TY - JOUR
T1 - Early Planet Formation in Embedded Disks (eDisk). VI. Kinematic Structures around the Very-low-mass Protostar IRAS 16253-2429
AU - Aso, Yusuke
AU - Kwon, Woojin
AU - Ohashi, Nagayoshi
AU - Jørgensen, Jes K.
AU - Tobin, John J.
AU - Aikawa, Yuri
AU - de Gregorio-Monsalvo, Itziar
AU - Han, Ilseung
AU - Kido, Miyu
AU - Koch, Patrick M.
AU - Lai, Shih Ping
AU - Lee, Chang Won
AU - Lee, Jeong Eun
AU - Li, Zhi Yun
AU - Lin, Zhe Yu Daniel
AU - Looney, Leslie W.
AU - Narayanan, Suchitra
AU - Phuong, Nguyen Thi
AU - Insa Choi, Jinshi Sai
AU - Saigo, Kazuya
AU - Santamaría-Miranda, Alejandro
AU - Sharma, Rajeeb
AU - Takakuwa, Shigehisa
AU - Thieme, Travis J.
AU - Tomida, Kengo
AU - Williams, Jonathan P.
AU - Yen, Hsi Wei
N1 - This paper makes use of the following ALMA data: ADS/JAO.ALMA#2019.1.00261.L and ADS/JAO.ALMA#2019.A.00034.S. ALMA is a partnership of ESO (representing its member states), NSF (USA) and NINS (Japan), together with NRC (Canada), MOST and ASIAA (Taiwan), and KASI (Republic of Korea), in cooperation with the Republic of Chile. The Joint ALMA Observatory is operated by ESO, AUI/NRAO, and NAOJ. The National Radio Astronomy Observatory is a facility of the National Science Foundation operated under cooperative agreement by Associated Universities, Inc. W.K. was supported by the National Research Foundation of Korea (NRF) grant funded by the Korean Government (MSIT; grant No. NRF-2021R1F1A1061794). N.O. acknowledges support from the National Science and Technology Council (NSTC) in Taiwan through the grant Nos. NSTC 109-2112-M-001-051 and 110-2112-M-001-031. J.K.J. acknowledges support from the Independent Research Fund Denmark (grant No. 0135-00123B). J.J.T. acknowledges support from NASA XRP 80NSSC22K1159. Y.A. acknowledges support by NAOJ ALMA Scientific Research Grant code 2019-13B, Grant-in-Aid for Scientific Research (S) 18H05222, and Grant-in-Aid for Transformative Research Areas (A) 20H05844 and 20H05847. I.d.G. acknowledges support from grant No. PID2020-114461GB-I00, funded by MCIN/AEI/10.13039/501100011033. P.M.K. acknowledges support from NSTC 108-2112- M-001-012, NSTC 109-2112-M-001-022, and NSTC 110-2112-M-001-057. S.P.L. and T.J.T. acknowledge grants from the National Science and Technology Council of Taiwan, grant Nos. 106-2119-M-007-021-MY3 and 109-2112-M-007-010-MY3. C.W.L. is supported by the Basic Science Research Program through the National Research Foundation of Korea (NRF) funded by the Ministry of Education, Science and Technology (grant No. NRF- 2019R1A2C1010851), and by the Korea Astronomy and Space Science Institute grant funded by the Korean Government (MSIT; Project No. 2022-1-840-05). J.E.L. was supported by the National Research Foundation of Korea (NRF) grant funded by the Korean Government (MSIT; grant No. 2021R1A2C1011718). Z.Y.L. is supported in part by NASA grant Nos. 80NSSC20K0533 and NSF AST-1910106. Z.Y.D.L. acknowledges support from NASA grant No. 80NSSC18K1095, the Jefferson Scholars Foundation, the NRAO ALMA Student Observing Support (SOS) SOSPA8-003, the Achievements Rewards for College Scientists (ARCS) Foundation Washington Chapter, the Virginia Space Grant Consortium (VSGC), and UVA research computing (RIVANNA). L.W.L. acknowledges support from NSF AST-2108794. S.N. acknowledges support from the National Science Foundation through the Graduate Research Fellowship Program under grant No. 2236415. Any opinions, findings, conclusions, or recommendations expressed in this material are those of the authors and do not necessarily reflect the views of the National Science Foundation. K.S. is supported by JSPS KAKENHI grant No. 21H04495. R.S. acknowledges support from the Independent Research Fund Denmark (grant No. 0135-00123B). S.T. is supported by JSPS KAKENHI grant Nos. 21H00048 and 21H04495, and by NAOJ ALMA Scientific Research grant No. 2022-20A. J.P.W. acknowledges support from NSF AST-2107841. H.-W.Y. acknowledges support from the National Science and Technology Council (NSTC) in Taiwan through grant No. NSTC 110-2628-M-001-003-MY3 and from the Academia Sinica Career Development Award (AS-CDA-111-M03).
PY - 2023/9/1
Y1 - 2023/9/1
N2 - Precise estimates of protostellar masses are crucial to characterize the formation of stars of low masses down to brown dwarfs (BDs; M * < 0.08 M ☉). The most accurate estimation of protostellar mass uses the Keplerian rotation in the circumstellar disk around the protostar. To apply the Keplerian rotation method to a protostar at the low-mass end, we have observed the Class 0 protostar IRAS 16253-2429 using the Atacama Large Millimeter/submillimeter Array (ALMA) in the 1.3 mm continuum at an angular resolution of 0.″07 (10 au), and in the 12CO, C18O, 13CO (J = 2-1), and SO (J N = 65−54) molecular lines, as part of the ALMA Large Program Early Planet Formation in Embedded Disks project. The continuum emission traces a nonaxisymmetric, disk-like structure perpendicular to the associated 12CO outflow. The position-velocity (PV) diagrams in the C18O and 13CO lines can be interpreted as infalling and rotating motions. In contrast, the PV diagram along the major axis of the disk-like structure in the 12CO line allows us to identify Keplerian rotation. The central stellar mass and the disk radius are estimated to be ∼0.12-0.17 M ☉ and ∼13-19 au, respectively. The SO line suggests the existence of an accretion shock at a ring (r ∼ 28 au) surrounding the disk and a streamer from the eastern side of the envelope. IRAS 16253-2429 is not a proto-BD but has a central stellar mass close to the BD mass regime, and our results provide a typical picture of such very-low-mass protostars.
AB - Precise estimates of protostellar masses are crucial to characterize the formation of stars of low masses down to brown dwarfs (BDs; M * < 0.08 M ☉). The most accurate estimation of protostellar mass uses the Keplerian rotation in the circumstellar disk around the protostar. To apply the Keplerian rotation method to a protostar at the low-mass end, we have observed the Class 0 protostar IRAS 16253-2429 using the Atacama Large Millimeter/submillimeter Array (ALMA) in the 1.3 mm continuum at an angular resolution of 0.″07 (10 au), and in the 12CO, C18O, 13CO (J = 2-1), and SO (J N = 65−54) molecular lines, as part of the ALMA Large Program Early Planet Formation in Embedded Disks project. The continuum emission traces a nonaxisymmetric, disk-like structure perpendicular to the associated 12CO outflow. The position-velocity (PV) diagrams in the C18O and 13CO lines can be interpreted as infalling and rotating motions. In contrast, the PV diagram along the major axis of the disk-like structure in the 12CO line allows us to identify Keplerian rotation. The central stellar mass and the disk radius are estimated to be ∼0.12-0.17 M ☉ and ∼13-19 au, respectively. The SO line suggests the existence of an accretion shock at a ring (r ∼ 28 au) surrounding the disk and a streamer from the eastern side of the envelope. IRAS 16253-2429 is not a proto-BD but has a central stellar mass close to the BD mass regime, and our results provide a typical picture of such very-low-mass protostars.
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U2 - 10.3847/1538-4357/ace624
DO - 10.3847/1538-4357/ace624
M3 - Article
AN - SCOPUS:85170027394
SN - 0004-637X
VL - 954
JO - Astrophysical Journal
JF - Astrophysical Journal
IS - 1
M1 - 101
ER -