2024A&A...688A..29S


Query : 2024A&A...688A..29S

2024A&A...688A..29S - Astronomy and Astrophysics, volume 688A29 (2024/8-1)

JWST detections of amorphous and crystalline HDO ice toward massive protostars.

SLAVICINSKA K., VAN DISHOECK E.F., TYCHONIEC L., NAZARI P., RUBINSTEIN A.E., GUTERMUTH R., TYAGI H., CHEN Y., BRUNKEN N.G.C., ROCHA W.R.M., MANOJ P., NARANG M., MEGEATH S.T., YANG Y.-L., LOONEY L.W., TOBIN J.J., BEUTHER H., BOURKE T.L., LINNARTZ H., FEDERMAN S., WATSON D.M. and LINZ H.

Abstract (from CDS):

Context. Tracing the origin and evolution of interstellar water is key to understanding many of the physical and chemical processes involved in star and planet formation. Deuterium fractionation offers a window into the physicochemical history of water due to its sensitivity to local conditions.
Aims. The aim of this work is to utilize the increased sensitivity and resolution of the James Webb Space Telescope (JWST) to quantify the HDO/H2O ratio in ices toward young stellar objects (YSOs) and to determine if the HDO/H2O ratios measured in the gas phase toward massive YSOs (MYSOs) are representative of the ratios in their ice envelopes.
Methods. Two protostars observed in the Investigating Protostellar Accretion (IPA) program using JWST NIRSpec were analyzed: HOPS 370, an intermediate-mass YSO (IMYSO), and IRAS 20126+4104, a MYSO. The HDO ice toward these sources was quantified via its 4.1 µm band. The contributions from the CH3OH combination modes to the observed optical depth in this spectral region were constrained via the CH3OH 3.53 µm band to ensure that the integrated optical depth of the HDO feature was not overestimated. H2O ice was quantified via its 3 µm band. New laboratory IR spectra of ice mixtures containing HDO, H2O, CH3OH, and CO were collected to aid in the fitting and chemical interpretation of the observed spectra.
Results. HDO ice is detected above the 3σ level in both sources. It requires a minimum of two components, one amorphous and one crystalline, to obtain satisfactory fits. The H2O ice band at 3 µm similarly requires both amorphous and crystalline components. The observed peak positions of the crystalline HDO component are consistent with those of annealed laboratory ices, which could be evidence of heating and subsequent recooling of the ice envelope (i.e., thermal cycling). The CH3OH 3.53 µm band is fit best with two cold components, one consisting of pure CH3OH and the other of CH3OH in an H2O-rich mixture. From these fits, ice HDO/H2O abundance ratios of 4.6 ± 1.8 × 10–3 and 2.6 ± 1.2 × 10–3 are obtained for HOPS 370 and IRAS 20126+4104, respectively.
Conclusions. The simultaneous detections of both crystalline HDO and crystalline H2O corroborate the assignment of the observed feature at 4.1 µm to HDO ice. The ice HDO/H2O ratios are similar to the highest reported gas HDO/H2O ratios measured toward MYSOs and the hot inner regions of isolated low-mass protostars, suggesting that at least some of the gas HDO/H2O ratios measured toward massive hot cores are representative of the HDO/H2O ratios in ices. The need for an H2O-rich CH3OH component in the CH3OH ice analysis supports recent experimental and observational results that indicate that some CH3OH ice may form prior to the CO freeze-out stage in H2O-rich ice layers.

Abstract Copyright: © The Authors 2024

Journal keyword(s): astrochemistry - techniques: spectroscopic - stars: protostars - ISM: abundances - ISM: molecules - infrared: ISM

Simbad objects: 32

goto Full paper

goto View the references in ADS

Number of rows : 32
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 NAME W3 IRS 5 Y*O 02 25 40.54 +62 05 51.4           B1 367 0
2 [JCC87] IRAS 2A Y*O 03 28 55.55 +31 14 36.7           ~ 513 3
3 ASR 114 Y*O 03 29 01.16520 +31 20 24.4140           ~ 79 1
4 V* V512 Per Or* 03 29 03.7578170808 +31 16 03.947525688           M3.5 419 0
5 [JCC87] IRAS 4A Y*O 03 29 10.49 +31 13 30.8           ~ 770 1
6 [JCC87] IRAS 4B Y*O 03 29 12.058 +31 13 02.05           ~ 625 0
7 LDN 1489 DNe 04 04 47.5 +26 19 42           ~ 238 0
8 RAFGL 5123 Y*O 04 31 34.07736 +18 08 04.9020           K3V/M3III 900 0
9 IRAS 04302+2247 Y*O 04 33 16.50096 +22 53 20.4000           ~ 215 0
10 IRAS 04361+2547 Y*O 04 39 13.89288 +25 53 20.8788           ~ 205 1
11 NAME Orion-KL SFR 05 35 14.16 -05 22 21.5           ~ 2421 1
12 NAME Orion Core ? 05 35 14.5 -05 22 30           ~ 212 0
13 OMC 2 MoC 05 35 27 -05 10.1           ~ 475 1
14 2MASS J05352762-0509337 Y*O 05 35 27.622 -05 09 33.78           ~ 128 0
15 NAME Ori A MoC 05 38 -07.1           ~ 3187 0
16 V* V883 Ori Or* 05 38 18.1018261392 -07 02 26.017707120           F:I: 274 0
17 HOPS 138 Y*O 05 38 48.33 -07 02 43.4           ~ 11 0
18 RAFGL 5163 Y*O 05 40 27.45024 -07 27 30.0564           ~ 151 1
19 IRAS 08448-4343 cor 08 46 33.8 -43 54 33           ~ 73 1
20 [B2001b] IRS 1 Y*O 12 01 36.53040 -65 08 51.9180           ~ 167 0
21 IRAS 16293-2422 cor 16 32 22.56 -24 28 31.8           ~ 1357 1
22 NAME NGC 6334 I(N) smm 17 20 54 -35 45.0           ~ 165 1
23 W 33a Y*O 18 14 39.56547 -17 52 02.2260           ~ 746 0
24 LDN 483 DNe 18 17 35 -04 39.8           ~ 359 0
25 CD-25 13135 PM* 18 27 18.6108819288 -25 04 23.845844784   12.75 11.51 10.764   M0.5 18 1
26 RAFGL 2271 SFR 18 53 18.54 +01 14 57.9           ~ 537 0
27 IRAS 18542+0114 cor 18 56 48.27432 +01 18 47.1132           ~ 37 0
28 LDN 663 DNe 19 36 55 +07 34.4           ~ 698 0
29 IRAS 20126+4104 Y*O 20 14 25.8816769656 +41 13 36.879427236           B2.5-B0.5 469 0
30 RAFGL 2591 Y*O 20 29 24.8230 +40 11 19.590           ~ 640 0
31 [WBN74] NGC 7538 IRS 1 Y*O 23 13 45.318 +61 28 11.69           ~ 433 3
32 IRAS 23118+6110 Y*O 23 14 02.09473 +61 27 18.8460           ~ 385 0

To bookmark this query, right click on this link: simbad:objects in 2024A&A...688A..29S and select 'bookmark this link' or equivalent in the popup menu