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arXiv 1306.5871astro-ph.SR
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具有吸积盘和自转的恒星形成I。太阳金属量在2至22 Msol之间的恒星

Star formation with disc accretion and rotation I. Stars between 2 and 22 Msol at solar metallicity

L. Haemmerlé, P. Eggenberger, G. Meynet, A. Maeder, C. Charbonnel

摘要:

恒星在形成过程中角动量的积累方式可能会影响它们的进一步演化。在冷盘吸积方案的框架中,我们第一次研究了角动量在恒星形成过程中如何在恒星内部积累,以及它在主序列(MS)上的演化后果。计算开始于Hayashi线上的0.7 Msol太阳金属丰度(Z=0.014)的流体静力核心作为一个固体旋转。吸积速率取决于吸积物体的光度,被认为在1.5e-5和1.7e-3 Msol/yr之间变化。假设吸积物质的角速度等于吸积恒星外层的角速度。模型计算的质量范围在零年龄的主要序列(ZAMS)之间的2和22 Msol。我们研究了如何内部和表面速度变化作为一个函数的时间在吸积阶段和朝着ZAMS的演变。恒星模型,其演变已遵循沿前MS阶段,被发现表现出浅梯度的角速度的ZAMS。有趣的是,对于ZAMS上的质量大于8 Msol,存在一个最大的表面速度,可以达到通过目前的情况下形成。通常,对于14 Msol的模型,只有表面速度低于临界速度45%的恒星才能形成。为了达到更高的速度,需要从核心旋转超过临界极限开始。我们发现,这个速度上限是较小的更高的质量。相比之下,低于8 Msol,没有限制,整个速度域,直到临界速度,可以达到。

英文摘要:

The way angular momentum is built up in stars during their formation process may have an impact on their further evolution. In the frame of the cold disc accretion scenario, we study for the first time how angular momentum builds up inside the star during its formation and what are the consequences for its evolution on the main sequence (MS). Computation begins from a hydrostatic core on the Hayashi line of 0.7 Msol at solar metallicity (Z=0.014) rotating as a solid body. Accretion rates depending on the luminosity of the accreting object are considered varying between 1.5e-5 and 1.7e-3 Msol/yr. The accreted matter is assumed to have an angular velocity equal to that of the outer layer of the accreting star. Models are computed for a mass-range on the zero-age main sequence (ZAMS) between 2 and 22 Msol. We study how the internal and surface velocities vary as a function of time during the accretion phase and the evolution towards the ZAMS. Stellar models, whose evolution has been followed along the pre-MS phase, are found to exhibit a shallow gradient of angular velocity on the ZAMS. Interestingly, for masses on the ZAMS larger than 8 Msol, there exists a maximum surface velocity that can be reached through the present scenario of formation. Typically, for 14 Msol models, only stars with surface velocities on the ZAMS lower than about 45% of the critical velocity can be formed. To reach higher velocities would require to start from cores rotating above the critical limit. We find that this upper velocity limit is smaller for higher masses. In contrast, below 8 Msol, there is no restriction and the whole domain of velocities, up to the critical one, can be reached.

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