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Hans Publishers, Astronomy & Astrophysics, (578), p. A53

DOI: 10.1051/0004-6361/201425207

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TheHerschelDwarf Galaxy Survey

This paper was not found in any repository, but could be made available legally by the author.
This paper was not found in any repository, but could be made available legally by the author.

Full text: Unavailable

Red circle
Preprint: archiving forbidden
Red circle
Postprint: archiving forbidden
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Published version: archiving forbidden
Data provided by SHERPA/RoMEO

Abstract

Context. The far-infrared (FIR) lines are important tracers of the cooling and physical conditions of the interstellar medium (ISM) and are rapidly becoming workhorse diagnostics for galaxies throughout the universe. There are clear indications of a different behavior of these lines at low metallicity that needs to be explored. Aims. Our goal is to explain the main differences and trends observed in the FIR line emission of dwarf galaxies compared to more metal-rich galaxies, and how this translates in ISM properties. Methods. We present Herschel/PACS spectroscopic observations of the [C II] 157 μm, [O I] 63 and 145 μm, [O III] 88 μm, [N II] 122 and 205 μm, and [N III] 57 μm fine-structure cooling lines in a sample of 48 low-metallicity star-forming galaxies of the guaranteed time key program Dwarf Galaxy Survey. We correlate PACS line ratios and line-to-L_(TIR) ratios with L_(TIR), L_(TIR)/L_B, metallicity, and FIR color, and interpret the observed trends in terms of ISM conditions and phase filling factors with Cloudy radiative transfer models. Results. We find that the FIR lines together account for up to 3 percent of L_(TIR) and that star-forming regions dominate the overall emission in dwarf galaxies. Compared to metal-rich galaxies, the ratios of [O III]_(88)/[N II]_(122) and [N III]_(57)/[N II]_(122) are high, indicative of hard radiation fields. In the photodissociation region (PDR), the [C II]_(157)/[O I]_(63) ratio is slightly higher than in metal-rich galaxies, with a small increase with metallicity, and the [O I]_(145)/[O I]_(63) ratio is generally lower than 0.1, demonstrating that optical depth effects should be small on the scales probed. The [O III]_(88)/[O I]_(63) ratio can be used as an indicator of the ionized gas/PDR filling factor, and is found to be ~4 times higher in the dwarfs than in metal-rich galaxies. The high [C II]/L_(TIR), [O I]/L_(TIR), and [O III]/L_(TIR) ratios, which decrease with increasing L_(TIR) and L_(TIR)/L_B, are interpreted as a combination of moderate far-UV fields and a low PDR covering factor. Harboring compact phases of a low filling factor and a large volume filling factor of diffuse gas, the ISM of low-metallicity dwarf galaxies has a more porous structure than that of metal-rich galaxies.