论文标题

安静的磁磁和表面重力振荡模式的太阳能周期变化

Solar-Cycle Variation of quiet-Sun Magnetism and Surface Gravity Oscillation Mode

论文作者

Korpi-Lagg, Maarit J., Korpi-Lagg, Andreas, Olspert, Nigul, Truong, Hong-Linh

论文摘要

安静的太阳磁性的起源正在争论中。从观察上研究太阳周期变化可以详细观察可以为我们提供有关如何解决争议的线索。我们研究了最安静的区域的太阳周期变化及其表面重力振荡($ f $ - )模式集成能量($ e_f $)。我们使用12年的HMI数据,并根据空间和时间安静应用严格的选择标准,以避免活跃区域(ARS)的任何影响。我们开发了一个自动化的高通量管道,以浏览所有可用的磁性图数据,并为所选安静区域计算$ e_f $。我们观察到磁场强度在包含多个超晶体细胞的最安静区域的明显太阳周期依赖性。对于小于超晶体细胞小的斑块大小,未检测到明显的循环依赖性。随着时间的推移,超级尺度上的$ e_f $并不是恒定的。在周期24周期的后期阶段(SC24,2011-2012)中,它大致恒定,但随着SC24的最大值接近,2013年开始减少。这种趋势一直持续到2017年中期,当时看到了在南部纬度较高的较高的迹象。缓慢的加强持续,在纬度地区比赤道区域更强大,但是$ e_f $永远不会返回到2011 - 2012年所看到的价值。而且,加强趋势持续到太阳能最低限度,直到SC25显然已经上升的几年。因此,$ e_f $行为与太阳周期不相同。预计$ e_f $与太阳周期的$ e_f $的反相关性预计是预计的,但是几年的相位移位表明与poloidal大规模磁场成分而不是环形磁带的相关。用QS $ e_f $校准AR信号并未显示出AR出现之前的$ f $ mode的显着增强。

The origin of the quiet Sun magnetism is under debate. Investigating the solar cycle variation observationally in more detail can give us clues about how to resolve the controversies. We investigate the solar cycle variation of the most magnetically quiet regions and their surface gravity oscillation ($f$-) mode integrated energy ($E_f$). We use 12 years of HMI data and apply a stringent selection criteria, based on spatial and temporal quietness, to avoid any influence of active regions (ARs). We develop an automated high-throughput pipeline to go through all available magnetogram data and to compute $E_f$ for the selected quiet regions. We observe a clear solar cycle dependence of the magnetic field strength in the most quiet regions containing several supergranular cells. For patch sizes smaller than a supergranular cell, no significant cycle dependence is detected. The $E_f$ at the supergranular scale is not constant over time. During the late ascending phase of Cycle 24 (SC24, 2011-2012), it is roughly constant, but starts diminishing in 2013, as the maximum of SC24 is approached. This trend continues until mid-2017, when hints of strengthening at higher southern latitudes are seen. Slow strengthening continues, stronger at higher latitudes than at the equatorial regions, but $E_f$ never returns back to the values seen in 2011-2012. Also, the strengthening trend continues past the solar minimum, to the years when SC25 is already clearly ascending. Hence the $E_f$ behavior is not in phase with the solar cycle. The anticorrelation of $E_f$ with the solar cycle in gross terms is expected, but the phase shift of several years indicates a connection to the poloidal large-scale magnetic field component rather than the toroidal one. Calibrating AR signals with the QS $E_f$ does not reveal significant enhancement of the $f$-mode prior to AR emergence.

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