TY - JOUR
T1 - IPA
T2 - Class 0 Protostars Viewed in CO Emission Using JWST
AU - Rubinstein, Adam E.
AU - Evans, Neal J.
AU - Tyagi, Himanshu
AU - Narang, Mayank
AU - Nazari, Pooneh
AU - Gutermuth, Robert
AU - Federman, Samuel
AU - Manoj, P.
AU - Green, Joel D.
AU - Watson, Dan M.
AU - Megeath, S. Thomas
AU - Rocha, Will R.M.
AU - Brunken, Nashanty G.C.
AU - Slavicinska, Katerina
AU - van Dishoeck, Ewine F.
AU - Beuther, Henrik
AU - Bourke, Tyler L.
AU - o Garatti, Alessio Caratti
AU - Hartmann, Lee
AU - Klaassen, Pamela
AU - Linz, Hendrik
AU - Looney, Leslie W.
AU - Muzerolle, James
AU - Stanke, Thomas
AU - Tobin, John J.
AU - Wolk, Scott J.
AU - Yang, Yao Lun
N1 - Support for A.E.R., D.M.W., R.G., S.F., S.T.M., W.F., J.G., and J.J.T. in program #1802 was provided by NASA through a grant from the STScI, which is operated by the Association of Universities for Research in Astronomy, Inc., under NASA contract NAS 5-03127. N.J.E. thanks the University of Texas at Austin for research support. P.N. acknowledges support by the NWO grant 618.000.001, Danish National Research Foundation (grant agreement No. DNRF150) and ESO. A.C.G. acknowledges from PRIN-MUR 2022 20228JPA3A \u201CThe path to star and planet formation in the JWST era (PATH)\u201D and by INAF-GoG 2022 \u201CNIR-dark Accretion Outbursts in Massive Young stellar objects (NAOMY)\u201D and Large Grant INAF 2022 \u201CYSOs Outflows, Disks and Accretion: toward a global framework for the evolution of planet-forming systems (YODA).\u201D E.F.vD. and W.R.M.R. are supported by EU A-ERC grant 101019751 MOLDISK Fellowship Program.
PY - 2024/10/1
Y1 - 2024/10/1
N2 - 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, 13CO is undetected, indicating that 12CO emission is optically thin. We use H2 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 ∼104 K), while one hotter component is required for v = 2 (≳3500 K). 13CO is depleted compared to the abundances found in the interstellar medium, indicating selective UV photodissociation of 13CO; 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 ∼1022 g for the lowest mass protostars to ∼1026 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.
AB - 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, 13CO is undetected, indicating that 12CO emission is optically thin. We use H2 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 ∼104 K), while one hotter component is required for v = 2 (≳3500 K). 13CO is depleted compared to the abundances found in the interstellar medium, indicating selective UV photodissociation of 13CO; 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 ∼1022 g for the lowest mass protostars to ∼1026 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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U2 - 10.3847/1538-4357/ad6b92
DO - 10.3847/1538-4357/ad6b92
M3 - Article
AN - SCOPUS:85206476354
SN - 0004-637X
VL - 974
JO - Astrophysical Journal
JF - Astrophysical Journal
IS - 1
M1 - 112
ER -