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INFRARED SPECTRA AND SPECTRAL ENERGY DISTRIBUTIONS FOR DUSTY STARBURSTS AND ACTIVE GALACTIC NUCLEI

Authors :
James R. Houck
Ashot Hovhannisyan
Areg M. Mickaelian
Daniel W. Weedman
Donald J. Barry
Vianney Lebouteiller
Lusine A. Sargsyan
Astrophysique Interprétation Modélisation (AIM (UMR_7158 / UMR_E_9005 / UM_112))
Centre National de la Recherche Scientifique (CNRS)-Institut national des sciences de l'Univers (INSU - CNRS)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris Diderot - Paris 7 (UPD7)
V.A. Ambartsumian Byurakan Astrophysical Observatory (BAO)
Astrophysique Interprétation Modélisation (AIM (UMR7158 / UMR_E_9005 / UM_112))
Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut national des sciences de l'Univers (INSU - CNRS)-Université Paris Diderot - Paris 7 (UPD7)-Centre National de la Recherche Scientifique (CNRS)
Source :
The Astrophysical Journal, The Astrophysical Journal, American Astronomical Society, 2011, 730 (1), pp.19. ⟨10.1088/0004-637X/730/1/19⟩, The Astrophysical Journal, 2011, 730 (1), pp.19. ⟨10.1088/0004-637X/730/1/19⟩
Publication Year :
2011
Publisher :
HAL CCSD, 2011.

Abstract

We present spectroscopic results for all galaxies observed with the Spitzer Infrared Spectrograph (IRS) that also have total infrared fluxes f IR measured with the Infrared Astronomical Satellite (IRAS), also using AKARI photometry when available. Infrared luminosities and spectral energy distributions (SEDs) from 8 μm to 160 μm are compared to polycyclic aromatic hydrocarbon emission from starburst galaxies or mid-infrared dust continuum from active galactic nuclei (AGNs) at rest-frame wavelengths ~8 μm. A total of 301 spectra are analyzed for which IRS and IRAS include the same unresolved source, as measured by the ratio f ν(IRAS 25 μm)/f ν(IRS 25 μm). Sources have 0.004 < z < 0.34 and 42.5 < log L IR < 46.8 (erg s–1) and cover the full range of starburst galaxy and AGN classifications. Individual spectra are provided electronically, but averages and dispersions are presented. We find that log [L IR/νL ν(7.7 μm)] = 0.74 ± 0.18 in starbursts, log [L IR/νL ν(7.7 μm)] = 0.96 ± 0.26 in composite sources (starburst plus AGN), log [L IR/νL ν(7.9 μm)] = 0.80 ± 0.25 in AGNs with silicate absorption, and that log [L IR/νL ν(7.9 μm)] = 0.51 ± 0.21 in AGNs with silicate emission. L IR for the most luminous absorption and emission AGNs are similar and 2.5 times larger than for the most luminous starbursts. AGNs have systematically flatter SEDs than starbursts or composites, but their dispersion in SEDs overlaps starbursts. Sources with the strongest far-infrared luminosity from cool dust components are composite sources, indicating that these sources may contain the most obscured starbursts.

Details

Language :
English
ISSN :
0004637X and 15384357
Database :
OpenAIRE
Journal :
The Astrophysical Journal, The Astrophysical Journal, American Astronomical Society, 2011, 730 (1), pp.19. ⟨10.1088/0004-637X/730/1/19⟩, The Astrophysical Journal, 2011, 730 (1), pp.19. ⟨10.1088/0004-637X/730/1/19⟩
Accession number :
edsair.doi.dedup.....dc44afdd131bc9a6329c4710b8475211