TY - JOUR
T1 - Can high-velocity protostellar jets help to drive low-velocity outflow?
AU - Machida, Masahiro N.
N1 - Funding Information:
This study was supported by JSPS KAKENHI Grant (JP17H06360, JP17K0538faa7, JP17KK0096, JP21H00046, JP21K03617: MNM).
Publisher Copyright:
© 2021 The Author(s).
PY - 2021/12/1
Y1 - 2021/12/1
N2 - Using three-dimensional magnetohydrodynamics simulations, the driving of protostellar jets is investigated in different star-forming cores with the parameters of magnetic field strength and mass accretion rate. Powerful high-velocity jets appear in strongly magnetized clouds when the mass accretion rate on to the protostellar system is lower than M ≤ 10-4 M⊙ yr-1. On the other hand, even at this mass accretion rate range, no jets appear for magnetic fields of prestellar clouds as weak as μ0 ≤5-10, where μ0 is the mass-to-flux ratio normalized by the critical value (2πG1/2)-1. For M ≥ 10-4 M⊙ yr-1, although jets usually appear just after protostar formation independent of the magnetic field strength, they soon weaken and finally disappear. Thus, they cannot help drive the low-velocity outflow when there is no low-velocity flow just before protostar formation. As a result, no significant mass ejection occurs during the early mass accretion phase either when the prestellar cloud is weaky magnetized or when the mass accretion rate is very high. Thus, protostars formed in such environments would trace different evolutionary paths from the normal star formation process.
AB - Using three-dimensional magnetohydrodynamics simulations, the driving of protostellar jets is investigated in different star-forming cores with the parameters of magnetic field strength and mass accretion rate. Powerful high-velocity jets appear in strongly magnetized clouds when the mass accretion rate on to the protostellar system is lower than M ≤ 10-4 M⊙ yr-1. On the other hand, even at this mass accretion rate range, no jets appear for magnetic fields of prestellar clouds as weak as μ0 ≤5-10, where μ0 is the mass-to-flux ratio normalized by the critical value (2πG1/2)-1. For M ≥ 10-4 M⊙ yr-1, although jets usually appear just after protostar formation independent of the magnetic field strength, they soon weaken and finally disappear. Thus, they cannot help drive the low-velocity outflow when there is no low-velocity flow just before protostar formation. As a result, no significant mass ejection occurs during the early mass accretion phase either when the prestellar cloud is weaky magnetized or when the mass accretion rate is very high. Thus, protostars formed in such environments would trace different evolutionary paths from the normal star formation process.
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U2 - 10.1093/mnras/stab2626
DO - 10.1093/mnras/stab2626
M3 - Article
AN - SCOPUS:85119482034
SN - 0035-8711
VL - 508
SP - 3208
EP - 3225
JO - Monthly Notices of the Royal Astronomical Society
JF - Monthly Notices of the Royal Astronomical Society
IS - 3
ER -