Investigating white-light flare mechanisms via the Paschen jump using high-resolution continuum observations from the Swedish 1-m Solar Telescope
利用瑞典1米太阳望远镜高分辨率连续谱观测通过帕邢跳变研究白光耀斑机制
Context. The continuum is understood to contain a large portion of the energy emitted by a solar flare. The optical continuum, known as white light (WL), is particularly relevant since it may be observed by ground-based instruments. Aims. We measured the WL enhancements short- and longward of the Paschen jump in order to gain insights into the possible mechanism(s) behind the creation of these increases in our two case studies. Methods. We took measurements from the Swedish 1-m Solar Telescope of the pseudo-continuum around the Ca II 8542 Å line as well as the true continuum around the KI7699 Å and the FeI6173 Å line, providing us with observations on both sides of the Paschen jump. Results. We observe WL enhancements of over 40% against the dark (pen-) umbral background in both flares. No WL excess is detectable against the granulation outside the sunspots. The WL excess in flare 1 is co-temporal with the derivative of the GOES soft X-ray and hard X-ray (HXR) measurements from the Advanced Space-based Solar Observatory (ASO-S), and the flare is compatible with the Neupert effect. For the second flare, a preceding smaller flare may be the cause of the temporal discrepancy. Signatures of chromospheric evaporation and condensation are found in the WL area for both flares. The ratio of intensities blueward and red-ward of the Paschen jump (i.e., the Paschen ratio) in flare 1 is below one for most WL pixels. This is in disagreement with the accepted WL formation mechanisms, which are both of photospheric and chromospheric origin. We believe this is a consequence of the Ca II 8542 Å pseudo-continuum being affected by line wing opacity changes. Conclusions. The co-temporality of WL and HXR enhancements suggests that the WL emission enhancements in flare 1 (and parts of flare 2) are a result of direct electron precipitation. We conclude that more reliable continuum measurements free of any nearby line influence are necessary in order to obtain conclusive evidence for the formation mechanism(s) behind optical continuum enhancements from such analysis as presented in this work.
展开 ▾用 SST/CRISP 同时覆盖帕邢跳变两侧的 K I 7699 Å、Fe I 6173 Å 真连续谱和 Ca II 8542 Å 伪连续谱,发现白光增强与 HXR 共时、符合 Neupert 效应;但帕邢比小于 1,揭示 Ca II 8542 Å 远翼不能作为连续谱代理。
过去白光耀斑机制常按光球 H⁻ 连续谱与色球氢复合辐射来区分,并以 Balmer/Paschen 跳变作为诊断依据(Neidig 1989;Ding+ 1994)。地面高分辨率观测开始系统测量耀斑连续谱(Kleint+ 2016),而 RADYN/F-CHROMA 耀斑模拟网格为解释帕邢比提供了模型参照(Carlsson+ 2023)。本文把这一思路用于 SST 跨帕邢跳变的两例 M 级耀斑,发现白光增强与硬 X 射线共时,但 Ca II 8542 Å 远翼伪连续谱受线翼不透明度污染,导致帕邢比低于 1。未来若要用帕邢跳变无歧义区分光球与色球起源,需要在严格无邻近谱线影响的窗口或采用光谱仪获取真连续谱观测。
预印本 2026-07-07 · 刊出 2026-08-11 · 收录 2026-08-20