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North-South Asymmetry of the Interplanetary Magnetic Field Magnitude and the Geomagnetic Indices

机译:行星际磁场强度和地磁指标的南北不对称

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Data of the daily interplanetary magnetic field (IMF), and the geomagnetic indices (aa, Ap, Kp, and DST) have been used to examine the asymmetry between the solar field north and south of the heliospheric current sheet, over the period (1975-2013). It important to note that during the positive polarity epochs: (T) refers to Toward the South of the heliospheric current sheet (Southern Hemisphere), and (A) refers to Away from North of the heliospheric current sheet (Northern Hemisphere). While, during the negative polarity epochs the opposite will be happened. The present study finds no clear indication of the presence of north-south asymmetry in the field magnitude, and also there is no magnetic solar cycle dependence that is evident. During the considered period, the north-south asymmetry for the considered parameters reaches maximum values around the declining phase or near to the minimum of the solar cycle. The geomagnetic indices have a clear asymmetry during the positive solar magnetic polarity period (qA > 0) and have a northern dominance during cycles (22 & 23) and southern dominance during cycles (21 & 24). From the power spectrum density, the considered parameters showed significant peaks which appeared in the north-south asymmetry but the 10.7 yr solar cycle was absent. In addition, the main periodicity of the asymmetry may be 5.2, 4.0 and 3.3 years that exist in the parameters with higher confidence levels. Finally, one can conclude that the asymmetry of the interplanetary parameters and the geomagnetic indices may provide multiple causes for producing the observed asymmetric modulations of cosmic rays.
机译:日间行星际磁场(IMF)和地磁指数(aa,Ap,Kp和DST)的数据已用于检验该时期(1975年)太阳圈电流片南北两极之间的不对称性-2013)。重要的是要注意,在正极性时期中,(T)表示向日球电流表的南侧(南半球),而(A)表示远离日球电流表的北侧(北半球)。而在负极性时期,将会发生相反的情况。本研究没有清楚地表明磁场强度存在南北不对称,也没有明显的磁太阳周期依赖性。在所考虑的时期内,所考虑参数的南北不对称在下降相位附近或接近太阳周期的最小值时达到最大值。在正太阳磁极性期间(qA> 0),地磁指数具有明显的不对称性,在周期(22和23)期间具有北部优势,在周期(21和24)期间具有南部优势。从功率谱密度来看,所考虑的参数显示出明显的峰值,该峰值出现在南北不对称处,但是没有10.7年的太阳周期。此外,不对称性的主要周期性可能是存在于置信度较高的参数中的5.2年,4.0年和3.3年。最后,可以得出结论,行星际参数和地磁指数的不对称性可能为产生观测到的宇宙射线的不对称调制提供多种原因。

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