2023A&A...679A.138S


Query : 2023A&A...679A.138S

2023A&A...679A.138S - Astronomy and Astrophysics, volume 679A138 (2023/11-1)

A JWST inventory of protoplanetary disk ices The edge-on protoplanetary disk HH 48 NE, seen with the Ice Age ERS program.

STURM J.A., McCLURE M.K., BECK T.L., HARSONO D., BERGNER J.B., DARTOIS E., BOOGERT A.C.A., CHIAR J.E., CORDINER M.A., DROZDOVSKAYA M.N., IOPPOLO S., LAW C.J., LINNARTZ H., LIS D.C., MELNICK G.J., McGUIRE B.A., NOBLE J.A., OBERG K.I., PALUMBO M.E., PENDLETON Y.J., PEROTTI G., PONTOPPIDAN K.M., QASIM D., ROCHA W.R.M., TERADA H., URSO R.G. and VAN DISHOECK E.F.

Abstract (from CDS):

Ices are the main carriers of volatiles in protoplanetary disks and are crucial to our understanding of the protoplanetary disk chemistry that ultimately sets the organic composition of planets. The Director's Discretionary-Early Release Science (DD-ERS) program Ice Age on the James Webb Space Telescope (JWST) follows the ice evolution through all stages of star and planet formation. JWST's exquisite sensitivity and angular resolution uniquely enable detailed and spatially resolved inventories of ices in protoplanetary disks. JWST/NIRSpec observations of the edge-on Class II protoplanetary disk HH 48 NE reveal spatially resolved absorption features of the major ice components H2O, CO2, and CO, and multiple weaker signatures from less abundant ices NH3, OCN–, and OCS. Isotopologue 13CO2 ice has been detected for the first time in a protoplanetary disk. Since multiple complex light paths contribute to the observed flux, the ice absorption features are filled in by ice-free scattered light. This implies that observed optical depths should be interpreted as lower limits to the total ice column in the disk and that abundance ratios cannot be determined directly from the spectrum. The 12CO2/13CO2 integrated absorption ratio of 14 implies that the 12CO2 feature is saturated, without the flux approaching zero, indicative of a very high CO2 column density on the line of sight, and a corresponding abundance with respect to hydrogen that is higher than interstellar medium values by a factor of at least a few. Observations of rare isotopologues are crucial, as we show that the 13CO2 observation allowed us to determine the column density of CO2 to be at least 1.6 × 1018 cm–2, which is more than an order of magnitude higher than the lower limit directly inferred from the observed optical depth. Spatial variations in the depth of the strong ice features are smaller than a factor of two. Radial variations in ice abundance, for example snowlines, are significantly modified since all observed photons have passed through the full radial extent of the disk. CO ice is observed at perplexing heights in the disk, extending to the top of the CO-emitting gas layer. Although poorly understood radiative transfer effects could contribute to this, we argue that the most likely interpretation is that we observed some CO ice at high temperatures, trapped in less volatile ices such as H2O and CO2. Future radiative transfer models will be required to constrain the physical origin of the ice absorption and the implications of these observations for our current understanding of disk physics and chemistry.

Abstract Copyright: © The Authors 2023

Journal keyword(s): astrochemistry - protoplanetary disks - radiative transfer - scattering - planets and satellites: formation - stars: individual: HH 48 NE

Simbad objects: 20

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Number of rows : 20
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 2MASS J03285129+3117397 Y*O 03 28 51.291 +31 17 39.79           ~ 28 0
2 V* HK Tau TT* 04 31 50.5715875272 +24 24 17.775307548 16.81 16.689 15.292     M0.5 358 1
3 V* HK Tau B TT* 04 31 50.6002481212 +24 24 15.502558869           ~ 95 0
4 IRAS 04302+2247 Y*O 04 33 16.50096 +22 53 20.4000           ~ 215 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* HV Tau LM* 04 38 35.2904827968 +26 10 38.640143136           M1Ve 160 0
7 V* HV Tau C TT* 04 38 35.5125950280 +26 10 41.316576204         14.90 K6 110 0
8 V* UY Aur Or* 04 51 47.3890167432 +30 47 13.551561492 12.82 12.96 11.90 10.59 9.52 M0e+M2.5e 379 0
9 M 43 HII 05 35 31 -05 16.2           ~ 201 0
10 V* TW Hya TT* 11 01 51.9053285064 -34 42 17.033218380   11.94 10.50 10.626 9.18 K6Ve 2144 1
11 IRAS 11030-7702 TT* 11 04 22.7159038128 -77 18 08.299910700     17.89     K6/M0e 75 0
12 HH 48 HH 11 04 22.8 -77 18 08           ~ 50 0
13 IRAS 11051-7706 Y*O 11 06 46.025 -77 22 29.67           ~ 101 0
14 NAME Cha 1 MoC 11 06 48 -77 18.0           ~ 1266 1
15 HD 100546 Be* 11 33 25.4408872296 -70 11 41.241297948   6.71 6.30   6.64 A0VaekB8_lB 894 1
16 CD-25 11111B TT* 15 49 15.5294156575 -26 00 50.039007268   13.37 12.81 14.02   A2IVe 35 0
17 HD 142527 Ae* 15 56 41.8882637904 -42 19 23.248281828   9.04 8.34     F6III 741 1
18 CRBR 2422.8-3423 Y*O 16 27 24.61320 -24 41 03.4080           ~ 101 1
19 BKLT J162813-243139 Y*O 16 28 13.6972712208 -24 31 39.845643564           ~ 79 0
20 IRAS 17178-2600 PN? 17 20 56.1353525664 -26 03 30.577658436   14.408 13.627 12.879   F2Ve 25 0

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