TY - GEN
T1 - Low-Mass Star Formation
T2 - 6th Zermatt Symposium on Conditions and Impact of Star Formation: From Lab to Space 2015
AU - Inutsuka, S. I.
AU - Machida, M.
AU - Matsumoto, T.
AU - Tsukamoto, Y.
AU - Iwasaki, K.
N1 - Publisher Copyright:
© 2016 EAS, EDP Sciences.
PY - 2016/5/20
Y1 - 2016/5/20
N2 - This review describes realistic evolution of magnetic field and rotation of the protostars, dynamics of outflows and jets, and the formation and evolution of protoplanetary disks. Recent advances in the protostellar collapse simulations cover a huge dynamic range from molecular cloud core density to stellar density in a self-consistent manner and account for all the non-ideal magnetohydrodynamical effects, such as Ohmic resistivity, ambipolar diffusion, and Hall current. We explain the emergence of the first core, i.e., the quasi-hydrostatic object that consists of molecular gas, and the second core, i.e., the protostar. Ohmic dissipation largely removes the magnetic flux from the center of a collapsing cloud core. A fast well-collimated bipolar jet along the rotation axis of the protostar is driven after the magnetic field is re-coupled with warm gas (∼103 K) around the protostar. The circumstellar disk is born in the "dead zone", a region that is de-coupled from the magnetic field, and the outer radius of the disk increases with that of the dead zone during the early accretion phase. The rapid increase of the disk size occurs after the depletion of the envelope of molecular cloud core. The effect of Hall current may create two distinct populations of protoplanetary disks.
AB - This review describes realistic evolution of magnetic field and rotation of the protostars, dynamics of outflows and jets, and the formation and evolution of protoplanetary disks. Recent advances in the protostellar collapse simulations cover a huge dynamic range from molecular cloud core density to stellar density in a self-consistent manner and account for all the non-ideal magnetohydrodynamical effects, such as Ohmic resistivity, ambipolar diffusion, and Hall current. We explain the emergence of the first core, i.e., the quasi-hydrostatic object that consists of molecular gas, and the second core, i.e., the protostar. Ohmic dissipation largely removes the magnetic flux from the center of a collapsing cloud core. A fast well-collimated bipolar jet along the rotation axis of the protostar is driven after the magnetic field is re-coupled with warm gas (∼103 K) around the protostar. The circumstellar disk is born in the "dead zone", a region that is de-coupled from the magnetic field, and the outer radius of the disk increases with that of the dead zone during the early accretion phase. The rapid increase of the disk size occurs after the depletion of the envelope of molecular cloud core. The effect of Hall current may create two distinct populations of protoplanetary disks.
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U2 - 10.1051/eas/1575045
DO - 10.1051/eas/1575045
M3 - Conference contribution
AN - SCOPUS:84973911476
T3 - EAS Publications Series
SP - 219
EP - 226
BT - Conditions and Impact of Star Formation 2015
A2 - Schaaf, R.
A2 - Stutzki, Jurgen
A2 - Simon, Robert
PB - EDP Sciences
Y2 - 7 September 2015 through 11 September 2015
ER -