The Astrophysical Journal (Jan 2024)

IPA: Class 0 Protostars Viewed in CO Emission Using JWST

  • Adam E. Rubinstein,
  • Neal J. Evans II,
  • Himanshu Tyagi,
  • Mayank Narang,
  • Pooneh Nazari,
  • Robert Gutermuth,
  • Samuel Federman,
  • P. Manoj,
  • Joel D. Green,
  • Dan M. Watson,
  • S. Thomas Megeath,
  • Will R. M. Rocha,
  • Nashanty G. C. Brunken,
  • Katerina Slavicinska,
  • Ewine F. van Dishoeck,
  • Henrik Beuther,
  • Tyler L. Bourke,
  • Alessio Caratti o Garatti,
  • Lee Hartmann,
  • Pamela Klaassen,
  • Hendrik Linz,
  • Leslie W. Looney,
  • James Muzerolle,
  • Thomas Stanke,
  • John J. Tobin,
  • Scott J. Wolk,
  • Yao-Lun Yang

DOI
https://doi.org/10.3847/1538-4357/ad6b92
Journal volume & issue
Vol. 974, no. 1
p. 112

Abstract

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We investigate the bright CO fundamental emission in the central regions of five protostars in their primary mass assembly phase using new observations from JWST’s Near-Infrared Spectrograph and Mid-Infrared Instrument. CO line emission images and fluxes are extracted for a forest of ∼150 rovibrational transitions from two vibrational bands, v = 1−0 and v = 2−1. However, ^13 CO is undetected, indicating that ^12 CO emission is optically thin. We use H _2 emission lines to correct fluxes for extinction and then construct rotation diagrams for the CO lines with the highest spectral resolution and sensitivity to estimate rotational temperatures and numbers of CO molecules. Two distinct rotational temperature components are required for v = 1 (∼600 to 1000 K and 2000 to ∼10 ^4 K), while one hotter component is required for v = 2 (≳3500 K). ^13 CO is depleted compared to the abundances found in the interstellar medium, indicating selective UV photodissociation of ^13 CO; therefore, UV radiative pumping may explain the higher rotational temperatures in v = 2. The average vibrational temperature is ∼1000 K for our sources and is similar to the lowest rotational temperature components. Using the measured rotational and vibrational temperatures to infer a total number of CO molecules, we find that the total gas masses range from lower limits of ∼10 ^22 g for the lowest mass protostars to ∼10 ^26 g for the highest mass protostars. Our gas mass lower limits are compatible with those in more evolved systems, which suggest the lowest rotational temperature component comes from the inner disk, scattered into our line of sight, but we also cannot exclude the contribution to the CO emission from disk winds for higher mass targets.

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