The Carriers of the "Unidentified" Infrared Emission Features: Clues from Polycyclic Aromatic Hydrocarbons with Aliphatic Sidegroups

Abstract

The "unidentified" infrared emission (UIE) features at 3.3, 6.2, 7.7, 8.6, and 11.3 μm are ubiquitously seen in various astrophysical regions. The UIE features are characteristic of the stretching and bending vibrations of aromatic hydrocarbons. The 3.3 μm feature resulting from aromatic C--H stretches is often accompanied by a weaker feature at 3.4 μm often attributed to aliphatic C--H stretches. The ratio of the observed intensity of the 3.3 μm aromatic C--H feature (I3.3) to that of the 3.4 μm aliphatic C--H feature (I3.4) allows one to estimate the aliphatic fraction (i.e. N C,aliph/N C,arom, the number of C atoms in aliphatic units to that in aromatic rings) of the UIE carriers, provided the intrinsic oscillator strengths of the 3.3 μm aromatic C--H stretch (A3.3) and the 3.4 μm aliphatic C--H stretch (A3.4) are known. In this article we summarize the computational results on A3.3 and A3.4 and their implications for the aromaticity and aliphaticity of the UIE carriers. We use density functional theory and second-order perturbation theory to derive A3.3 and A3.4 from the infrared vibrational spectra of seven PAHs with various aliphatic substituents (e.g., methyl-, dimethyl-, ethyl-, propyl-, butyl-PAHs, and PAHs with unsaturated alkyl-chains). The mean band strengths of the aromatic (A3.3) and aliphatic (A3.4) C--H stretches are derived and then employed to estimate the aliphatic fraction of the UIE carriers by comparing A3.4/A3.3 with I3.4/I3.3. We conclude that the UIE emitters are predominantly aromatic, as revealed by the observationally-derived ratio <I3.4/I3.3> ~ 0.12 and the computationally-derived ratio <A3.4/A3.3> ~ 1.76 which suggest an upper limit of N C,aliph/N C,arom ~ 0.02 for the aliphatic fraction of the UIE carriers.

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