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Investigating the Nested Structure of the Outflow from the Low Luminosity Protostar IRAS 16253-2429 Using JWST and ALMA

Mayank Narang*, Himanshu Tyagi, Nagayoshi Ohashi, P. Manoj, S. Thomas Megeath, John J. Tobin, Ewine F. Van Dishoeck, Neal J. Evans II, Dan M. Watson, Alessio Caratti O Garatti, Jes K. Jorgensen, Robert Gutermuth, Yusuke Aso, Henrik Beuther, Leslie W. Looney, David A. Neufeld, Guillem Anglada, Mayra Osorio, Adam E. Rubinstein, Samuel FedermanLee W. Hartmann, Pooneh Nazari, Nicole Karnath, Hendrik Linz, Thomas Stanke, Tyler L. Bourke, Yao-Lun Yang, Rolf Kuiper, Joel Green, Pamela Klaassen, Wafa Zakri, Nolan Habel, Nashanty Brunken, James Muzerolle, Katerina Slavicinska, Amelia M. Stutz, Lukasz Tychoniec, Scott Wolk, Will R. M. Rocha, William J. Fischer

*Corresponding author for this work

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Abstract

Understanding the earliest stage of star and planet formation requires detailed observations to address the connection and interplay between the accretion, outflow, and disk evolution. We present results from the observations of the low luminosity (Lbol similar to 0.2 L circle dot) and mass (M* similar to 0.15 M circle dot) Class 0 protostar IRAS 16253-2429, conducted as part of the eDisk Atacama Large Millimeter/submillimeter Array (ALMA) large program and the JWST cycle-1 GO Investigating Protostellar Accretion program. Observations reveal a wide hourglass-shaped continuum cavity traced in scattered light (at <= 5 mu m), with a brighter, extended northern side. We detect 15 pure rotational H2 transitions (Eup: 1015-21411 K), revealing a wide-angle molecular outflow. The outflow width (as traced in H2 0-0 S(11)) at the protostellar location measures <= 35 au, slightly larger than the dust and Keplerian disk diameters (similar to 30 au) but wider than the 20-23 au jet width in [Fe II]. The opening angle narrows from 40 degrees to 35 degrees for the low-J H2 lines (up to S(5)) and the cold gas component (ALMA 12CO) to similar to 28 degrees-19 degrees for the high-J H2 lines (S(7)-S(11)). Position-velocity diagrams of H2 reveal higher velocities for higher Eup, ranging from 12.5 km s-1 for H2 0-0 S(1) and S(2) to 28.5 km s-1 for H2 0-0 S(5) and S(7) with respect to the mean flow velocity. The nested excitation and velocity structure of the collimated jet and wide-angle wind suggest a magnetohydrodynamic wind as a likely launching mechanism, similar to the findings in other protostars and Class II sources. The lower velocity millimeter CO may be gas from the infalling envelope accelerated outwards by the wide-angle wind along the cavity walls.
Original languageEnglish
Article number184
JournalAstrophysical Journal
Volume1000
Issue number2
Number of pages17
ISSN0067-0049
DOIs
Publication statusPublished - 23 Mar 2026

Keywords

  • Early planet formation
  • Magnetocentrifugally driven flows
  • Webb-space-telescope
  • Nearby dense cores
  • Spitzer c2d survey
  • Young stars
  • Embedded disks
  • Bipolar outflows
  • Unified model
  • Accretion disks

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