论文标题

第一颗恒星形成的磁场。-II结果

Magnetic fields in the formation of the first stars.--II Results

论文作者

Stacy, Athena, McKee, Christopher F., Lee, Aaron T., Klein, Richard I., Li, Pak Shing

论文摘要

从Z = 100处的宇宙学初始条件开始,我们模拟磁场对人口III恒星形成的影响,并将我们的结果与纸张I的预测进行比较。我们使用Gadget-2在该场较弱时遵循系统的演变。我们引入了一种通过跟踪变形张量的演变来处理运动场的新方法。对于弥漫性天体等离子体,模拟的这一阶段的生长速率低于预期的,该等离子体具有非常低的电阻率(高磁性PRANDTL数);我们将其归因于模拟中的较大数值电阻率,对应于磁性的阶数统一数。当磁场在Z = 27处的Minihalo的核心中开始动态显着,我们将其映射到均匀的网格上,并遵循自适应网格细化中的演变,在Orion2中的MHD模拟。 Orion2模拟中该领域的非线性演变违反了通量冻结,并且与Xu&Lazarian提出的理论一致。该田地以密度〜10^10-10^12 cm^-3接近电气。当在没有磁场的Orion2中进行相同的计算时,几种原始的质体形成,质量为〜1至30 m_sol,带有磁场,仅在模拟结束时只有一个〜30 m_sol Protostar形成。因此,磁场抑制了低质量的流行III星的形成,产生了最重的POP III IMF,并导致没有观察到的POP III恒星。

Beginning with cosmological initial conditions at z=100, we simulate the effects of magnetic fields on the formation of Population III stars and compare our results with the predictions of Paper I. We use Gadget-2 to follow the evolution of the system while the field is weak. We introduce a new method for treating kinematic fields by tracking the evolution of the deformation tensor. The growth rate in this stage of the simulation is lower than expected for diffuse astrophysical plasmas, which have a very low resistivity (high magnetic Prandtl number); we attribute this to the large numerical resistivity in simulations, corresponding to a magnetic Prandtl number of order unity. When the magnetic field begins to be dynamically significant in the core of the minihalo at z=27, we map it onto a uniform grid and follow the evolution in an adaptive mesh refinement, MHD simulation in Orion2. The nonlinear evolution of the field in the Orion2 simulation violates flux-freezing and is consistent with the theory proposed by Xu & Lazarian. The fields approach equipartition with kinetic energy at densities ~ 10^10 - 10^12 cm^-3. When the same calculation is carried out in Orion2 with no magnetic fields, several protostars form, ranging in mass from ~ 1 to 30 M_sol with magnetic fields, only a single ~ 30 M_sol protostar forms by the end of the simulation. Magnetic fields thus suppress the formation of low-mass Pop III stars, yielding a top-heavy Pop III IMF and contributing to the absence of observed Pop III stars.

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