TY - JOUR
T1 - Molecules with ALMA at planet-forming scales (MAPS). XVII. determining the 2D thermal structure of the HD 163296 disk
AU - Calahan, Jenny K.
AU - Bergin, Edwin A.
AU - Zhang, Ke
AU - Schwarz, Kamber R.
AU - Öberg, Karin I.
AU - Guzmán, Viviana V.
AU - Walsh, Catherine
AU - Aikawa, Yuri
AU - Alarcón, Felipe
AU - Andrews, Sean M.
AU - Bae, Jaehan
AU - Bergner, Jennifer B.
AU - Booth, Alice S.
AU - Bosman, Arthur D.
AU - Cataldi, Gianni
AU - Czekala, Ian
AU - Huang, Jane
AU - Ilee, John D.
AU - Law, Charles J.
AU - Le Gal, Romane
AU - Long, Feng
AU - Loomis, Ryan A.
AU - Ménard, François
AU - Nomura, Hideko
AU - Qi, Chunhua
AU - Teague, Richard
AU - Van'T Hoff, Merel L.R.
AU - Wilner, David J.
AU - Yamato, Yoshihide
N1 - Funding Information:
This paper makes use of the following ALMA data: ADS/ JAO.ALMA#2018.1.01055.L. ALMA is a partnership of ESO (representing its member states), NSF (USA) and NINS (Japan), together with NRC (Canada), MOST and ASIAA (Taiwan), and KASI (Republic of Korea), in cooperation with the Republic of Chile. The Joint ALMA Observatory is operated by ESO, AUI/ NRAO and NAOJ. The National Radio Astronomy Observatory is a facility of the National Science Foundation operated under cooperative agreement by Associated Universities, Inc. J.K.C. acknowledges support from the National Science Foundation Graduate Research Fellowship under grant No. DGE 1256260 and the National Aeronautics and Space Administration FINESST grant, under grant No. 80NSSC19K1534. E.A.B. acknowledges support from NSF AAG grant #1907653. K.Z. acknowledges the support of the Office of the Vice Chancellor for Research and Graduate Education at the University of Wisconsin- Madison with funding from the Wisconsin Alumni Research Foundation, and the support of NASA through Hubble Fellowship grant HST-HF2-51401.001 awarded by the Space Telescope Science Institute, which is operated by the Association of Universities for Research in Astronomy, Inc., for NASA, under contract NAS5-26555. K.R.S. acknowledges the support of NASA through Hubble Fellowship Program grant HST-HF2-51419.001, awarded by the Space Telescope Science Institute,which is operated by the Association of Universities for Research in Astronomy, Inc., for NASA, under contract NAS5-26555. K.I.Ö. acknowledges support from the Simons Foundation (SCOL #321183) and an NSF AAG grant (#1907653). R.T. and F.L. acknowledge support from the Smithsonian Institution as a Submillimeter Array (SMA) Fellow. J.D.I. acknowledges support from the Science and Technology Facilities Council of the United Kingdom (STFC) under ST/T000287/1. C.J.L. acknowledges funding from the National Science Foundation Graduate Research Fellowship under grant DGE1745303. R.L.G. acknowledges support from a CNES fellowship grant. M.L.R.H. acknowledges support from the Michigan Society of Fellows. Y.A. acknowledges support by NAOJ ALMA Scientific Research grant code 2019-13B and Grant-in-Aid for Scientific Research (S) 18H05222. S.M.A. and J.H. acknowledge funding support from the National Aeronautics and Space Administration under grant No. 17- XRP17 2-0012 issued through the Exoplanets Research Program. Support for this work was provided by NASA through the NASA Hubble Fellowship grant #HST-HF2-51460.001-A awarded by the Space Telescope Science Institute, which is operated by the Association of Universities for Research in Astronomy, Inc., for NASA, under contract NAS5-26555. J.B. acknowledges support by NASA through the NASA Hubble Fellowship grant #HSTHF2- 51427.001-A awarded by the Space Telescope Science Institute, which is operated by the Association of Universities for Research in Astronomy, Incorporated, under NASA contract NAS5-26555. C.W. acknowledges financial support from the University of Leeds, STFC, and UKRI (grant Nos. ST/ R000549/1, ST/T000287/1, MR/T040726/1). I.C. was supported by NASA through the NASA Hubble Fellowship grant HST-HF2-51405.001-A awarded by the Space Telescope Science Institute, which is operated by the Association of Universities for Research in Astronomy, Inc., for NASA, under contract NAS5- 26555. F.M. acknowledges support from ANR of France under contract ANR-16-CE31-0013 (Planet-Forming-Disks) and ANR- 15-IDEX-02 (through CDP "Origins of Life"). G.C. is supported by the NAOJ ALMA Scientific Research grant code 2019-13B. V. V.G. acknowledges support from FONDECYT Iniciación 11180904 and ANID project Basal AFB-170002. F.A. acknowledges support from NSF AAG grant No. 1907653. J.B.B. acknowledges support from NASA through the NASA Hubble Fellowship grant No. HST-HF2-51429.001-A, awarded by the Space Telescope Science Institute, which is operated by the Association of Universities for Research in Astronomy, Inc., for NASA, under contract NAS5-26555. A.S.B acknowledges the studentship funded by the Science and Technology Facilities Council of the United Kingdom (STFC). A.D.B. acknowledges support from NSF AAG grant No. 1907653. H.N. acknowledges support by NAOJ ALMA Scientific Research grant code 2018-10B and Grant-in-Aid for Scientific Research 18H05441. Y.Y. is supported by IGPEES, WINGS Program, the University of Tokyo. We also thank the referee for a careful read of the text and insightful comments.
Publisher Copyright:
© 2021. The American Astronomical Society. All rights reserved.
PY - 2021/11
Y1 - 2021/11
N2 - Understanding the temperature structure of protoplanetary disks is key to interpreting observations, predicting the physical and chemical evolution of the disk, and modeling planet formation processes. In this study, we constrain the two-dimensional thermal structure of the disk around the Herbig Ae star HD 163296. Using the thermochemical code RAC2D, we derive a thermal structure that reproduces spatially resolved Atacama Large Millimeter/submillimeter Array observations (~0".12 (13 au)-0".25 (26 au)) of 12CO J=2 - 1, 13CO J=1 - 0, 2 - 1, C18O J=1 - 0, 2 - 1, and C17O J=1 - 0, the HD J=1 - 0 flux upper limit, the spectral energy distribution (SED), and continuum morphology. The final model incorporates both a radial depletion of CO motivated by a timescale shorter than typical CO gas-phase chemistry (0.01 Myr) and an enhanced temperature near the surface layer of the the inner disk (z/r≳ 0.21). This model agrees with the majority of the empirically derived temperatures and observed emitting surfaces derived from the J=2 - 1 CO observations. We find an upper limit for the disk mass of 0.35 M⊙, using the upper limit of the HD J=1 - 0 and J=2 - 1 flux. With our final thermal structure, we explore the impact that gaps have on the temperature structure constrained by observations of the resolved gaps. Adding a large gap in the gas and small dust additionally increases gas temperature in the gap by only 5%-10%. This paper is part of the MAPS special issue of the Astrophysical Journal Supplement.
AB - Understanding the temperature structure of protoplanetary disks is key to interpreting observations, predicting the physical and chemical evolution of the disk, and modeling planet formation processes. In this study, we constrain the two-dimensional thermal structure of the disk around the Herbig Ae star HD 163296. Using the thermochemical code RAC2D, we derive a thermal structure that reproduces spatially resolved Atacama Large Millimeter/submillimeter Array observations (~0".12 (13 au)-0".25 (26 au)) of 12CO J=2 - 1, 13CO J=1 - 0, 2 - 1, C18O J=1 - 0, 2 - 1, and C17O J=1 - 0, the HD J=1 - 0 flux upper limit, the spectral energy distribution (SED), and continuum morphology. The final model incorporates both a radial depletion of CO motivated by a timescale shorter than typical CO gas-phase chemistry (0.01 Myr) and an enhanced temperature near the surface layer of the the inner disk (z/r≳ 0.21). This model agrees with the majority of the empirically derived temperatures and observed emitting surfaces derived from the J=2 - 1 CO observations. We find an upper limit for the disk mass of 0.35 M⊙, using the upper limit of the HD J=1 - 0 and J=2 - 1 flux. With our final thermal structure, we explore the impact that gaps have on the temperature structure constrained by observations of the resolved gaps. Adding a large gap in the gas and small dust additionally increases gas temperature in the gap by only 5%-10%. This paper is part of the MAPS special issue of the Astrophysical Journal Supplement.
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UR - http://www.scopus.com/inward/citedby.url?scp=85119655228&partnerID=8YFLogxK
U2 - 10.3847/1538-4365/ac143f
DO - 10.3847/1538-4365/ac143f
M3 - Article
AN - SCOPUS:85119655228
SN - 0067-0049
VL - 257
JO - Astrophysical Journal, Supplement Series
JF - Astrophysical Journal, Supplement Series
IS - 1
M1 - 17
ER -