Gas and dust mass in the disk around the Herbig Ae star HD169142

TL;DR

This study models the gas component of the HD169142 disk using CO isotopologue observations, constraining its mass, structure, and gas-to-dust ratio, and finds the disk is in Keplerian rotation with distinct vertical CO regions.

Contribution

It provides the first detailed 3D analysis of CO isotopologue emission in the HD169142 disk, deriving its gas mass and vertical structure using radiative transfer modeling.

Findings

Disk is in Keplerian rotation with ~13° inclination.

Gas mass estimated between 0.006 and 0.03 solar masses.

Gas-to-dust ratio consistent with 25 to 100 depending on assumptions.

Abstract

We investigate the physical structure of the gas component of the disk around the pre-main-sequence star HD169142. The 13CO and C18O J=2-1 line emission is observed from the disk with 1.4'' resolution using the Submillimeter Array. We adopt the disk physical structure derived from a model which fits the spectral energy distribution of HD169142. We obtain the full three-dimensional information on the CO emission with the aid of a molecular excitation and radiative transfer code. This information is used for the analysis of our observations and previous 12CO J=2-1 and 1.3 mm continuum data. The disk is in Keplerian rotation and seen at an inclination close to 13 deg from face-on. We conclude that the regions traced by different CO isotopologues are distinct in terms of their vertical location within the disk, their temperature and their column densities. With the given disk structure, we find that freeze-out is not efficient enough to remove a significant amount of CO from gas phase. Both observed lines match the model prediction both in flux and in the spatial structure of the emission. Therefore we use our data to derive the 13CO and C18O mass and consequently the 12CO mass using standard isotopic ratios. We constrain the total disk gas mass to (0.6-3.0)x10(-2) Msun. Adopting a maximum dust opacity of 2 cm2 per gram of dust we derive a minimum dust mass of 2.16x10(-4) Msun from the fit to the 1.3 mm data. Comparison of the derived gas and dust mass shows that the gas to dust mass ratio of 100 is only possible under the assumption of a dust opacity of 2 cm2/g and 12CO abundance of 10(-4) with respect to H2. However, our data are also compatible with a gas to dust ratio of 25, with a dust opacity of 1 cm2/g and 12CO abundance of 2x10(-4).