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IRAC Instrument Handbook - IRSA - California Institute of Technology

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<strong>IRAC</strong> <strong>Instrument</strong> <strong>Handbook</strong><br />

Figure 2.10: <strong>IRAC</strong> point source sensitivity as a function <strong>of</strong> frame time, for high background. To convert to<br />

MJy/sr, see equation 2.8.<br />

In the sensitivity figures, the dashed line at 0.6 µJy is the confusion limit predicted by Franceschini et al.<br />

(1991, [10]). This does not represent a hard sensitivity limit, but rather indicates where source confusion<br />

affects reliability <strong>of</strong> source extractions for low background regions. Data from IOC/SV show noise<br />

decreasing as N to 0.25 µJy (channels 1 and 2) or 0.6 µJy (channels 3 and 4). Moderately deep source<br />

counts indicate that a source density equivalent to 36 beams/source is reached at 20.5 mag, or 1.8 and 1.1<br />

µJy at 3.6 and 4.5 µm, respectively (Fazio et al. 2004, [9]). The confusion estimates by Franceschini et<br />

al. and Fazio et al. are for low background, extragalactic observations only. For observations <strong>of</strong> higher<br />

background or more “cluttered” regions (such as the Galactic Plane) the confusion noise will be much<br />

more significant.<br />

For diffuse emission, the surface brightness sensitivity per pixel (in MJy/sr) is<br />

0.<br />

03 f<br />

f<br />

ex<br />

N<br />

p<br />

pix<br />

× the point source sensitivity [in µJy]. (2.8)<br />

<strong>Instrument</strong> Description 23 Sensitivity and Saturation

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