Herschel-SPIRE Fourier transform spectroscopy of the nearby spiral galaxy IC 342

We present observations of the nearby spiral galaxy IC 342 with the Herschel Spectral and Photometric Imaging Receiver (SPIRE) Fourier transform spectrometer. The spectral range afforded by SPIRE, 196-671 μm, allows us to access a number of 12CO lines from J = 4-3 to J = 13-12 with the highest J tra...

Full description

Bibliographic Details
Main Authors: Rigopoulou, D, Hurley, P, Swinyard, B, Virdee, J, Croxall, K, Hopwood, R, Lim, T, Magdis, G, Pearson, C, Pellegrini, E, Polehampton, E, Smith, J
Format: Journal article
Language:English
Published: 2013
_version_ 1826299337763717120
author Rigopoulou, D
Hurley, P
Swinyard, B
Virdee, J
Croxall, K
Hopwood, R
Lim, T
Magdis, G
Pearson, C
Pellegrini, E
Polehampton, E
Smith, J
author_facet Rigopoulou, D
Hurley, P
Swinyard, B
Virdee, J
Croxall, K
Hopwood, R
Lim, T
Magdis, G
Pearson, C
Pellegrini, E
Polehampton, E
Smith, J
author_sort Rigopoulou, D
collection OXFORD
description We present observations of the nearby spiral galaxy IC 342 with the Herschel Spectral and Photometric Imaging Receiver (SPIRE) Fourier transform spectrometer. The spectral range afforded by SPIRE, 196-671 μm, allows us to access a number of 12CO lines from J = 4-3 to J = 13-12 with the highest J transitions observed for the first time. In addition we present measurements of 13CO, [CI] and [N II].We use a radiative transfer code coupled with Bayesian likelihood analysis to model and constrain the temperature, density and column density of the gas. We find two 12CO components, one at 35K and one at 400K with CO column densities of 6.3 × 1017 and 0.4 × 1017 cm-2 and CO gas masses of 1.26 × 107 and 0.15 × 107M⊙ for the cold and warm components, respectively. The inclusion of the high-J 12CO line observations indicate the existence of a much warmer gas component (~400 K) confirming earlier findings from H2 rotational line analysis from Infrared Space Observatory and Spitzer. The mass of the warm gas is 10 per cent of the cold gas, but it likely dominates the CO luminosity. In addition, we detect strong emission from [N II] 205 μm and the 13P1 → 13P0 and 13P2 → 3P1 [C I] lines at 370 and 608 μm, respectively. The measured 12CO line ratios can be explained by photon-dominated region (PDR) models although additional heating by e.g. cosmic rays cannot be excluded. The measured [C I] line ratio together with the derived [C] column density of 2.1 × 1017 cm-2 and the fact that [C I] is weaker than CO emission in IC 342 suggests that [C I] likely arises in a thin layer on the outside of the CO emitting molecular clouds consistent with PDRs playing an important role. © 2013 The Authors. Published by Oxford University Press on behalf of the Royal Astronomical Society.
first_indexed 2024-03-07T05:00:24Z
format Journal article
id oxford-uuid:d81339da-77dc-469c-9b41-ee9cf9cfb1fb
institution University of Oxford
language English
last_indexed 2024-03-07T05:00:24Z
publishDate 2013
record_format dspace
spelling oxford-uuid:d81339da-77dc-469c-9b41-ee9cf9cfb1fb2022-03-27T08:45:46ZHerschel-SPIRE Fourier transform spectroscopy of the nearby spiral galaxy IC 342Journal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:d81339da-77dc-469c-9b41-ee9cf9cfb1fbEnglishSymplectic Elements at Oxford2013Rigopoulou, DHurley, PSwinyard, BVirdee, JCroxall, KHopwood, RLim, TMagdis, GPearson, CPellegrini, EPolehampton, ESmith, JWe present observations of the nearby spiral galaxy IC 342 with the Herschel Spectral and Photometric Imaging Receiver (SPIRE) Fourier transform spectrometer. The spectral range afforded by SPIRE, 196-671 μm, allows us to access a number of 12CO lines from J = 4-3 to J = 13-12 with the highest J transitions observed for the first time. In addition we present measurements of 13CO, [CI] and [N II].We use a radiative transfer code coupled with Bayesian likelihood analysis to model and constrain the temperature, density and column density of the gas. We find two 12CO components, one at 35K and one at 400K with CO column densities of 6.3 × 1017 and 0.4 × 1017 cm-2 and CO gas masses of 1.26 × 107 and 0.15 × 107M⊙ for the cold and warm components, respectively. The inclusion of the high-J 12CO line observations indicate the existence of a much warmer gas component (~400 K) confirming earlier findings from H2 rotational line analysis from Infrared Space Observatory and Spitzer. The mass of the warm gas is 10 per cent of the cold gas, but it likely dominates the CO luminosity. In addition, we detect strong emission from [N II] 205 μm and the 13P1 → 13P0 and 13P2 → 3P1 [C I] lines at 370 and 608 μm, respectively. The measured 12CO line ratios can be explained by photon-dominated region (PDR) models although additional heating by e.g. cosmic rays cannot be excluded. The measured [C I] line ratio together with the derived [C] column density of 2.1 × 1017 cm-2 and the fact that [C I] is weaker than CO emission in IC 342 suggests that [C I] likely arises in a thin layer on the outside of the CO emitting molecular clouds consistent with PDRs playing an important role. © 2013 The Authors. Published by Oxford University Press on behalf of the Royal Astronomical Society.
spellingShingle Rigopoulou, D
Hurley, P
Swinyard, B
Virdee, J
Croxall, K
Hopwood, R
Lim, T
Magdis, G
Pearson, C
Pellegrini, E
Polehampton, E
Smith, J
Herschel-SPIRE Fourier transform spectroscopy of the nearby spiral galaxy IC 342
title Herschel-SPIRE Fourier transform spectroscopy of the nearby spiral galaxy IC 342
title_full Herschel-SPIRE Fourier transform spectroscopy of the nearby spiral galaxy IC 342
title_fullStr Herschel-SPIRE Fourier transform spectroscopy of the nearby spiral galaxy IC 342
title_full_unstemmed Herschel-SPIRE Fourier transform spectroscopy of the nearby spiral galaxy IC 342
title_short Herschel-SPIRE Fourier transform spectroscopy of the nearby spiral galaxy IC 342
title_sort herschel spire fourier transform spectroscopy of the nearby spiral galaxy ic 342
work_keys_str_mv AT rigopouloud herschelspirefouriertransformspectroscopyofthenearbyspiralgalaxyic342
AT hurleyp herschelspirefouriertransformspectroscopyofthenearbyspiralgalaxyic342
AT swinyardb herschelspirefouriertransformspectroscopyofthenearbyspiralgalaxyic342
AT virdeej herschelspirefouriertransformspectroscopyofthenearbyspiralgalaxyic342
AT croxallk herschelspirefouriertransformspectroscopyofthenearbyspiralgalaxyic342
AT hopwoodr herschelspirefouriertransformspectroscopyofthenearbyspiralgalaxyic342
AT limt herschelspirefouriertransformspectroscopyofthenearbyspiralgalaxyic342
AT magdisg herschelspirefouriertransformspectroscopyofthenearbyspiralgalaxyic342
AT pearsonc herschelspirefouriertransformspectroscopyofthenearbyspiralgalaxyic342
AT pellegrinie herschelspirefouriertransformspectroscopyofthenearbyspiralgalaxyic342
AT polehamptone herschelspirefouriertransformspectroscopyofthenearbyspiralgalaxyic342
AT smithj herschelspirefouriertransformspectroscopyofthenearbyspiralgalaxyic342