Discovery of a Collimated Jet from the Low-luminosity Protostar IRAS 16253−2429 in a Quiescent Accretion Phase with the JWST

Author:

Narang MayankORCID,Manoj P.ORCID,Tyagi HimanshuORCID,Watson Dan M.ORCID,Megeath S. ThomasORCID,Federman SamuelORCID,Rubinstein Adam E.ORCID,Gutermuth RobertORCID,Caratti o Garatti AlessioORCID,Beuther HenrikORCID,Bourke Tyler L.ORCID,Van Dishoeck Ewine F.ORCID,Evans Neal J.ORCID,Anglada GuillemORCID,Osorio MayraORCID,Stanke ThomasORCID,Muzerolle JamesORCID,Looney Leslie W.ORCID,Yang Yao-LunORCID,Klaassen PamelaORCID,Karnath NicoleORCID,Atnagulov PrabhaniORCID,Brunken NashantyORCID,Fischer William J.ORCID,Furlan EliseORCID,Green JoelORCID,Habel NolanORCID,Hartmann LeeORCID,Linz HendrikORCID,Nazari PoonehORCID,Pokhrel RiwajORCID,Rahatgaonkar RohanORCID,Rocha Will R. M.ORCID,Sheehan PatrickORCID,Slavicinska KaterinaORCID,Stutz Amelia M.ORCID,Tobin John J.ORCID,Tychoniec LukaszORCID,Wolk ScottORCID

Abstract

Abstract Investigating Protostellar Accretion (IPA) is a JWST Cycle 1 GO program that uses NIRSpec integral field units and MIRI Medium Resolution Spectrograph to obtain 2.9–28 μm spectral cubes of young, deeply embedded protostars with luminosities of 0.2–10,000 L and central masses of 0.15–12 M . In this Letter, we report the discovery of a highly collimated atomic jet from the Class 0 protostar IRAS 16253−2429, the lowest-luminosity source (L bol = 0.2 L ) in the IPA program. The collimated jet is detected in multiple [Fe ii] lines and [Ne ii], [Ni ii], and H i lines but not in molecular emission. The atomic jet has a velocity of about 169 ± 15 km s−1, after correcting for inclination. The width of the jet increases with distance from the central protostar from 23 to 60 au, corresponding to an opening angle of 2.°6 ± 0.°5. By comparing the measured flux ratios of various fine-structure lines to those predicted by simple shock models, we derive a shock speed of 54 km s−1 and a preshock density of 2.0 × 103 cm−3 at the base of the jet. From these quantities and using a suite of jet models and extinction laws, we compute a mass-loss rate between 0.4 and 1.1 ×10−10 M yr −1. The low mass-loss rate is consistent with simultaneous measurements of low mass accretion rate (2.4 ± 0.8 × 10−9 M yr−1) for IRAS 16253−2429 from JWST observations, indicating that the protostar is in a quiescent accretion phase. Our results demonstrate that very low-mass protostars can drive highly collimated, atomic jets, even during the quiescent phase.

Publisher

American Astronomical Society

Subject

Space and Planetary Science,Astronomy and Astrophysics

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