Published March 1, 2015 | Version v1
Journal article

ALMA reveals the molecular medium fueling the nearest nuclear starburst

  • 1. National Radio Astronomy Observatory, 520 Edgemont Road, Charlottesville, VA 22903 (United States)
  • 2. Department of Astronomy, Laboratory for Millimeter-Wave Astronomy and Joint Space Institute, University of Maryland, College Park, MD 20742 (United States)
  • 3. Department of Astrophysical Sciences, Princeton University, Princeton, NJ 08544 (United States)
  • 4. Department of Physics, University of Alberta, Edmonton, AB T6G 2R3 (Canada)
  • 5. Max Planck Institute für Astronomie, Königstuhl 17, D-69117 Heidelberg (Germany)
  • 6. New Mexico Institute of Mining and Technology, 801 Leroy Place, Socorro, NM 87801 (United States)
  • 7. National Radio Astronomy Observatory, P.O. Box O, 1003 Lopezville Road, Socorro, NM 87801 (United States)
  • 8. Steward Observatory, University of Arizona, 933 North Cherry Avenue, Tucson, AZ 85721 (United States)
  • 9. Max-Planck-Institut für Extraterrestrische Physik (MPE), Giessenbachstr., D-85748 Garching (Germany)
  • 10. European Southern Observatory, Karl-Schwarzschild-Strasse 2, D-85748 Garching (Germany)

Description

We use ALMA observations to derive mass, length, and time scales associated with NGC 253's nuclear starburst. This region forms ∼2 M ☉ yr–1 of stars and resembles other starbursts in ratios of gas, dense gas, and star formation tracers, with star formation consuming the gas reservoir at a normalized rate 10 times higher than in normal galaxy disks. We present new ∼35 pc resolution observations of bulk gas tracers (CO), high critical density transitions (HCN, HCO+, and CS), and their isotopologues. The starburst is fueled by a highly inclined distribution of dense gas with vertical extent <100 pc and radius ∼250 pc. Within this region, we identify 10 starburst giant molecular clouds (GMCs) that appear as both peaks in the dense gas tracer cubes and the HCN-to-CO ratio map. These are massive (∼107 M ☉) structures with sizes (∼30 pc) similar to GMCs in other systems, but compared to GMCs in normal galaxy disks, they have high line widths (σ ∼ 20-40 km s–1, Mach number M ∼ 90) and high surface and volume densities (Σmol ∼ 6000 M ☉ pc–2, n H2 ∼ 2000 cm–3). The self gravity from such high densities can explain the high line widths and the short free fall time τff ∼ 0.7 Myr in the clouds helps explain the more efficient star formation in NGC 253. Though the high inclination obscures the geometry somewhat, we show that simple models suggest a compact, clumpy region of high gas density embedded in a more extended, non-axisymmetric, bar-like distribution. Over the starburst, the surface density still exceeds that of a typical disk galaxy GMC and, as in the clouds, timescales in the disk as a whole are short compared to those in normal galaxy disks. The orbital time (∼10 Myr), disk free fall time (≲ 3 Myr), and disk crossing time (≲ 3 Myr) are each an order of magnitude shorter than in a normal galaxy disk. Finally, the CO-to-H2 conversion factor implied by our cloud calculations is approximately Galactic, contrasting with results showing a low value for the whole starburst region. The contrast provides resolved support for the idea of mixed molecular ISM phases in starburst galaxies.

Availability note (English)

Available from http://dx.doi.org/10.1088/0004-637X/801/1/25

Additional details

Identifiers

Publishing Information

Journal Title
Astrophysical Journal
Journal Volume
801
Journal Issue
1
Series
Since 2009, the country of publication for this journal is the UK.
Journal Page Range
[28 p.]
ISSN
0004-637X
CODEN
ASJOAB