TY - JOUR
T1 - exoALMA. VII. Benchmarking hydrodynamics and radiative transfer codes
AU - Bae, Jaehan
AU - Flock, Mario
AU - Izquierdo, Andrés
AU - Kanagawa, Kazuhiro
AU - Ono, Tomohiro
AU - Pinte, Christophe
AU - Price, Daniel J.
AU - Rosotti, Giovanni P.
AU - Wafflard-Fernandez, Gaylor
AU - Lesur, Geoffroy
AU - Masset, Frédéric
AU - Andrews, Sean M.
AU - Barraza-Alfaro, Marcelo
AU - Benisty, Myriam
AU - Cataldi, Gianni
AU - Cuello, Nicolás
AU - Curone, Pietro
AU - Czekala, Ian
AU - Facchini, Stefano
AU - Fasano, Daniele
AU - Galloway-Sprietsma, Maria
AU - Hall, Cassandra
AU - Hammond, Iain
AU - Huang, Jane
AU - Lodato, Giuseppe
AU - Longarini, Cristiano
AU - Stadler, Jochen
AU - Teague, Richard
AU - Wilner, David J.
AU - Winter, Andrew J.
AU - Wölfer, Lisa
AU - Yoshida, Tomohiro C.
N1 - Funding: J.B. acknowledges support from NASA XRP grant No. 80NSSC23K1312. M.B., D.F., and J.S. have received funding from the European Research Council (ERC) under the European Union’s Horizon 2020 research and innovation program (PROTOPLANETS, grant agreement No. 101002188). P.C. acknowledges support by the Italian Ministero dell’Istruzione, Università e Ricerca through the grant Progetti Premiali 2012 - iALMA (CUP C52I13000140001) and by the ANID BASAL project FB210003. N.C. has received funding from the European Research Council (ERC) under the European Union Horizon Europe research and innovation program (grant agreement No. 101042275, project Stellar-MADE). S.F. is funded by the European Union (ERC, UNVEIL, 101076613), and acknowledges financial contribution from PRIN-MUR 2022YP5ACE. MF is supported by a grant-in-Aid from the Japan Society for the Promotion of Science (KAKENHI: No. JP22H01274). C.H. acknowledges support from NSF AAG grant No. 2407679. I.H. is supported by an Australian Government Research Training Program (RTP) Scholarship. Support for AFI was provided by NASA through the NASA Hubble Fellowship grant No. HST-HF2-51532.001-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. G.L. has received funding from the European Union’s Horizon 2020 research and innovation program under the Marie Sklodowska-Curie grant agreement No. 823823 (DUSTBUSTERS). C.L. has received funding from the European Union’s Horizon 2020 research and innovation program under the Marie Sklodowska-Curie grant agreement No. 823823 (DUSTBUSTERS) and by the UK Science and Technology research Council (STFC) via the consolidated grant ST/W000997/1. C.P. acknowledges Australian Research Council funding via FT170100040, DP18010423, DP220103767, and DP240103290. D.P. acknowledges Australian Research Council funding via DP18010423, DP220103767, and DP240103290. G.R. acknowledges funding from the Fondazione Cariplo, grant no. 2022-1217, and the European Research Council (ERC) under the European Union’s Horizon Europe Research & Innovation Programme under grant agreement no. 101039651 (DiscEvol). G.W.F. acknowledges support from the European Research Council (ERC) under the European Union Horizon 2020 research and innovation program (grant agreement no. 815559 (MHDiscs)). G.W.F. was granted access to the HPC resources of IDRIS under the allocation A0120402231 made by GENCI. T.C.Y. acknowledges support by grant-in-Aid for JSPS Fellows JP23KJ1008.
PY - 2025/5/1
Y1 - 2025/5/1
N2 - Forward modeling is often used to interpret substructures observed in protoplanetary disks. To ensure the robustness and consistency of the current forward-modeling approach from the community, we conducted a systematic comparison of various hydrodynamics and radiative transfer codes. Using four grid-based hydrodynamics codes (FARGO3D, Idefix, Athena++, and PLUTO) and a smoothed-particle hydrodynamics code (Phantom), we simulated a protoplanetary disk with an embedded giant planet. We then used two radiative transfer codes (mcfost and RADMC-3D) to calculate disk temperatures and create synthetic 12CO cubes. Finally, we retrieved the location of the planet from the synthetic cubes using DISCMINER. We found strong consistency between the hydrodynamics codes, particularly in the density and velocity perturbations associated with planet-driven spirals. We also found a good agreement between the two radiative transfer codes: the disk temperature in mcfost and RADMC-3D models agrees within ≲3% everywhere in the domain. In synthetic 12CO channel maps, this results in brightness temperature differences within ±1.5 K in all our models. This good agreement ensures consistent retrieval of planet’s radial/azimuthal location with only a few percent of scatter, with velocity perturbations varying ≲20% among the models. Notably, while the planet-opened gap is shallower in the Phantom simulation, we found that this does not impact the planet location retrieval. In summary, our results demonstrate that any combination of the tested hydrodynamics and radiative transfer codes can be used to reliably model and interpret planet-driven kinematic perturbations.
AB - Forward modeling is often used to interpret substructures observed in protoplanetary disks. To ensure the robustness and consistency of the current forward-modeling approach from the community, we conducted a systematic comparison of various hydrodynamics and radiative transfer codes. Using four grid-based hydrodynamics codes (FARGO3D, Idefix, Athena++, and PLUTO) and a smoothed-particle hydrodynamics code (Phantom), we simulated a protoplanetary disk with an embedded giant planet. We then used two radiative transfer codes (mcfost and RADMC-3D) to calculate disk temperatures and create synthetic 12CO cubes. Finally, we retrieved the location of the planet from the synthetic cubes using DISCMINER. We found strong consistency between the hydrodynamics codes, particularly in the density and velocity perturbations associated with planet-driven spirals. We also found a good agreement between the two radiative transfer codes: the disk temperature in mcfost and RADMC-3D models agrees within ≲3% everywhere in the domain. In synthetic 12CO channel maps, this results in brightness temperature differences within ±1.5 K in all our models. This good agreement ensures consistent retrieval of planet’s radial/azimuthal location with only a few percent of scatter, with velocity perturbations varying ≲20% among the models. Notably, while the planet-opened gap is shallower in the Phantom simulation, we found that this does not impact the planet location retrieval. In summary, our results demonstrate that any combination of the tested hydrodynamics and radiative transfer codes can be used to reliably model and interpret planet-driven kinematic perturbations.
KW - Protoplanetary disks
KW - Planetary-disk interactions
KW - Hydrodynamical simulations
KW - Radiative transfer simulations
UR - https://www.scopus.com/pages/publications/105003942755
U2 - 10.3847/2041-8213/adc436
DO - 10.3847/2041-8213/adc436
M3 - Review article
AN - SCOPUS:105003942755
SN - 2041-8205
VL - 984
JO - Astrophysical Journal Letters
JF - Astrophysical Journal Letters
IS - 1
M1 - L12
ER -