SIMBAD references

2007ApJ...671...73Y - Astrophys. J., 671, 73-84 (2007/December-2)

HCN to HCO+ millimeter line diagnostics of AGN molecular tori. I. Radiative transfer modeling.

YAMADA M., WADA K. and TOMISAKA K.

Abstract (from CDS):

We explore millimeter line diagnostics of an obscuring molecular torus modeled by a hydrodynamic simulation with three-dimensional non-local thermodynamic equilibrium radiative transfer calculations. Based on the results of a high-resolution hydrodynamic simulation of the molecular torus around an active galactic nucleus, we calculate the intensities of the HCN and HCO+ rotational lines as two representative high-density tracers. Three-dimensional radiative transfer calculations shed light on a complicated excitation state in the inhomogeneous torus, even though a spatially uniform chemical structure is assumed. We find that similar transition coefficients for the HCN and HCO+ rotational lines lead to a natural concordance of the level population distributions of these molecules and a line ratio RHCN/HCO+≲1 for the same molecular abundance value over 2 orders of magnitude. Our results suggest that HCN must be much more abundant than HCO+ (yHCN≳10yHCO+^_) in order to obtain the high ratio (RHCN/HCO+∼2) observed in some nearby galaxies. There is a remarkable dispersion in the relation between integrated intensity and column density, indicative of possible shortcomings of the HCN(1-0) and HCO+(1-0) lines as high-density tracers. The internal structures of inhomogeneous molecular tori down to subparsec scales in external galaxies will be revealed by the forthcoming Atacama Large Millimeter/submillimeter Array. Three-dimensional radiative transfer calculations of molecular lines with a high-resolution hydrodynamic simulation prove to be a powerful tool to provide a physical basis for molecular-line diagnostics of the central regions of external galaxies.

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Journal keyword(s): Galaxies: Active - Galaxies: ISM - ISM: Molecules - Radiative Transfer - Radio Lines: Galaxies

Simbad objects: 10

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