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The Far-Infrared Spectrum of Arp 220*

Eduardo González-Alfonso et al 2004 ApJ 613 247-261   doi: 10.1086/422868  Help

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Eduardo González-Alfonso1,4,5, Howard A. Smith2, Jacqueline Fischer3 and José Cernicharo4
1 Universidad de Alcalá de Henares, Departamento de Física, Campus Universitario, E-28871 Alcalá de Henares, Madrid, Spain
2 Harvard-Smithsonian Center for Astrophysics, 60 Garden Street, Cambridge, MA 02138
3 Naval Research Laboratory, Remote Sensing Division, Code 7213, Washington, DC 20375
4 CSIC, IEM, Departamento Astrofísica Molecular e Infrarroja, Serrano 123, E-28006 Madrid, Spain
5 Visiting Astronomer, Harvard-Smithsonian Center for Astrophysics, 60 Garden Street, Cambridge, MA 02138
E-mail: eduardo.gonzalez@uah.es, hsmith@cfa.harvard.edu, jackie.fischer@nrl.navy.mil and cerni@damir.iem.csic.es

ABSTRACT. Infrared Space Observatory Long Wavelength Spectrometer grating observations of the ultraluminous infrared galaxy Arp 220 shows absorption in molecular lines of OH, H2O, CH, NH, and NH3, as well as in the [O I] 63 μm line and emission in the [C II] 158 μm line. We have modeled the continuum and the emission/absorption of all observed features by means of a nonlocal radiative transfer code. The continuum from 25 to 1300 μm is modeled as a warm (106 K) nuclear region that is optically thick in the far-infrared, attenuated by an extended region (2'') that is heated mainly through absorption of nuclear infrared radiation. The molecular absorption in the nuclear region is characterized by high excitation due to the high-infrared radiation density. The OH column densities are high toward the nucleus (2-6 × 1017 cm-2) and the extended region (~2 × 1017 cm-2). The H2O column density is also high toward the nucleus (2-10 × 1017 cm-2) and lower in the extended region. The column densities in a halo that accounts for the absorption in the lowest lying lines are similar to what are found in the diffuse clouds toward the star-forming regions in the Sgr B2 molecular cloud complex near the Galactic center. Most notable are the high column densities found for NH and NH3 toward the nucleus, with values of ~1.5 × 1016 cm-2 and ~3 × 1016 cm-2, respectively, whereas the NH2 column density is lower than ~2 × 1015 cm-2. A combination of photodissociation regions (PDRs) in the extended region and hot cores with enhanced H2O photodissociation and a possible shock contribution in the nuclei may explain the relative column densities of OH and H2O, whereas the nitrogen chemistry may be strongly affected by cosmic-ray ionization. The [C II] 158 μm line is well reproduced by our models and its "deficit" relative to the C II/far-IR ratio in normal and starburst galaxies is suggested to be mainly a consequence of the dominant non-PDR component of far-infrared radiation, although our models alone cannot rule out extinction effects in the nuclei.

Subject headings: galaxies: abundances; galaxies: individual (Arp 220); galaxies: ISM; galaxies: starburst; infrared: galaxies; radiative transfer

* Based on observations with the Infrared Space Observatory, an ESA project with instruments funded by ESA Member States (especially the principal investigator countries: France, Germany, Netherlands, and the United Kingdom) and with the participation of ISAS and NASA.

Print publication: Issue 1 (2004 September 20)
Received 2004 February 27, accepted for publication 2004 May 27

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