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Living Image 3.1

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F. Fluorescent Imaging<br />

Specifying Signal<br />

Levels and f/stop<br />

Settings<br />

F.4 <strong>Image</strong> Data Display<br />

214<br />

Figure F.6 Illustration of the in vivo fluorescence process.<br />

At 600-900 nm, light transmission through tissue is highest and the generation of<br />

autofluorescence is lower. Therefore it is important to select fluorophores that are active<br />

in the 600-900 nm range. Fluorophores such as GFP that are active in the 450-600 nm<br />

range will still work, but the depth of detection may be limited to within several<br />

millimeters of the surface.<br />

Fluorescent signals are usually brighter than bioluminescent signals, so imaging times are<br />

shorter, typically from one to 30 seconds. The bright signal enables a lower binning level<br />

that produces better spatial resolution. Further, the f/stop can often be set to higher values;<br />

f/2 or f/4 is recommended for fluorescence imaging. A higher f/stop improves the depth<br />

of field, yielding a sharper image. For more details on the f/stop, see Lens Aperture,<br />

page 191.<br />

Fluorescent image data can be displayed in units of counts or photons (absolute,<br />

calibrated), or in terms of efficiency (calibrated, normalized). For more details, see<br />

Quantifying <strong>Image</strong> Data, page 199.<br />

If the image is displayed in photons, you can compare images with different exposure<br />

times, f/stop setting, or binning level. When an image is displayed in terms of efficiency,<br />

the fluorescent image is normalized against a stored reference image of the excitation light<br />

intensity. Efficiency image data is without units and represents the ratio of emitted light<br />

to incident light. For more details on efficiency, see page 201.<br />

Fluorescent Efficiency The detected fluorescent signal depends on the amount of fluorophore present in the<br />

sample and the intensity of the incident excitation light. At the sample stage, the incident<br />

excitation light is not uniform over the FOV. It peaks at the center of the FOV and drops<br />

of slowly toward the edges (Figure F.7). To eliminate the excitation light as a variable from<br />

the measurement, the data can be displayed in terms of efficiency (Figure F.8).

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