2011
DOI: 10.1088/0004-637x/743/1/94
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OBSERVATIONS OF Arp 220 USINGHERSCHEL-SPIRE: AN UNPRECEDENTED VIEW OF THE MOLECULAR GAS IN AN EXTREME STAR FORMATION ENVIRONMENT

Abstract: We present Herschel SPIRE-FTS observations of Arp 220, a nearby ultraluminous infrared galaxy. The FTS provides continuous spectral coverage from 1 The SPIRE beam shapes are not gaussian; the effective beam solid angle can be found in the Herschel Observer's manual.

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Cited by 266 publications
(494 citation statements)
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References 95 publications
(89 reference statements)
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“…A thorough investigation of the water emission in the HERUS sample is beyond the scope of the current work and will be reported on in a forthcoming paper; however, we note that our measured fluxes for the water lines in Mrk 231 and Arp 220 are consistent within the errors with the results of González-Alfonso et al (2010. Finally, in addition to the above species, we also detect HCO + /HOC + (6−5) at 537 GHz (557 μm) in IRAS 13120 −5453, and confirm the detection of both HCO + /HOC + and HCN at 532 GHz (562 μm) in Arp 220 Rangwala et al (2011). In Table 4 the water line fluxes as measured by the SPIRE FTS for the HERUS local ULIRGs are tabulated in units of 10 −18 Wm −2 .…”
Section: Fitted Spectrasupporting
confidence: 90%
See 1 more Smart Citation
“…A thorough investigation of the water emission in the HERUS sample is beyond the scope of the current work and will be reported on in a forthcoming paper; however, we note that our measured fluxes for the water lines in Mrk 231 and Arp 220 are consistent within the errors with the results of González-Alfonso et al (2010. Finally, in addition to the above species, we also detect HCO + /HOC + (6−5) at 537 GHz (557 μm) in IRAS 13120 −5453, and confirm the detection of both HCO + /HOC + and HCN at 532 GHz (562 μm) in Arp 220 Rangwala et al (2011). In Table 4 the water line fluxes as measured by the SPIRE FTS for the HERUS local ULIRGs are tabulated in units of 10 −18 Wm −2 .…”
Section: Fitted Spectrasupporting
confidence: 90%
“…The [N II] line is indicative of hot HII regions rather than the PDR and can be used to estimate the fraction of [C II] emission that comes from ionized gas, rather than from PDRs. In many cases, the [N II] line is partially resolved and relatively broad (see Figure 9) and a sinc-Gauss profile was used to model the line in many instances where FWHM of ∼300-400 km −1 were measured, Although broad, these widths are still significantly smaller than those in systems that unambiguously are shown to have massive outflows (e.g., Feruglio et al 2010;Cicone et al 2014) Water is the second most oxygenated molecule (following CO) in the warm interstellar medium of galaxies and has been detected by Herschel in observations of nearby ULIRGs (González-Alfonso et al 2010;Rangwala et al 2011;PereiraSantaella et al 2013). The HERUS ULIRGs are also found to be abundant in water lines, in particular the ortho-H 2 O lines, IRAS 23230-6926, IRAS 06206-6315), and where the water lines, although detected, are significantly weaker than the CO lines (IRAS 09022-3615, IRAS 10565+2448, NGC 6240).…”
Section: Fitted Spectramentioning
confidence: 99%
“…The optical depth is τ(ν) is defined by τ(ν) = κ ν Σ dust and is commonly represented as τ(ν) = (ν/ν 0 ) β , where β is the spectral emissivity index and ν 0 is the frequency where optical depth equals unity (Draine, 2006), often assumed as = 3 THz from laboratory experiments (≈100µm) although the measured value from a number of galaxies tends more towards 1.5 THz (≈200µm Conley et al, 2011;Rangwala et al, 2011). The dust mass absorption coefficient has an identical frequency dependence, κ ν = κ 0 (ν/ν 0 ) β , since τ ≡ κΣ dust .…”
Section: Direct Modified Blackbody Sed Modelingmentioning
confidence: 99%
“…The , as well as a decrease with FIR color in star-forming galaxies (Malhotra et al 2001). Several hypotheses to explain the apparent line deficit in galaxies include (1) more dust screening at high ionization parameter (Luhman et al 2003;Abel et al 2009); (2) lower photoelectric efficiency due to charged small dust grains under intense radiation fields (Malhotra et al 2001;Croxall et al 2012); (3) lower photoelectric efficiency due to a decrease in the PAH abundance under hard radiation fields (Madden et al 2006;Rubin et al 2009); and (4) large dust optical depths leading to extinction of the emission lines (Papadopoulos et al 2010;Rangwala et al 2011). The dwarf galaxies extend the relative importance of the gas cooling to high values.…”
Section: Interpretation Of the [C Ii]/l Tir And [O I]/l Tir Trendsmentioning
confidence: 99%