On the decay of strong magnetization in global disc simulations with toroidal fields

On the decay of strong magnetization in global disc simulations with toroidal fields
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关于环形场全局圆盘模拟中强磁化强度的衰减

DOI:
10.1093/mnras/stx274
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发表时间:
2017
影响因子:
4.8
通讯作者:
Sądowski, Aleksander
Sądowski, Aleksander
中科院分区:
物理与天体物理2区
文献类型:
--
作者:
Fragile, P. Chris;Sądowski, Aleksander

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吸积盘中的强磁化可以解决许多与低质量 X 射线双星稳定性和状态转换相关的突出问题。然而,目前还不清楚真正的圆盘是如何被强磁化的,即使它们被强磁化,它们是否能保持这种状态。在本文中,我们通过一对全局盘模拟来解决后一个问题。在这里,我们只考虑最初完全包含在紧凑环内的纯环形磁场的情况。我们发现,仅在几十个轨道周期内,最初强磁化盘的磁化强度 Pmag/Pgas≥ 10 就下降到 ≲ 0.1,类似于最初弱磁化盘达到的稳态值。这与最近使用最初的强环形磁场进行的剪切箱模拟是一致的,强有力的结论是强磁化环形磁场不能局部自维持。这些结果似乎将净极向通量或扩展径向场作为建立强磁化盘的唯一途径,从而排除了热塌陷的情况。
Strong magnetization in accretion discs could resolve a number of outstanding issues related to stability and state transitions in low-mass X-ray binaries. However, it is unclear how real discs become strongly magnetized and, even if they do, whether they can remain in such a state. In this paper, we address the latter issue through a pair of global disc simulations. Here, we only consider cases of initially purely toroidal magnetic fields contained entirely within a compact torus. We find that over only a few tens of orbital periods, the magnetization of an initially strongly magnetized disc,Pmag/Pgas≥ 10, drops to ≲ 0.1, similar to the steady-state value reached in initially weakly magnetized discs. This is consistent with recent shearing box simulations with initially strong toroidal fields, the robust conclusion being that strongly magnetized toroidal fields cannot be locally self-sustaining. These results appear to leave net poloidal flux or extended radial fields as the only avenues for establishing strongly magnetized discs, ruling out the thermal collapse scenario.
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期刊: Publications of the Astronomical Society of Japan 58・1
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