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Features of cosmic ray neutron monitor intensity in relation to CMEs and IMF

机译:宇宙射线中子监测强度与CME和IMF的关系

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It is well known that Coronal Mass Ejections are vast structures of plasma and magnetic fields that are e ex- xpelled from the sun pelled into the heliosphere, which is detected by remote sensing and in in-situ spacecraft observations. R Re- ecent work indicates that the open magnetic flux from coronal holes may be a more important driver of cosmic cent cosmic-ray modulation than coronal mass ejections (CMEs), which originate from closed closed-field regions on the Sun. Influence of four types of CMEs namely Asymmetric 'Full' Halo CMEs, Partial Halo CMEs, Asymmetric and Complex 'Full' Halo CMEs and 'Full' Halo CMEs on cosmic ray neutron monitor intensity have been inv investigated in this study. The data estigated of two different ground based neutron monitors and CME events observed with instruments onboard and Wind spacecraft have been used in the present analysis. The method of superposed epoch (Chree) analysis has been used to the arrival times of these CMEs. The occurrence frequency of three different types of CMEs used in the present ana he anal- lysis shows complex behavior. However, significant increase in cosmic ray intensity is observed few days after the ysis onset of asymmetric full hal halo and few days after the onset of full halo CMEs. The fluctuations in cosmic ray i o intensity tensity are more prior to the onset of both types of the CMEs. However, during Partial Halo CMEs the cosmic ray i intensity tensity peaks, 8 8- 9 days prior to the onset of CMEs and dep depressed 3 days prior to the onset of CMEs, whereas in case of ressed asymmetric and complex full CMEs, the intensity depressed 2 days prior to the onset of CMEs and enhanced 2 days after the onset of CMEs. The deviations in cosmic ray intensity are more pronounced in case for asymmetric and complex full halo CMEs compared to other CMEs. The cosmic ray intensity shows nearly good anti anti-correlation with interplanetary magnetic field strength (B) during asymmetric full halo CMEs and partial halo CMEs, whereas it shows poor correlation with B during other CMEs. The interplanetary magnetic field strength B shows significant characteristics before and after the onset of these three types of CMEs.
机译:众所周知,日冕物质抛射是等离子体和磁场的巨大结构,它们是从被太阳辐射到日光层中而被驱除的,这可以通过遥感和在原位航天器的观测中检测到。最近的研究表明,与日冕质量抛射(CME)相比,日冕孔的开放磁通量可能是更重要的推动宇宙分宇宙射线调制的因素,而日冕物质抛射(CME)源自太阳的封闭近场区域。本研究研究了四种类型的CME,即不对称的“全”光晕CME,部分光晕的CME,不对称和复杂的“全”光晕CME和“全”光晕CME对宇宙射线中子监测强度的影响。在本分析中,使用了两个不同的地面中子监测器和用机载仪器和“风”飞船观测到的CME事件的数据估计。叠加历元(Chree)分析方法已用于这些CME的到达时间。本分析中使用的三种不同类型的CME的发生频率显示出复杂的行为。但是,在不对称全晕光晕发作后几天和全晕光CME发作几天后,观察到宇宙射线强度显着增加。宇宙射线强度强度的波动是在两种类型的CME出现之前发生的。但是,在偏晕CME期间,宇宙射线i强度强度峰值出现在CME发生之前的8-8-9天,而Dep则在CME发生发生的3天之前被压低,而在隐伏不对称和复杂的完整CME发生时,强度CME发生前2天抑郁,CME发生后2天增强。与其他CME相比,在不对称和复杂的完整光晕CME情况下,宇宙射线强度的偏差更为明显。在不对称的完整光晕CME和部分光晕CME中,宇宙射线强度显示出与行星际磁场强度(B)几乎良好的抗相关性,而在其他CME中,与B的相关性却很差。在这三种类型的CME发生之前和之后,行星际磁场强度B表现出显着的特征。

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