 values <strong>of</strong> 17, 1.6, and<br />

1.5, respectively. Rejection <strong>of</strong> the single-exponential model<br />

is clearly justified by the data. However, it is less clear that<br />

three decay times are needed. The ratio <strong>of</strong> the χ R 2 values is<br />

1.07, which is attributed to random error with a probability<br />

<strong>of</strong> over 20% (Table 4.3). The fractional amplitude <strong>of</strong> the<br />

third component was less than 1%, and the authors accepted<br />

the double exponential fit as descriptive <strong>of</strong> their protein.<br />

4.13.2. Green Fluorescent Protein:<br />

Systematic Errors in the Data<br />

Green fluorescent protein (GFP) spontaneously becomes<br />

fluorescent following synthesis <strong>of</strong> its amino-acid chain.

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!