Published February 1, 2021 | Version v1
Journal article

The TW Hya Rosetta Stone Project. III. Resolving the Gaseous Thermal Profile of the Disk

  • 1. University of Michigan, 323 West Hall, 1085 South University Avenue, Ann Arbor, MI 48109 (United States)
  • 2. Center for Astrophysics - Harvard & Smithsonian, 60 Garden Street, Cambridge, MA 02138 (United States)
  • 3. Astronomy Department, University of Virginia, Charlottesville, VA 22904 (United States)
  • 4. University of Chicago, Department of the Geophysical Sciences, Chicago, IL 60637 (United States)
  • 5. Division of Chemistry & Chemical Engineering, California Institute of Technology, Pasadena, CA 91125 (United States)
  • 6. Leiden Observatory, Leiden University, 2300 RA Leiden (Netherlands)
  • 7. Instituto de Astrofísica, Ponticia Universidad Católica de Chile, Av. Vicuña Mackenna 4860, 7820436 Macul, Santiago (Chile)
  • 8. Tartu Observatory, University of Tartu, Observatooriumi 1, 61602, Tõravere (Estonia)
  • 9. National Radio Astronomy Observatory (NRAO), 520 Edgemont Rd., Charlottesville, VA 22903 (United States)
  • 10. Leiden Observatory, Leiden University, P.O. Box 9513, 2300 RA Leiden (Netherlands)
  • 11. School of Physics and Astronomy University of Leeds, Leeds LS2 9JT (United Kingdom)

Description

The thermal structure of protoplanetary disks is a fundamental characteristic of the system that has wide-reaching effects on disk evolution and planet formation. In this study, we constrain the 2D thermal structure of the protoplanetary disk TW Hya structure utilizing images of seven CO lines. This includes new ALMA observations of 12CO J = 2–1 and C18O J = 2–1 as well as archival ALMA observations of 12CO J = 3–2, 13CO J = 3–2 and 6–5, and C18O J = 3–2 and 6–5. Additionally, we reproduce a Herschel observation of the HD J = 1–0 line flux and the spectral energy distribution and utilize a recent quantification of CO radial depletion in TW Hya. These observations were modeled using the thermochemical code RAC2D, and our best-fit model reproduces all spatially resolved CO surface brightness profiles. The resulting thermal profile finds a disk mass of 0.025 M and a thin upper layer of gas depleted of small dust with a thickness of ∼1.2% of the corresponding radius. Using our final thermal structure, we find that CO alone is not a viable mass tracer, as its abundance is degenerate with the total H2 surface density. Different mass models can readily match the spatially resolved CO line profiles with disparate abundance assumptions. Mass determination requires additional knowledge, and, in this work, HD provides the additional constraint to derive the gas mass and support the inference of CO depletion in the TW Hya disk. Our final thermal structure confirms the use of HD as a powerful probe of protoplanetary disk mass. Additionally, the method laid out in this paper is an employable strategy for extraction of disk temperatures and masses in the future.

Availability note (English)

Available from http://dx.doi.org/10.3847/1538-4357/abd255

Additional details

Identifiers

Publishing Information

Journal Title
Astrophysical Journal
Journal Volume
908
Journal Issue
1
Journal Page Range
[22 p.]
ISSN
0004-637X
CODEN
ASJOAB

INIS

Country of Publication
United Kingdom
Country of Input or Organization
International Atomic Energy Agency (IAEA)
INIS RN
53081089
Subject category
S79: ASTROPHYSICS, COSMOLOGY AND ASTRONOMY; S71: CLASSICAL AND QUANTUM MECHANICS, GENERAL PHYSICS;
Descriptors DEI
BRIGHTNESS; CARBON MONOXIDE; DENSITY; DUSTS; ENERGY SPECTRA; LAYERS; PLANETS; PROBES; PROTOPLANETS; SURFACES
Descriptors DEC
CARBON COMPOUNDS; CARBON OXIDES; CHALCOGENIDES; OPTICAL PROPERTIES; OXIDES; OXYGEN COMPOUNDS; PHYSICAL PROPERTIES; SPECTRA