论文标题
反埃面流的磁拓扑
The magnetic topology of the inverse Evershed flow
论文作者
论文摘要
逆冲流(IEF)是向色球高度下黑子的质量运动。我们结合了来自Dunn太阳能望远镜的NOAA 12418的高分辨率观测值,并从Helioseis震(Helioseissic and Maginate Imager)(HMI)(HMI)组合了矢量磁场测量值,以确定IEF的驱动器。我们从H $α$和Ca II IR的光谱中得出了色球线(LOS)速度。 HMI数据用于非无磁场外推以跟踪活动区域的黑子附近的闭合场线。我们确定了它们的长度和高度,位于其内部和外部脚点,以及沿它们的衍生流速度。与IEF相关的磁场线平均在13毫米的长度上达到3毫米的高度。内部(外部)脚点位于1.2(1.9)黑子半径。内部和外部足点之间的平均场强差$ΔB$为+400 g。温度差$ΔT$与$ΔB$抗相关,平均值为-100 k。压力差$ΔP$以$ΔB$为主,主要是$ΔB$的,主要是正面的,其驱动力是平均1.7 kpa的内部脚步。从$ΔP$中预测的速度将具有2-10 km s $^{ - 1} $的LOS速度,并具有方形依赖性。我们发现,IEF是沿磁场线驱动的,该磁场线通过气压差将网络元件与外部半月连接起来,这是由于经典的虹吸流动场景所预测的田间强度差而导致的。
The inverse Evershed flow (IEF) is a mass motion towards sunspots at chromospheric heights. We combined high-resolution observations of NOAA 12418 from the Dunn Solar Telescope and vector magnetic field measurements from the Helioseismic and Magnetic Imager (HMI) to determine the driver of the IEF. We derived chromospheric line-of-sight (LOS) velocities from spectra of H$α$ and Ca II IR. The HMI data were used in a non-force-free magnetic field extrapolation to track closed field lines near the sunspot in the active region. We determined their length and height, located their inner and outer foot points, and derived flow velocities along them. The magnetic field lines related to the IEF reach on average a height of 3 Mm over a length of 13 Mm. The inner (outer) foot points are located at 1.2 (1.9) sunspot radii. The average field strength difference $ΔB$ between inner and outer foot points is +400 G. The temperature difference $ΔT$ is anti-correlated with $ΔB$ with an average value of -100 K. The pressure difference $Δp$ is dominated by $ΔB$ and is primarily positive with a driving force towards the inner foot points of 1.7 kPa on average. The velocities predicted from $Δp$ reproduce the LOS velocities of 2-10 km s$^{-1}$ with a square-root dependence. We find that the IEF is driven along magnetic field lines connecting network elements with the outer penumbra by a gas pressure difference that results from a difference in field strength as predicted by the classical siphon flow scenario.