IPA. Accretion rate of a low-mass Class 0 protostar, measured via mid-infrared fluorescent OH emission
astro-ph.SR
/ Authors
Dan M. Watson, Mayank Narang, Caeley V. Pittman, Himanshu Tyagi, Robert Gutermuth, Adam E. Rubinstein, Neal J. Evans, Lee W. Hartmann, S. Thomas Megeath, P. Manoj
and 34 more authors
Catherine C. Espaillat, Nuria Calvet, Alessio Caratti o Garatti, Ewine F. van Dishoeck, Tyler L. Bourke, Joel D. Green, Carey M. Lisse, Pamela Klaassen, Leslie W. Looney, Pooneh Nazari, David A. Neufeld, John J. Tobin, Scott J. Wolk, Guillem Anglada, Prabhani Atnagulov, Henrik Beuther, Nashanty G. C. Brunken, Samuel Federman, Elise Furlan, Nolan Habel, Nicole Karnath, Hendrik Linz
/ Abstract
The earliest stages of star formation are highlighted by complex interactions between accretion, outflow, and radiative processes, which shape the chemical and physical environment of the emerging protostar. James Webb Space Telescope observations of the low-mass, low-luminosity Class 0 protostar IRAS 16253-2429 reveal a central compact source. This object exhibits a rich mid-infrared emission spectrum of OH pure rotational lines and $\rm CO_2$ ro-vibrational lines. Unusually for a young stellar object, it has no mid-infrared line emission from $\rm H_2O$ to match the other molecules. We demonstrate that the emitting OH molecules arise from UV photodissociation of $\rm H_2O$ in its second absorption band at $λ= 114-145$ nm, and that the OH emission is a fluorescent cascade starting with highest-excitation rotational states. This situation offers the opportunity of using the infrared OH spectrum to measure the UV flux from the central protostar. Thereby we determine the disk-star accretion rate to be $3 \times 10^{-10} \ M_\sun \ {\rm year^{-1}}$, and demonstrate that the system luminosity arises mostly from the protostar's photosphere rather than from accretion luminosity. The result is in accord with the measured outflow rate of IRAS 16253-2429 and lies within the outflow/accretion-flow rate trend often inferred for protostars; and with episodic accretion as the dominant mechanism by which this protostar has grown.