Evolution of First Cores in Rotating Molecular Cores
Evolution of First Cores in Rotating Molecular Cores
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DOI:
10.1086/504028
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发表时间:
2006-07
期刊:
影响因子:
--
通讯作者:
K. Saigo;K. Tomisaka
中科院分区:
文献类型:
--
作者:
K. Saigo;K. Tomisaka
We investigate the effect of rotation on the star formation process quantitatively using axisymmetric numerical calculations. An adiabatic hydrostatic object (the so-called first core) forms in a contracting cloud core, after the central region becomes optically thick and continues to contract, driven by mass accretion onto it. The structure of a rotating first core is characterized by its total angular momentum Jcore and mass Mcore, both of which increase by accretion with time. We find that the first core evolves with a constant Jcore/M. Evolutionary paths of first cores can be classified into two types. In a slowly rotating core with Jcore/M 0.015G/(ciso) stops its contraction before the central density reaches the H2 dissociation density and does not begin the second collapse. These rapidly rotating first cores suffer from nonaxisymmetric instabilities, such as formation of massive spiral arms, deformation into a bar, or fragmentation. Although the rotating first cores have small average luminosities of Lcore = 0.003-0.03 L☉, assuming a constant mass accretion rate core. Their lifetimes last several thousand years or more, which is much longer than those expected for nonrotating clouds (~1000 yr). We expect that at least several percent of prestellar cores contain first cores as very low luminosity objects. Furthermore, we find a core with 0.012G/(ciso) < Jcore/M < 0.015G/(ciso) may form close binary systems with initial separation of 0.02-0.1 AU after the second collapse phase.