4.7 Article

The Role of Neutral Hydrogen in Setting the Abundances of Molecular Species in the Milky Way's Diffuse Interstellar Medium. II. Comparison between Observations and Theoretical Models

期刊

ASTROPHYSICAL JOURNAL
卷 926, 期 2, 页码 -

出版社

IOP Publishing Ltd
DOI: 10.3847/1538-4357/ac4160

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资金

  1. NSF from the NRAO [SOSPA6-023]
  2. University of Wisconsin
  3. John Simon Guggenheim fellowship
  4. Max Planck Institute for Extraterrestrial Physics
  5. INSU/CNRS (France)
  6. MPG (Germany)
  7. IGN (Spain)
  8. [W19AQ]
  9. [S20AB]

向作者/读者索取更多资源

By comparing observations and models, we find that structures in the diffuse interstellar medium can be explained by different chemical models based on their temperature and density. High-temperature and high-density structures are typically found in environments close to massive star formation and in directions with thermally unstable H i. However, some observations cannot be explained by photodissociation region models, suggesting the need for alternative mechanisms.
We compare observations of H i from the Very Large Array (VLA) and the Arecibo Observatory and observations of HCO+ from the Atacama Large Millimeter/submillimeter Array (ALMA) and the Northern Extended Millimeter Array (NOEMA) in the diffuse (A ( V ) less than or similar to 1) interstellar medium (ISM) to predictions from a photodissociation region (PDR) chemical model and multiphase ISM simulations. Using a coarse grid of PDR models, we estimate the density, FUV radiation field, and cosmic-ray ionization rate (CRIR) for each structure identified in HCO+ and H i absorption. These structures fall into two categories. Structures with T ( s ) < 40 K, mostly with N(HCO+) less than or similar to 10(12) cm(-2), are consistent with modest density, FUV radiation field, and CRIR models, typical of the diffuse molecular ISM. Structures with spin temperature T ( s ) > 40 K, mostly with N(HCO+) greater than or similar to 10(12) cm(-2), are consistent with high density, FUV radiation field, and CRIR models, characteristic of environments close to massive star formation. The latter are also found in directions with a significant fraction of thermally unstable H i. In at least one case, we rule out the PDR model parameters, suggesting that alternative mechanisms (e.g., nonequilibrium processes like turbulent dissipation and/or shocks) are required to explain the observed HCO+ in this direction. Similarly, while our observations and simulations of the turbulent, multiphase ISM agree that HCO+ formation occurs along sight lines with N(H I) greater than or similar to 10(21) cm(-2), the simulated data fail to explain HCO+ column densities greater than or similar to few x 10(12) cm(-2). Because a majority of our sight lines with HCO+ had such high column densities, this likely indicates that nonequilibrium chemistry is important for these lines of sight.

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