2025A&A...694A.147G


Query : 2025A&A...694A.147G

2025A&A...694A.147G - Astronomy and Astrophysics, volume 694A147 (2025/2-1)

MINDS The influence of outer dust disc structure on the volatile delivery to the inner disc.

GASMAN D., TEMMINK M., VAN DISHOECK E.F., KURTOVIC N.T., GRANT S.L., SELLEK A., TABONE B., HENNING T., KAMP I., GUDEL M., BARRADO D., CARATTI O GARATTI A., GLAUSER A.M., WATERS L.B.F.M., ARABHAVI A.M., JANG H., KANWAR J., LIENERT J.L., PEROTTI G., SCHWARZ K. and VLASBLOM M.

Abstract (from CDS):

Context. The Atacama Large Millimeter/submillimeter Array (ALMA) has revealed that the millimetre dust structures of protoplanetary discs are extremely diverse, ranging from small and compact dust discs to large discs with multiple rings and gaps. It has been proposed that the strength of H2O emission in the inner disc particularly depends on the influx of icy pebbles from the outer disc, a process that would correlate with the outer dust disc radius, and that could be prevented by pressure bumps. Additionally, the dust disc structure should also influence the emission of other gas species in the inner disc. Since terrestrial planets likely form in the inner disc regions, understanding their composition is of interest.
Aims. This work aims to assess the influence of pressure bumps on the inner disc's molecular reservoirs. The presence of a dust gap, and potentially giant planet formation farther out in the disc, may influence the composition of the inner disc, and thus the building blocks of terrestrial planets.
Methods. Using the improved sensitivity and spectral resolution of the Mid-InfraRed Instrument's (MIRI) Medium Resolution Spectrometer (MRS) on the James Webb Space Telescope (JWST) compared to Spitzer, we compared the observational emission properties of H2O, HCN, C2H2, and CO2 with the outer dust disc structure from ALMA observations, in eight discs with confirmed gaps in ALMA observations, and two discs with gaps of tens of astronomical units in width, around stars with M⋆ ≥ 0.45 M⊙ . We used new visibility plane fits of the ALMA data to determine the outer dust disc radius and identify substructures in the discs.
Results. We find that the presence of a dust gap does not necessarily result in weak H2O emission. Furthermore, the relative lack of colder H2O-emission seems to go hand in hand with elevated emission from carbon-bearing species. Of the discs that show significant substructure within the CO and CH4 snowlines, most show detectable emission from the carbon-bearing species. The discs with cavities and extremely wide gaps appear to behave as a somewhat separate group, with stronger cold H2O emission and weak warm H2O emission.
Conclusions. We conclude that fully blocking radial dust drift from the outer disc seems difficult to achieve, even for discs with very wide gaps or cavities, which can still show significant cold H2O emission. However, there does seem to be a dichotomy between discs that show a strong cold H2O excess and ones that show strong emission from HCN and C2H2. Better constraints on the influence of the outer dust disc structure and inner disc composition require more information on substructure formation timescales and disc ages, along with the importance of trapping of (hyper)volatiles like CO and CO2 into more strongly bound ices like H2O and chemical transformation of CO into less volatile species.

Abstract Copyright: © The Authors 2025

Journal keyword(s): astrochemistry - protoplanetary disks - stars: variables: T Tauri, Herbig Ae/Be - infrared: planetary systems - submillimeter: planetary systems

Simbad objects: 16

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Number of rows : 16
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 V* BP Tau Or* 04 19 15.8339827632 +29 06 26.926959492   13.13 12.12 11.89   K5/7Ve 721 0
2 V* IQ Tau Or* 04 29 51.5569574040 +26 06 44.859710736 15.43   13.80 12.28 11.11 M0.5 281 0
3 V* HL Tau Or* 04 31 38.5107609312 +18 13 57.859747968   15.89 14.49 14.39   K5 1546 0
4 V* GK Tau Or* 04 33 34.5630097872 +24 21 05.855136732 15.50   13.00 12.02 10.62 K7:Ve 338 0
5 V* DL Tau Or* 04 33 39.0767679288 +25 20 38.101382952 14.04 14.59 13.40 11.85 10.89 K7Ve 372 0
6 V* CI Tau Or* 04 33 52.0143963264 +22 50 30.094090908 14.97 15.09 13.80     K4IVe 422 1
7 V* HP Tau Or* 04 35 52.7819078592 +22 54 23.156947512 17.39 14.9 14.90     K2-5e 243 1
8 V* DR Tau Or* 04 47 06.2151561264 +16 58 42.813872580 12.03 11.86 10.50 12.19   K5Ve 585 0
9 V* SY Cha Or* 10 56 30.3883129248 -77 11 39.401977596         11.29 K5Ve 194 0
10 IRAS 11030-7702 TT* 11 04 22.7159038128 -77 18 08.299910700     17.89     K6/M0e 75 0
11 CD-40 8434 TT* 14 08 10.1545500744 -41 23 52.573291080   13.42 12.18 11.71 10.506 K7IVe 546 0
12 V* GW Lup Or* 15 46 44.7290527536 -34 30 35.677420056   13.8       M1.5e 201 0
13 THA 15-12 Or* 15 56 09.2066646912 -37 56 06.126118692   13.12 11.93 11.45   M0e 554 0
14 V* V1279 Sco Or* 16 08 22.4935277520 -39 04 46.427612052   14.99 13.66 11.70 11.21 M0.4 154 1
15 V* V1094 Sco TT* 16 08 36.1772010696 -39 23 02.464980972 16.01 15.00 13.48 12.47 11.45 ~ 101 1
16 IRAS 16285-2355 Y*O 16 31 35.65752 -24 01 29.4708           ~ 178 0

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