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Efstathiou, Andreas
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Preferred name
Efstathiou, Andreas
Translated Name
Ευσταθίου, Ανδρέας
Position
Rector, Professor
Main Affiliation
School
Scopus Author ID
7005273826
Google Scholar ID
WxhQowAAAAJ
2 results
Now showing 1 - 2 of 2
- PublicationFar-infrared fine-structure line diagnostics of ultraluminous infrared galaxies(Institute of Physics Publishing, 2013-10-10)
; ;D. Farrah ;V. Lebouteiller ;H. W. W. Spoon ;J. Bernard-Salas ;C. Pearson ;D. Rigopoulou ;H. A. Smith ;E. González-Alfonso ;D. L. Clements ;D. Cormier ;J. Afonso ;S. M. Petty ;K. Harris ;P. Hurley ;C. Borys ;A. Verma ;A. CoorayV. SalvatelliWe present Herschel observations of 6 fine-structure lines in 25 ultraluminous infrared galaxies at z < 0.27. The lines, [O III]52 μm, [N III]57 μm, [O I]63 μm, [N II]122 μm, [O I]145 μm, and [C II]158 μm, are mostly single Gaussians with widths <600 km s-1 and luminosities of 107-109 LO. There are deficits in the [O I]63/L IR, [N II]/L IR, [O I]145/L IR, and [C II]/L IR ratios compared to lower luminosity systems. The majority of the line deficits are consistent with dustier H II regions, but part of the [C II] deficit may arise from an additional mechanism, plausibly charged dust grains. This is consistent with some of the [C II] originating from photodissociation regions or the interstellar medium (ISM). We derive relations between far-IR line luminosities and both the IR luminosity and star formation rate. We find that [N II] and both [O I] lines are good tracers of the IR luminosity and star formation rate. In contrast, [C II] is a poor tracer of the IR luminosity and star formation rate, and does not improve as a tracer of either quantity if the [C II] deficit is accounted for. The continuum luminosity densities also correlate with the IR luminosity and star formation rate. We derive ranges for the gas density and ultraviolet radiation intensity of 101 < n < 102.5 and 102.2 < G 0 < 103.6, respectively. These ranges depend on optical type, the importance of star formation, and merger stage. We do not find relationships between far-IR line properties and several other parameters: active galactic nucleus (AGN) activity, merger stage, mid-IR excitation, and SMBH mass. We conclude that these far-IR lines arise from gas heated by starlight, and that they are not strongly influenced by AGN activity - PublicationHerMES: Spectral energy distributions of submillimeter galaxies at z > 4*(Institute of Physics Publishing, 2014-03-20)
; ;J.-S. Huang ;D. Rigopoulou ;G. Magdis ;M. Rowan-Robinson ;Y. Dai ;J. J. Bock ;D. Burgarella ;S. Chapman ;D. L. Clements ;A. Cooray ;D. Farrah ;J. Glenn ;S. Oliver ;A. J. Smith ;L. Wang ;M. Page ;D. Riechers ;I. Roseboom ;M. Symeonidis ;G. G. Fazio ;M. YunT. M. A. WebbWe present a study of the infrared properties for a sample of seven spectroscopically confirmed submillimeter galaxies (SMGs) at z > 4.0. By combining ground-based near-infrared, Spitzer IRAC and MIPS, Herschel SPIRE, and ground-based submillimeter/millimeter photometry, we construct their spectral energy distributions (SEDs) and a composite model to fit the SEDs. The model includes a stellar emission component at λrest < 3.5 μm, a hot dust component peaking at λrest ∼ 5 μm, and cold dust component which becomes significant for λrest > 50 μm. Six objects in the sample are detected at 250 and 350 μm. The dust temperatures for the sources in this sample are in the range of 40-80 K, and their LFIR ∼ 1013 L⊙ qualifies them as hyper-luminous infrared galaxies. The mean FIR-radio index for this sample is around 〈q〉 = 2.2 indicating no radio excess in their radio emission. Most sources in the sample have 24 μm detections corresponding to a rest-frame 4.5 μm luminosity of Log10(L4.5/L ⊙) = 11 ∼ 11.5. Their L4.5/LFIR ratios are very similar to those of starburst-dominated SMGs at z ∼ 2. The L CO-LFIR relation for this sample is consistent with that determined for local ULIRGs and SMGs at z ∼ 2. We conclude that SMGs at z > 4 are hotter and more luminous in the FIR but otherwise very similar to those at z ∼ 2. None of these sources show any sign of the strong QSO phase being triggered.