{
  "annotation_id": "8f999fdb-17bc-486e-91a3-1bd0a492b02b",
  "date_created": "2026-02-17T05:53:12.061000Z",
  "date_modified": "2026-02-17T05:53:12.061000Z",
  "file_hash": "0b05caed94ebb02d02695b3826ba5943d188e789b5ff17210bdc9b6a837c2809",
  "private": false,
  "record": {
    "abstract": "Aims: The G28.37+0.07 star-forming region is a prototypical infrared dark cloud (IRDC) located at the interface of a converging gas flow. This study characterizes the properties of this dynamic gas flow. Methods: Combining data from the Northern Extended Millimeter Array (NOEMA) with single-dish data from the IRAM30m observatory, we mapped large spatial scales (~81pc^2) at high angular resolution (7.0\u0027\u0027x2.6\u0027\u0027 corresponding ~2.3x10^4au or ~0.1pc) down to core scales. The spectral setup in the 3mm band covers many spectral lines as well as the continuum emission. Results: The data reveal the proposed west-east converging gas flow in all observed dense gas tracers. We estimate a mass-flow rate along that flow around 10^-3M_sun/yr. Comparing these west-east flow rates to infall rates toward sources along the line of sight, the gas flow rates are roughly a factor of 25 greater than than those along the line of sight. This confirms the dominance of longitudinal motions along the converging gas flow in G28.37. For comparison, in the main north-south IRDC formed by the west-east converging gas flow, infall rates along the line of sight are about an order of magnitude greater than those along the west-east flow. In addition to the kinematic analysis, a comparison of CH_3CN-derived gas temperatures with Herschel-derived dust temperatures typically show higher gas temperatures toward high-density sources. We discuss whether mechanical heating from the conversion of the flow\u0027s kinetic energy into thermal energy may explain some of the observed temperature differences. Conclusions: The differences between flow rates along the converging flow, perpendicular to it, and toward the sources at the IRDC center indicate that at the interfaces of converging gas flows - where most of the active star formation takes place - originally more directed gas flows can convert into multidirectional infall motions.",
    "arxiv_id": "2601.07407",
    "authors": [
      "H. Beuther",
      "C. Gieser",
      "H. Linz",
      "Q. Zhang",
      "S. Feng",
      "A. Ahmadi",
      "J. D. Soler",
      "D. Semenov",
      "M. R. A. Wells",
      "S. Reyes-Reyes"
    ],
    "categories": [
      "astro-ph.GA"
    ],
    "license": "http://creativecommons.org/licenses/by/4.0/",
    "title": "The converging gas flow around the infrared dark cloud G28.3",
    "url": "https://arxiv.org/abs/2601.07407",
    "version": "v1"
  },
  "schema_id": "dorsal/arxiv",
  "source": {
    "execution_id": "ecf54184-ece5-4ddf-b109-2af33531a48d",
    "id": "arXiv Dataset",
    "type": "Model",
    "variant": "snapshot-2026-01-17",
    "version": "0.1.0"
  },
  "user_id": 1000002
}