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TRACING ABUNDANCES IN GALAXIES WITH THE SPITZER ...

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Figure 1.8 Example structures of PAH molecules following Allamandola et al.<br />

(1989). The vertices of the hexagons represent carbon atoms.<br />

When a PAH molecule absorbs an energetic (UV or optical) photon, it quickly<br />

(∼10 −12 –10 −10 s) redistributes the energy over the vibrational modes of the PAH,<br />

and then the PAH relaxes to the ground state by emitting IR photons over the<br />

next seconds to hours, producing features such as the ones found at 6.2, 7.7, 8.6,<br />

11.2, and 12.7 µm (Draine & Li, 2001; Li & Draine, 2002). A C–C stretching mode<br />

produces the 6.2 and 7.7 µm features, a C–H in-plane bending mode causes the<br />

8.6 µm feature, and C–H out-of-plane bending gives rise to the 11.2 and 12.7 µm<br />

features. PAHs with sizes between twenty and forty carbon atoms are probably<br />

the dominant emitters of these features (Allamandola et al., 1989). The type of<br />

PAHs formed gives indications about the material from which they were made as<br />

well as their thermal history (Leger et al., 1987).<br />

1.5 Observing with the Spitzer Space Telescope<br />

This dissertation employs infrared data from the Spitzer Space Telescope. It has an<br />

85 cm diameter and was launched August 25, 2003 and is expected to have a ∼5+<br />

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