论文标题

使用遗传算法得出的小型耀斑的能量分布

Energy distribution of small-scale flares derived using genetic algorithm

论文作者

Kawai, Toshiki, Imada, Shinsuke

论文摘要

为了了解冠状加热的机制,至关重要的是,提出小规模耀斑,即所谓的纳米光的贡献,对太阳能电晕的加热。迄今为止,几项研究试图得出耀斑的发生频率分布,以揭示小规模耀斑的贡献。然而,没有研究通过以下条件来得出分布的研究:(1)冠状回旋血浆通过小尺寸耀斑加热的冠状等离子体的演变,(2)循环小于观察到的图像的空间分辨率,以及(3)多波长观察。为了考虑到这些条件,我们引入了一种新方法,以基于一维环路模拟和机器学习技术(即遗传算法)对小规模耀斑进行统计分析。首先,我们获得了六个sDO/AIA光曲线的通道。其次,我们进行了许多冠状环模拟,并在伪曼纳中获得每个模拟的SDO/AIA光曲线。第三,使用遗传算法,我们估算了重现观察结果的模拟光曲线的最佳组合。因此,观察到的冠状环被小尺寸耀斑加热,其能量通量大于通常间歇性地加热活性区域所需的冠状环。此外,我们得出了在1到3范围内具有各种幂律指数的发生频率分布,该指数部分支持纳米洛雷加热模型。相比之下,我们发现冠状加热的$ 90 \%$是由能量大于$ 10^{25}〜\ mathrm {erg} $的耀斑完成的。

To understand the mechanism of coronal heating, it is crucial to derive the contribution of small-scale flares, the so-called nanoflares, to the heating up of the solar corona. To date, several studies have tried to derive the occurrence frequency distribution of flares as a function of energy to reveal the contribution of small-scale flares. However, there are no studies that derive the distribution with considering the following conditions: (1) evolution of the coronal loop plasma heated by small-scale flares, (2) loops smaller than the spatial resolution of the observed image, and (3) multiwavelength observation. To take into account these conditions, we introduce a new method to analyze small-scale flares statistically based on a one-dimensional loop simulation and a machine learning technique, that is, genetic algorithm. First, we obtain six channels of SDO/AIA light curves of the active-region coronal loops. Second, we carry out many coronal loop simulations and obtain the SDO/AIA light curves for each simulation in a pseudo-manner. Third, using the genetic algorithm, we estimate the best combination of simulated light curves that reproduce the observation. Consequently, the observed coronal loops are heated by small-scale flares with energy flux larger than that typically required to heat up an active region intermittently. Moreover, we derive the occurrence frequency distribution which have various power-law indices in the range from 1 to 3, which partially supports the nanoflare heating model. In contrast, we find that $90\%$ of the coronal heating is done by flares that have energy larger than $10^{25}~\mathrm{erg}$.

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