TY - JOUR
T1 - The Co-evolution of Disks and Stars in Embedded Stages
T2 - The Case of the Very-low-mass Protostar IRAS 15398-3359
AU - Okoda, Yuki
AU - Oya, Yoko
AU - Sakai, Nami
AU - Watanabe, Yoshimasa
AU - Jrgensen, Jes K.
AU - Van Dishoeck, Ewine F.
AU - Yamamoto, Satoshi
N1 - Funding Information:
This paper makes use of the following ALMA data set: ADS/ JAO.ALMA#2013.1.01157.S. ALMA is a partnership of the ESO (representing its member states), the NSF (USA), and NINS (Japan), together with the NRC (Canada) and the NSC and ASIAA (Taiwan), in cooperation with the Republic of Chile. The Joint ALMA Observatory is operated by the ESO, the AUI/ NRAO, and the NAOJ. The authors are grateful to the ALMA staff for their excellent support. This study is supported by Grants-in-Aid from the Ministry of Education, Culture, Sports, Science, and Technologies of Japan (25108005 and 18H05222). J.K.J. acknowledges support from the European Research Council (ERC) under the European Union’s Horizon 2020 research and innovation programme (grant agreement No. 646908) through ERC Consolidator Grant ”S4F”. Research at Centre for Star and Planet Formation is funded by the Danish National Research Foundation. E.v.D. is supported by EU A-ERC grant 291141 CHEMPLAN. Yuki Okoda thanks the Advanced Leading Graduate Course for Photon Science (ALPS) for financial support.
Publisher Copyright:
© 2018. The American Astronomical Society. All rights reserved..
PY - 2018/9/10
Y1 - 2018/9/10
N2 - We have observed the CCH (N = 3-2, J = 7/2-5/2, F = 4-3 and 3-2) and SO (67-56) emission at a 0.″2 angular resolution toward the low-mass Class 0 protostellar source IRAS 15398-3359 with ALMA. The CCH emission traces the infalling-rotating envelope near the protostar with the outflow cavity extended along the northeast-southwest axis. On the other hand, the SO emission has a compact distribution around the protostar. The CCH emission is relatively weak at the continuum peak position, while the SO emission has a sharp peak there. Although the maximum velocity shift of the CCH emission is about 1 km s-1 from the systemic velocity, a velocity shift higher than 2 km s-1 is seen for the SO emission. This high-velocity component is most likely associated with the Keplerian rotation around the protostar. The protostellar mass is estimated to be from the velocity profile of the SO emission. With this protostellar mass, the velocity structure of the CCH emission can be explained by the model of the infalling-rotating envelope, where the radius of the centrifugal barrier is estimated to be 40 au from the comparison with the model. The disk mass evaluated from the dust continuum emission by assuming the dust temperature of 20-100 K is 0.1-0.9 times the stellar mass, resulting in the Toomre Q parameter of 0.4-5. Hence, the disk structure may be partly unstable. All these results suggest that a rotationally supported disk can form in the earliest stages of the protostellar evolution.
AB - We have observed the CCH (N = 3-2, J = 7/2-5/2, F = 4-3 and 3-2) and SO (67-56) emission at a 0.″2 angular resolution toward the low-mass Class 0 protostellar source IRAS 15398-3359 with ALMA. The CCH emission traces the infalling-rotating envelope near the protostar with the outflow cavity extended along the northeast-southwest axis. On the other hand, the SO emission has a compact distribution around the protostar. The CCH emission is relatively weak at the continuum peak position, while the SO emission has a sharp peak there. Although the maximum velocity shift of the CCH emission is about 1 km s-1 from the systemic velocity, a velocity shift higher than 2 km s-1 is seen for the SO emission. This high-velocity component is most likely associated with the Keplerian rotation around the protostar. The protostellar mass is estimated to be from the velocity profile of the SO emission. With this protostellar mass, the velocity structure of the CCH emission can be explained by the model of the infalling-rotating envelope, where the radius of the centrifugal barrier is estimated to be 40 au from the comparison with the model. The disk mass evaluated from the dust continuum emission by assuming the dust temperature of 20-100 K is 0.1-0.9 times the stellar mass, resulting in the Toomre Q parameter of 0.4-5. Hence, the disk structure may be partly unstable. All these results suggest that a rotationally supported disk can form in the earliest stages of the protostellar evolution.
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U2 - 10.3847/2041-8213/aad8ba
DO - 10.3847/2041-8213/aad8ba
M3 - Article
AN - SCOPUS:85053475005
SN - 2041-8205
VL - 864
JO - Astrophysical Journal Letters
JF - Astrophysical Journal Letters
IS - 2
M1 - L25
ER -