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RELATION BETWEEN THE CORONAL MASS EJECTION ACCELERATION AND THE NON-THERMAL FLARE CHARACTERISTICS

机译:冠状动脉抛射加速度与非热耀斑特征的关系

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We investigate the relationship between the main acceleration phase of coronal mass ejections (CMEs) and the particle acceleration in the associated flares as evidenced in Reuven Ramaty High Energy Solar Spectroscopic Imager non-thermal X-rays for a set of 37 impulsive flare-CME events. Both the CME peak velocity and peak acceleration yield distinct correlations with various parameters characterizing the flare-accelerated electron spectra. The highest correlation coefficient is obtained for the relation of the CME peak velocity and the total energy in accelerated electrons (c = 0.85), supporting the idea that the acceleration of the CME and the particle acceleration in the associated flare draw their energy from a common source, probably magnetic reconnection in the current sheet behind the erupting structure. In general, the CME peak velocity shows somewhat higher correlations with the non-thermal flare parameters than the CME peak acceleration, except for the spectral index of the accelerated electron spectrum, which yields a higher correlation with the CME peak acceleration (c ≈ –0.6), indicating that the hardness of the flare-accelerated electron spectrum is tightly coupled to the impulsive acceleration process of the rising CME structure. We also obtained high correlations between the CME initiation height h 0 and the non-thermal flare parameters, with the highest correlation of h 0 to the spectral index δ of flare-accelerated electrons (c ≈ 0.8). This means that CMEs erupting at low coronal heights, i.e., in regions of stronger magnetic fields, are accompanied by flares that are more efficient at accelerating electrons to high energies. In the majority of events (~80%), the non-thermal flare emission starts after the CME acceleration, on average delayed by ≈6 minutes, in line with the standard flare model where the rising flux rope stretches the field lines underneath until magnetic reconnection sets in. We find that the current sheet length at the onset of magnetic reconnection is 21 ± 7?Mm. The flare hard X-ray peaks are well synchronized with the peak of the CME acceleration profile, and in 75% of the cases they occur within ±5?minutes. Our findings provide strong evidence for the tight coupling between the CME dynamics and the particle acceleration in the associated flare in impulsive events, with the total energy in accelerated electrons being closely correlated with the peak velocity (and thus the kinetic energy) of the CME, whereas the number of electrons accelerated to high energies is decisively related to the CME peak acceleration and the height of the pre-eruptive structure.
机译:我们研究了冠状物质抛射(CME)的主要加速阶段与相关耀斑中的粒子加速度之间的关系,如鲁汶拉玛特高能太阳光谱成像仪非热X射线对37个脉冲耀斑CME事件的集合所证明的。 CME峰速度和峰加速度都与表征耀斑加速电子光谱的各种参数产生明显的相关性。对于CME峰值速度和加速电子中的总能量之间的关系,获得了最高的相关系数(c = 0.85),这支持了CME的加速度和相关耀斑中的粒子加速度从共同点吸收能量的想法。源,可能是喷发结构后面的电流表中的磁重新连接。通常,CME峰值速度与非热耀斑参数的相关性比CME峰值加速度高,但加速电子光谱的光谱指数除外,它与CME峰值加速度具有更高的相关性(c≈–0.6 ),表明耀斑加速电子光谱的硬度与上升的CME结构的脉冲加速过程紧密相关。我们还获得了CME起始高度h 0和非热耀斑参数之间的高度相关性,其中h 0与耀斑加速电子的光谱指数δ的相关性最高(c≈0.8)。这意味着在低日冕高度即在较强磁场区域爆发的CME伴随着耀斑,这些耀斑更有效地将电子加速为高能。在大多数事件中(约80%),非热耀斑的排放在CME加速后开始,平均延迟≈6分钟,这与标准的耀斑模型一致,在该模型中,上升的通量绳将下方的磁力线伸展到磁重新连接开始。我们发现,磁性重新连接开始时的当前薄板长度为21±7?Mm。耀斑的硬X射线峰与CME加速度曲线的峰很好地同步,在75%的情况下,它们在±5分钟内发生。我们的发现为脉冲事件中CME动力学和相关耀斑中的粒子加速度之间的紧密耦合提供了有力的证据,加速电子中的总能量与CME的峰值速度(以及动能)密切相关,而加速到高能的电子数量与CME峰值加速度和喷发前结构的高度密切相关。

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