论文标题
从毫米波长下的极化程度中推断出太阳耀斑的磁场不对称性
Inferring the magnetic field asymmetry of solar flares from the degree of polarisation at millimetre wavelengths
论文作者
论文摘要
毫米波的太阳耀斑的极化测量用于研究发射源的磁场构型。我们分析了两种太阳耀斑(Sol2013-02-17和Sol2013-11-05),通过在45和90 GHz处的毫米度(诗歌)在1-15 GHz的太阳(诗歌)在1-15 GHz处观察到的毫米度(poemas)的极化发射,并由无线电望远镜网络(RSTN)以及高频(RSTN)和高频(212GHAR)(212GHAR)(212 GHAR)(S Soler)(S Soler)(S Soler)(S SOLER)。同样,这些耀斑的硬X射线是由Reuvis Ramaty高能太阳能光谱成像仪(Rhessi)同时检测到的。使用模型在空间变化的3D磁场回路结构中模拟陀螺仪发射的模型拟合了通量和极化无线电光谱。对于{建模},固定磁回路几何形状,场强是磁场的唯一自由参数。此外,模型的均匀电子分布{假定},其能量电子的数量密度和电子光谱指数作为游离参数。拟合的模型对每个事件的偏振和无线电光谱的观察程度很好地复制了,从而产生了回路和耀斑源的物理参数。我们的结果表明,在太阳耀斑期间的高度极化可以通过位于高度不对称磁路的{footpoints}的两个来源来解释,而低极化度来自对称磁路的脚步来源。
Polarisation measurements of solar flares at millimetre-waves were used to investigate the magnetic field configuration of the emitting sources. We analyse two solar flares (SOL2013-02-17 and SOL2013-11-05) observed by the POlarisation Emission of Millimetre Activity at the Sun (POEMAS) at 45 and 90 GHz, at microwaves from 1 - 15 GHz by the Radio Solar Telescope Network (RSTN), and at high frequencies (212 GHz) by the Solar Submillimetre Telescope (SST). Also, hard X-rays from these flares were simultaneously detected by the Reuven Ramaty High-Energy Solar Spectroscopic Imager (RHESSI). The flux and polarisation radio spectra were fit using a model that simulates gyrosynchrotron emission in a spatially-varying 3D magnetic field loop structure. For the {modelling}, the magnetic loop geometry was fixed and the field strength was the only free parameter of the magnetic field. In addition, a uniform electron distribution was {assumed by} the model, with the number density of energetic electrons and the electron spectral index as free parameters. The fitted model reproduced reasonably well the observed degree of polarisation and radio flux spectra for each event yielding the physical parameters of the loop and flaring sources. Our results indicate that the high degree of polarisation during a solar flare can be explained by two sources located at the {footpoints} of highly asymmetric magnetic loops whereas low polarisation degrees arise from footpoint sources of symmetric magnetic loops.