TY - JOUR
T1 - Gas and dust cooling along the major axis of M 33 (HerM33es). Herschel/PACS [C II] and [O I] observations
AU - Kramer, Carsten
AU - Nikola, Thomas
AU - Anderl, Sibylle
AU - Bertoldi, Frank
AU - Boquien, Médéric
AU - Braine, Jonathan
AU - Buchbender, Christof
AU - Combes, Françoise
AU - Henkel, Christian
AU - Hermelo, Israel
AU - Israel, Frank
AU - Relaño, Monica
AU - Röllig, Markus
AU - Schuster, Karl
AU - Tabatabaei, Fatemeh
AU - van der Tak, Floris
AU - Verley, Simon
AU - van der Werf, Paul
AU - Wiedner, Martina
AU - Xilouris, Emmanuel M.
PY - 2020/7/1
Y1 - 2020/7/1
N2 - Context. M 33 is a gas rich spiral galaxy of the Local Group. Its
vicinity allows us to study its interstellar medium (ISM) on linear
scales corresponding to the sizes of individual giant molecular clouds.
Aims: We investigate the relationship between the two major gas
cooling lines and the total infrared (TIR) dust continuum.
Methods: We mapped the emission of gas and dust in M 33 using the
far-infrared lines of [C II] and [O I](63 μm) and the total infrared
continuum. The line maps were observed with the PACS spectrometer on
board the Herschel Space Observatory. These maps have 50 pc resolution
and form a ∼370 pc wide stripe along its major axis covering the
sites of bright H II regions, but also more quiescent arm and inter-arm
regions from the southern arm at 2 kpc galacto-centric distance to the
south out to 5.7 kpc distance to the north. Full-galaxy maps of the
continuum emission at 24 μm from Spitzer/MIPS, and at 70 μm, 100
μm, and 160 μm from Herschel/PACS were combined to obtain a map of
the TIR. Results: TIR and [C II] intensities are correlated over
more than two orders of magnitude. The range of TIR translates to a
range of far ultraviolet (FUV) emission of G0, obs ∼ 2 to
200 in units of the average Galactic radiation field. The binned [C
II]/TIR ratio drops with rising TIR, with large, but decreasing scatter.
The contribution of the cold neutral medium to the [C II] emission, as
estimated from VLA H I data, is on average only 10%. Fits of modified
black bodies to the continuum emission were used to estimate dust mass
surface densities and total gas column densities. A correction for
possible foreground absorption by cold gas was applied to the [O I] data
before comparing it with models of photon dominated regions. Most of the
ratios of [C II]/[O I] and ([C II]+[O I])/TIR are consistent with two
model solutions. The median ratios are consistent with one solution at n
∼ 2 × 102 cm-3, G0 ∼ 60,
and a second low-FUV solution at n ∼ 104 cm-3,
G0 ∼ 1.5. Conclusions: The bulk of the gas along
the lines-of-sight is represented by a low-density, high-FUV phase with
low beam filling factors ∼1. A fraction of the gas may, however, be
represented by the second solution.
Maps of TIR, [C II], [O I] shown in Figs. 2 and 3 are only available at
the CDS via anonymous ftp to http://cdsarc.u-strasbg.fr
(ftp://130.79.128.5) or via http://cdsarc.u-strasbg.fr/viz-bin/cat/J/A+A/639/A61
Herschel is an ESA space observatory with science instruments provided
by European-led Principal Investigator consortia and with important
participation from NASA.
AB - Context. M 33 is a gas rich spiral galaxy of the Local Group. Its
vicinity allows us to study its interstellar medium (ISM) on linear
scales corresponding to the sizes of individual giant molecular clouds.
Aims: We investigate the relationship between the two major gas
cooling lines and the total infrared (TIR) dust continuum.
Methods: We mapped the emission of gas and dust in M 33 using the
far-infrared lines of [C II] and [O I](63 μm) and the total infrared
continuum. The line maps were observed with the PACS spectrometer on
board the Herschel Space Observatory. These maps have 50 pc resolution
and form a ∼370 pc wide stripe along its major axis covering the
sites of bright H II regions, but also more quiescent arm and inter-arm
regions from the southern arm at 2 kpc galacto-centric distance to the
south out to 5.7 kpc distance to the north. Full-galaxy maps of the
continuum emission at 24 μm from Spitzer/MIPS, and at 70 μm, 100
μm, and 160 μm from Herschel/PACS were combined to obtain a map of
the TIR. Results: TIR and [C II] intensities are correlated over
more than two orders of magnitude. The range of TIR translates to a
range of far ultraviolet (FUV) emission of G0, obs ∼ 2 to
200 in units of the average Galactic radiation field. The binned [C
II]/TIR ratio drops with rising TIR, with large, but decreasing scatter.
The contribution of the cold neutral medium to the [C II] emission, as
estimated from VLA H I data, is on average only 10%. Fits of modified
black bodies to the continuum emission were used to estimate dust mass
surface densities and total gas column densities. A correction for
possible foreground absorption by cold gas was applied to the [O I] data
before comparing it with models of photon dominated regions. Most of the
ratios of [C II]/[O I] and ([C II]+[O I])/TIR are consistent with two
model solutions. The median ratios are consistent with one solution at n
∼ 2 × 102 cm-3, G0 ∼ 60,
and a second low-FUV solution at n ∼ 104 cm-3,
G0 ∼ 1.5. Conclusions: The bulk of the gas along
the lines-of-sight is represented by a low-density, high-FUV phase with
low beam filling factors ∼1. A fraction of the gas may, however, be
represented by the second solution.
Maps of TIR, [C II], [O I] shown in Figs. 2 and 3 are only available at
the CDS via anonymous ftp to http://cdsarc.u-strasbg.fr
(ftp://130.79.128.5) or via http://cdsarc.u-strasbg.fr/viz-bin/cat/J/A+A/639/A61
Herschel is an ESA space observatory with science instruments provided
by European-led Principal Investigator consortia and with important
participation from NASA.
KW - galaxies: ISM
KW - galaxies: individual: M 33
KW - infrared: galaxies
KW - infrared: ISM
U2 - 10.1051/0004-6361/201936754
DO - 10.1051/0004-6361/201936754
M3 - Article
SN - 0004-6361
VL - 639
JO - Astronomy & Astrophysics
JF - Astronomy & Astrophysics
M1 - A61
ER -