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Spatially resolved observations of a split-band coronal type-II radio burst

机译:分裂带冠状II型无线电的空间分辨观测   爆

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摘要

Context. The origin of coronal type-II radio bursts and of theirband-splitting are still not fully understood. Aims. To make progress insolving this problem on the basis of one extremely well observed solar eruptiveevent. Methods. The relative dynamics of multi-thermal eruptive plasmas,observed in detail by the SDO/AIA and of the harmonic type-II burst sources,observed by the NRH at ten frequencies from 445 to 151 MHz, is studied for thepartially behind the limb event on 3 November 2010. Special attention is givento the band-splitting of the burst. Analysis is supplemented by investigationof coronal hard X-ray (HXR) sources observed by the RHESSI. Results. It isfound that the flare impulsive phase was accompanied by the formation of adouble coronal HXR source, whose upper part coincided with the hot (T~10 MK)eruptive plasma blob. The leading edge (LE) of the eruptive plasmas (T~1-2 MK)moved upward from the flare region with the speed of v=900-1400 km/s. The typeII burst source initially appeared just above the LE apex and moved with thesame speed and in the same direction. After about 20 s it started to move abouttwice faster, but still in the same direction. At any given moment the lowfrequency component (LFC) source of the splitted type-II burst was situatedabove the high frequency component (HFC) source, which in turn was situatedabove the LE. It is also found that at a given frequency the HFC source waslocated slightly closer to the photosphere than the LFC source. Conclusions.The shock wave, which could be responsible for the observed type-II radioburst, was initially driven by the multi-temperature eruptive plasmas, butlater transformed to a freely propagating blast shock wave. The most preferableinterpretation of the type-II burst splitting is that its LFC was emitted fromthe upstream region of the shock, whereas the HFC - from the downstream region.
机译:上下文。冠状II型无线电爆发的起源及其频带分裂仍未完全了解。目的为了在解决这一问题的基础上取得进展,需要进行一次非常出色的太阳爆发事件。方法。研究了SDO / AIA和NII在445至151 MHz的十个频率上详细观测到的多热喷发等离子体的相对动力学,以及NRH在445至151 MHz的十个频率下观测到的II型谐波猝发源的相对动力学。 2010年11月3日。特别注意突发的频带分裂。通过对RHESSI观测到的冠状硬X射线(HXR)来源进行调查来补充分析。结果。发现火炬脉冲相伴随着双冠状HXR源的形成,其上部与热的(T〜10 MK)爆发的血浆团相吻合。爆发等离子体(T〜1-2 MK)的前缘(LE)从耀斑区域向上移动,速度为v = 900-1400 km / s。 II型爆发源最初出现在LE顶点上方,并以相同的速度和相同的方向移动。大约20秒钟后,它开始以大约两倍的速度移动,但方向仍然相同。在任何给定时刻,分裂的II型突发的低频分量(LFC)源都位于高频分量(HFC)源上方,而高频分量(HFC)源又位于LE上方。还发现在给定的频率下,HFC源的位置比LFC源的位置稍微靠近光球。结论:可能引起所观察到的II型放射性爆炸的冲击波最初是由多温度喷发等离子体驱动的,但后来转变为自由传播​​的爆炸冲击波。对II型爆发分裂的最优选解释是,其LFC是从激波的上游区域发出的,而HFC是从激流的下游区域发出的。

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