2025A&A...703A.139S


Query : 2025A&A...703A.139S

2025A&A...703A.139S - Astronomy and Astrophysics, volume 703A139 (2025/11-1)

UV-irradiated outflows from low-mass protostars in Ophiuchus with JWST/MIRI.

SKRETAS I.M., KARSKA A., FRANCIS L., ROCHA W.R.M., VAN GELDER M.L., TYCHONIEC L., FIGUEIRA M., SEWILO M., WYROWSKI F. and SCHILKE P.

Abstract (from CDS):

Context. The main accretion phase of protostars is characterized by the ejection of material in the form of bipolar jets and outflows. In addition, external UV irradiation can potentially have a significant impact on the excitation conditions within these outflows. High-resolution observations in the mid-infrared (mid-IR) allow us to investigate the details of those energetic processes through the emission of shock-excited H2.
Aims. Our aim is to spatially resolve H2, ionic, and atomic emission within the outflows of low-mass protostars, and investigate its origin in connection to shocks influenced by external ultraviolet irradiation.
Methods. We analyze spectral maps of 5 Class I protostars in the Ophiuchus molecular cloud from the James Webb Space Telescope (JWST) Medium Resolution Spectrometer (MIRI/MRS). The MIRI/MRS field of view covers an area between ∼3.2″ × 3.7″ at 6 μm and 6.6″ × 7.7″ at 25 μm and with a resolution of ∼0.3 to 1″, corresponding to spatial scales of a few hundred astronomical units.
Results. Four out of five protostars in our sample show strong H2, [Ne II], and [Fe II] emission associated with outflows and jets. Pure rotational H2 transitions from S(1) to S(8) are found and show two distinct temperature components on Boltzmann diagrams with rotational temperatures of ∼500-600 K and ∼1000-3000 K, respectively. Both C-type shocks propagating at high pre-shock densities (nH ≥ 104 cm–3) and J-type shocks at low pre-shock densities (nH ≤ 103 cm–3) reproduce the observed line ratios. However, only C-type shocks produce sufficiently high column densities of H2, whereas predictions from a single J-type shock reproduce the observed rotational temperatures of the gas better. A combination of various types of shocks could play a role in protostellar outflows as long as UV irradiation is included in the models. The origin of this radiation is likely internal, since no significant differences in the excitation conditions of outflows are seen at various locations in the cloud.
Conclusions. Observations with MIRI offer an unprecedented view of protostellar outflows, allowing us to determine the properties of outflowing gas even at very close distances to the driving source. Further constraints on the physical conditions within outflows can be placed thanks to the possibility of direct comparisons of such observations with state-of-the-art shock models.

Abstract Copyright: © The Authors 2025

Journal keyword(s): shock waves - stars: formation - stars: jets - stars: protostars - stars: winds - outflows - ISM: jets and outflows

Simbad objects: 29

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Number of rows : 29
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 NGC 1333 OpC 03 29 09.2 +31 20 59           ~ 1575 1
3 HH 211 Y*O 03 43 56.52 +32 00 52.8           ~ 414 0
4 V* DG Tau TT* 04 27 04.6921275888 +26 06 16.060169268 13.57 13.97 10.50 12.28   K6Ve 1092 1
5 IRAS 04365+2535 Y*O 04 39 35.19360 +25 41 44.7252           ~ 330 0
6 TMC-1 MoC 04 41 45.9 +25 41 27           ~ 1872 0
7 TMC-1E PoC 04 41 53.8 +25 36 26           ~ 12 0
8 2MASS J05352762-0509337 Y*O 05 35 27.622 -05 09 33.78           ~ 128 0
9 NGC 2071 RNe 05 47 10 +00 18.0           ~ 661 1
10 2MASS J08254384-5100326 Y*O 08 25 43.85 -51 00 32.7           ~ 327 1
11 BHR 71 MoC 12 01 37 -65 08.8           ~ 163 0
12 NAME Upper Sco-Cen As* 16 15 -24.2           ~ 1497 1
13 * sig Sco bC* 16 21 11.3157134 -25 35 34.051476 2.32 3.02 2.89 1.69 1.58 B1III+B1:V 898 0
14 HD 147889 Or* 16 25 24.3163637976 -24 27 56.569805208 8.56 8.73 7.90     B2V 512 1
15 * rho Oph ** 16 25 35.11766 -23 26 49.8150 4.30 4.85 4.63 4.27 3.96 B2IV+B2V 670 0
16 CRBR 2315.8-1700 Y*O 16 26 17.22936 -24 23 45.3660           ~ 47 0
17 GSS 30 Y*O 16 26 21.38160 -24 23 04.0524           ~ 223 1
18 NAME rho Oph A Cloud MoC 16 26 26.4 -24 22 33           ~ 312 1
19 GSS 35 TT* 16 26 34.1761719864 -24 23 28.283473860     16.53 14.75 12.51 B3 254 1
20 NAME rho Oph E MoC 16 27 02.0 -24 38 31           ~ 65 0
21 [GY92] 197 Y*O 16 27 05.24616 -24 36 29.7936           ~ 74 1
22 WL 17 Y*O 16 27 06.77616 -24 38 14.9964           ~ 113 0
23 CRBR 2422.8-3423 Y*O 16 27 24.61320 -24 41 03.4080           ~ 101 1
24 NAME rho Oph F MoC 16 27 37.3 -24 42 28           ~ 65 0
25 HD 147899 * 16 27 49.1989560744 -58 17 30.977880684   10.41 10.33     B9/A0V 8 0
26 NAME Ophiuchus Molecular Cloud SFR 16 28 06 -24 32.5           ~ 3969 1
27 * alf Sco s*r 16 29 24.45970 -26 25 55.2094 4.08 2.75 0.91 -0.64 -1.87 M1.5Iab+B2Vn 786 0
28 LDN 1689 DNe 16 32 22.5 -24 28 29           ~ 153 0
29 LDN 1157 DNe 20 39 06.4 +68 02 13           ~ 606 0

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