论文标题
内半月边界III的独特磁特性。模拟黑子的分析
A distinct magnetic property of the inner penumbral boundary III. Analysis of simulated sunspots
论文作者
论文摘要
对黑子观测的分析揭示了覆盖边界的基本磁特性,即磁场的垂直成分的不变性。我们的目的是分析模拟黑子中Umbra-Penumbra边界的磁性,从而评估它们与观察到的黑子的相似性。此外,我们旨在研究等离子体$β$的作用以及动力在对流运动中模拟黑子中磁能的比率。我们使用Muram Code的一组非灰色仿真运行。这些数据用于合成然后将其降解为Hinode SpectropoloPolariMeter样观测值的Stokes曲线。然后,将数据视为黑子的真实HINODE观测值,并确定了翁布尔边界处的磁性。潜在场外推的模拟在其罩边界上产生逼真的磁场构型。两个具有潜在场上边界但不同地下磁场结构的模拟在其半身范围内有显着差异。通过在上边界处强迫更多的水平磁场来增加半部宽度,从而导致与观测不一致的磁性特性。这意味着半月的大小由磁场的地下结构给出。没有一个黑子模拟与同时观察到的磁场和方向的特性一致。强大的向外导向的Evershed流仅在顶部边界处具有人为增强的磁场的水平分量的设置中发现,这与向上边界处观察到的磁场特性不一致。我们想强调的是,模拟黑子的“光球”边界是由等值场值的磁场强度定义的。
The analyses of sunspot observations revealed a fundamental magnetic property of the umbral boundary, the invariance of the vertical component of the magnetic field. We aim to analyse the magnetic properties of the umbra-penumbra boundary in simulated sunspots and thus assess their similarity to observed sunspots. Also, we aim to investigate the role of plasma $β$ and the ratio of kinetic to magnetic energy in simulated sunspots on the convective motions. We use a set of non-grey simulation runs of sunspots with the MURaM code. These data are used to synthesise the Stokes profiles that are then degraded to the Hinode spectropolarimeter-like observations. Then, the data are treated like real Hinode observations of a sunspot and magnetic properties at the umbral boundaries are determined. Simulations with potential field extrapolation produce a realistic magnetic field configuration on their umbral boundaries. Two simulations with potential field upper boundary, but different subsurface magnetic field structures, differ significantly in the extent of their penumbrae. Increasing the penumbra width by forcing more horizontal magnetic fields at the upper boundary results in magnetic properties that are not consistent with observations. This implies that the size of the penumbra is given by the subsurface structure of the magnetic field. None of the sunspot simulations is consistent with observed properties of the magnetic field and direction of the Evershed flow at the same time. Strong outward directed Evershed flows are only found in setups with artificially enhanced horizontal component of the magnetic field at the top boundary that are not consistent with the observed magnetic field properties at the UP boundary. We want to stress out that the `photospheric' boundary of simulated sunspots is defined by a magnetic field strength of equipartition field value.