2025A&A...699A.361V


Query : 2025A&A...699A.361V

2025A&A...699A.361V - Astronomy and Astrophysics, volume 699A361 (2025/7-1)

JWST Observations of Young protoStars (JOYS) Overview of program and early results.

VAN DISHOECK E.F., TYCHONIEC L., ROCHA W.R.M., SLAVICINSKA K., FRANCIS L., VAN GELDER M.L., RAY T.P., BEUTHER H., CARATTI O GARATTI A., BRUNKEN N.G.C., CHEN Y., DEVARAJ R., GEERS V.C., GIESER C., GREENE T.P., JUSTTANONT K., LE GOUELLEC V.J.M., KAVANAGH P.J., KLAASSEN P.D., JANSSEN A.G.M., NAVARRO M.G., NAZARI P., NOTSU S., PEROTTI G., RESSLER M.E., REYES S.D., SELLEK A.D., TABONE B., TAP C., THEIJSSEN N.C.M.A., COLINA L., GUDEL M., HENNING T., LAGAGE P.-O., OSTLIN G., VANDENBUSSCHE B. and WRIGHT G.S.

Abstract (from CDS):

Context. The embedded phase of star formation is a crucial period in the development of a young star when the system still accretes matter, emerges from its natal cloud with assistance from powerful jets and outflows, and forms a disk, thus setting the stage for the birth of a planetary system. The mid-infrared spectral line observations now possible with unprecedented sensitivity, spectral resolution, and sharpness from the James Webb Space Telescope (JWST) are key for probing many of the physical and chemical processes on subarcsecond scales that occur in highly extincted regions. They provide unique diagnostics and complement millimeter observations.
Aims. The aim of the JWST Observations of Young protoStars (JOYS) program is to address a wide variety of topics ranging from protostellar accretion and the nature of primeval jets, winds, and outflows to the chemistry of gas and ice in hot cores and cold dense protostellar environments to the characteristics of the embedded disks. We introduce the JOYS program and show representative results.
Methods. The JWST Mid-InfraRed Instrument (MIRI) Medium Resolution Spectrometer (MRS) Integral Field Unit (IFU) 5-28 μm maps of 17 low-mass targets (23 if binary components are counted individually) and six high-mass protostellar sources were taken with resolving powers R = λ/Δλ = 1500-4000. We used small mosaics ranging from 1 × 1 to 3 × 3 MRS tiles to cover ~4″ to 20″ fields of view, providing spectral imaging on spatial scales down to ∼30 au (low mass) and ∼600 au (high mass). For HH 211, the complete ∼1' blue outflow lobe was mapped with the MRS. Atomic lines were interpreted with published shock models, whereas molecular lines were analyzed with simple rotation diagrams and local thermodynamic equilibrium slab models. We stress the importance of taking infrared pumping into account. Inferred abundance ratios were compared with detailed hot core chemical models including X-rays, whereas ice spectra were fit through comparison with laboratory spectra.
Results. The JWST MIRI-MRS spectra show a wide variety of features, with their spatial distribution providing key insight into their physical origin. The atomic line maps differ among refractory (e.g., Fe), semi-refractory (e.g., S), and volatile elements (e.g., Ne) and are linked to their different levels of depletion and local (shock) conditions. Jets are prominently seen in lines of [Fe II] and other refractory elements, whereas the pure rotational H2 lines probe hot (∼1000 K) and warm (few ×102 K) gas inside the cavity, as well as gas associated with jets, entrained outflows, and cavity walls for both low- and high-mass sources. Wide-angle winds are found in low-J H2 lines. Nested stratified jet structures containing an inner ionized core with an outer molecular layer are commonly seen in the youngest sources. While [S I] follows the jet as seen in [Fe II] in the youngest protostars, it is different in more evolved sources, where it is concentrated on source. Noble gas lines such as [Ne II] 12.8 μm reveal a mix of jet shock and photoionized emission. The H I recombination lines serve as a measure of protostellar accretion rates but are also associated with more extended jets. Gaseous molecular emission (CO2, C2H2, HCN, H2O, CH4, SO2, SiO) is seen toward several sources, but it is cool compared with what is found in more evolved disks, with excitation temperatures of only 100-250 K, and likely associated with the warm inner envelopes (“hot cores”). Along the outflow, CO2 is often extended, thus contrasting with C2H2 , which is usually centered on source. Water emission is commonly detected on source, even if relatively weak. Off source, it is seen only in the highest density shocks, such as those associated with NGC 1333 IRAS4B. Some sources show gaseous molecular lines in absorption, including NH3 in one case. Deep ice features are seen toward the protostars, revealing not just the major ice components but also ions (as part of salts) and complex organic molecules, with comparable abundances from low- to high-mass sources. The relative abundances of some gas and ice species are similar, which is consistent with ice sublimation in hot cores. We present a second detection of HDO ice in a solar-mass source, with an HDO/H2O ice ratio of ∼0.4%, thus providing a link with HDO/H2O in disks and comets. A deep search for solid O2 suggests that it is not a significant oxygen reservoir. Only a few embedded Class I disks show the same forest of water lines as Class II disks. This may be due to significant dust extinction of the upper layers in young disks caused by less settling of small dust as well as radial drift bringing in fresh dust.
Conclusions. This paper illustrates the wide range of science questions that a single MIRI-MRS IFU data set can address. Our data suggest many similarities between low- and high-mass sources. Large source samples across evolutionary stages and luminosities are needed to further develop these diagnostics of the physics and chemistry of protostellar systems.

Abstract Copyright: © The Authors 2025

Journal keyword(s): methods: laboratory: solid state - stars: formation - ISM: atoms - ISM: jets and outflows - ISM: molecules

Simbad objects: 64

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Number of rows : 64
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 LDN 1448 DNe 03 22.5 +30 35           ~ 546 0
2 IRAS F03226+3033 Y*O 03 25 38.83 +30 44 06.2           ~ 371 0
3 [SDA2014] West4 Y*O 03 25 38.83 +30 44 06.2           ~ 266 1
4 [JCC87] IRAS 2A Y*O 03 28 55.55 +31 14 36.7           ~ 513 3
5 [TLL2016] Per-emb-12-B Rad 03 29 10.4270 +31 13 32.099           ~ 9 0
6 [JCC87] IRAS 4A Y*O 03 29 10.49 +31 13 30.8           ~ 770 1
7 [TLL2016] Per-emb-12-A Rad 03 29 10.5370 +31 13 30.925           ~ 7 0
8 [JCC87] IRAS 4B Y*O 03 29 12.058 +31 13 02.05           ~ 625 0
9 NAME IRAS 4B1 South Y*O 03 29 12.06 +31 13 01.7           ~ 47 1
10 NAME IRAS 4B1 North Y*O 03 29 12.06 +31 13 05.4           ~ 15 0
11 [TLL2016] Per-emb-40-A Rad 03 33 16.6690 +31 07 54.902           ~ 5 0
12 2MASS J03331667+3107548 Y*O 03 33 16.68 +31 07 54.9           ~ 139 2
13 [TLL2016] Per-emb-40-B Rad 03 33 16.6800 +31 07 55.269           ~ 4 0
14 JCMTSE J033317.8+310932 cor 03 33 17.85 +31 09 31.9           ~ 140 0
15 [HKM99] B1-b cor 03 33 20.32 +31 07 21.5           ~ 242 0
16 [KJD2006] SMM J033335+31075 PoC 03 33 21.3 +31 07 28           ~ 118 0
17 NAME Perseus Cloud SFR 03 35.0 +31 13           ~ 1553 0
18 HH 211 Y*O 03 43 56.52 +32 00 52.8           ~ 414 0
19 SSTc2d J034444.0+320136 Y*O 03 44 43.955 +32 01 36.16           ~ 35 1
20 [EM98] DG Tau B cRN Y*O 04 27 02.66088 +26 05 30.4548           ~ 208 0
21 V* DF Tau TT* 04 27 02.7932020080 +25 42 22.453341516 11.97 12.25 11.42 10.31 9.14 M3Ve 528 1
22 IRAS 04365+2535 Y*O 04 39 35.19360 +25 41 44.7252           ~ 330 0
23 [HSW2018] L1527 Y*? 04 39 53.90 +26 03 09.6           ~ 3 0
24 IRAS 04368+2557 Y*O 04 39 53.97816 +26 03 09.6804           ~ 309 0
25 NAME Taurus Complex SFR 04 41.0 +25 52           ~ 4971 0
26 [ATH2005] IRAS 04381+2540 NIR A IR 04 41 12.65 +25 46 35.9           ~ 7 0
27 IRAS 04381+2540 Y*O 04 41 12.67920 +25 46 35.4216           K0-M2 133 1
28 [ATH2005] IRAS 04381+2540 NIR B IR 04 41 12.69 +25 46 36.0           ~ 3 0
29 TMC-1 MoC 04 41 45.9 +25 41 27           ~ 1872 0
30 2MASS J05352762-0509337 Y*O 05 35 27.622 -05 09 33.78           ~ 128 0
31 2MASS J08254384-5100326 Y*O 08 25 43.85 -51 00 32.7           ~ 327 1
32 [B2001b] IRS 2 Y*O 12 01 33.86688 -65 08 44.9232           ~ 42 0
33 [B2001b] IRS 1 Y*O 12 01 36.53040 -65 08 51.9180           ~ 167 0
34 BHR 71 MoC 12 01 37 -65 08.8           ~ 163 0
35 NAME BHR 71 MM HII 12 01 37.1 -65 08 54           ~ 47 0
36 IRAS 15398-3359 Y*? 15 43 02.21016 -34 09 07.7112       18.38 21.72 ~ 215 0
37 WL 20 TT* 16 27 15.69840 -24 38 43.4364           M0 86 0
38 YLW 16B Or* 16 27 29.43528 -24 39 16.1892           ~ 108 0
39 NAME Ophiuchus Molecular Cloud SFR 16 28 06 -24 32.5           ~ 3969 1
40 IRAS 16253-2429 FIR 16 28 22.2 -24 36 31           ~ 66 0
41 NAME IRAS 16293-2422B Y*O 16 32 22.63 -24 28 31.8           ~ 352 0
42 GAL 012.89+00.49 HII 18 11 51.3 -17 31 29           ~ 217 0
43 [LHM2019] Serpens Emb 8-c Y*? 18 29 48.030 +01 16 42.70           ~ 4 0
44 SH 2-68 N Y*O 18 29 48.09 +01 16 45.0           ~ 161 1
45 [LHM2019] Serpens Emb 8-b Y*? 18 29 48.130 +01 16 44.57           ~ 4 0
46 NAME Serpens Cloud SFR 18 29 49 +01 14.8           ~ 1195 1
47 GCNM 23 Y*O 18 29 49.63 +01 15 21.9           ~ 291 2
48 [CRM93] Knot E PoC 18 29 49.63 +01 15 22.3           ~ 4 0
49 [LHM2019] Serpens SMM1-b2 Y*? 18 29 49.660 +01 15 21.20           ~ 3 0
50 [LHM2019] Serpens SMM1-b1 Y*? 18 29 49.680 +01 15 21.09           ~ 3 0
51 [FJD2019] 10 mm 18 29 49.80 +01 15 20.3           ~ 2 0
52 NAME Serpens SMM 1a mm 18 29 49.80 +01 15 20.6           ~ 27 0
53 V* V371 Ser Or* 18 29 51.21240 +01 16 39.4860           ~ 132 1
54 NAME Serpens SMM 4 cor 18 29 57.1 +01 13 15           ~ 143 0
55 [EC89] SVS 4-5 Y*O 18 29 57.59 +01 13 00.6           ~ 38 1
56 IRAS 18274+0112 Y*O 18 29 57.73680 +01 14 05.6940           M4: 143 2
57 NAME SERPENS SMM 3 Y*O 18 29 59.28 +01 14 01.7           ~ 111 1
58 [TKB2013] C1-S cor 18 42 46.50 -04 04 16.0           ~ 18 0
59 AGAL G028.344+00.061 cor 18 42 50.45 -04 03 17.7           ~ 93 0
60 NAME Dragon Nebula DNe 18 42 50.6 -04 03 30           ~ 177 0
61 AGAL G028.398+00.081 cor 18 42 51.86 -03 59 43.3           ~ 60 0
62 [WZP2008] IRS 2 IR 18 42 51.92 -03 59 54.0           ~ 5 0
63 IRAS 18449-0115 cor 18 47 34.27 -01 12 43.2           ~ 430 1
64 Mol 160 Rad 23 40 54.5 +61 10 28           ~ 121 0

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