Effect of geomagnetic storms on VLF waves at low latitudes based on the analysis of whistlers and VLF emissions observed at Indian ground stations: A Review

K. K. Singh, A. P. Mishra
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Abstract

. A review of the effect of geomagnetic storms on very low frequency (VLF) waves (whistlers and emissions) at low latitudes is presented, based on the spectral analysis of the storm-time VLF data collected over a period of about four decades at our low latitude ground-based Indian stations. The review begins with an introduction about the characteristics of whistlers and VLF emissions and the importance of storm-time VLF events for the developments of our theoretical knowledge in plasma physics. This is followed by four different sections (2-5) in order to understand and explain the physics of VLF events observed at low latitudes during magnetic storms. All aspects of whistler duct and geomagnetic activity are described in section 2 whereas section 3 deals with VLF wave (whistlers and emissions) activity and whistler dispersion. Section 4 presents method of analysis of whistler duct alongwith duct lifetime and VLF emission source used in the spectral analysis of storm-time VLF data reported in the present paper. Section 5 describes in brief the experimental setup used in recording of VLF data at our Indian ground stations with a presentation of some selected storm-time whistlers and emissions alongwith their detailed spectral analysis of the observed salient features. Spectral analyses of the storm-time whistlers and emissions using VLF data from our Indian stations have provided the following results (section 6): mid/high latitude emissions generated in the equatorial region of higher 𝐿 -values through the process of Doppler-shifted cyclotron resonance mechanism and propagated along the higher field lines in different ducts formed by disturbances during magnetic storm and after exiting from the ducts, they penetrated the ionosphere and are trapped in Earth-ionosphere waveguide and after propagating in the waveguide are thus recorded at low latitude ground stations. (3) The increased intensity of whistler and emission activities during magnetic storm periods are due to the formation of additional ducts by the enhanced flux of energetic electrons during magnetic storm periods. along with their dispersion analysis. The dispersion analysis of the storm-time whistlers observed at mentioned Indian stations, shows, that unusual high dispersion whistlers are registered during magnetic storm periods and their dispersions ranges from about 15 - 250 s 1/2 . From the dispersion analysis of these observed storm-time high dispersion whistlers using Dowder-Allcock method (Dowden and Allcock, 1971) and curve-fitting technique of Tarcsai (Tarcsai, 1975), we find that these whistlers have propagated along the higher geomagnetic field lines in different ducts corresponding to 𝐿 -values of 2.88 to 6.52. Hence it may be inferred that storm-time whistlers recorded at low latitudes belong to mid/high latitudes and these whistlers may have propagated in different ducts along higher 𝐿 -values and after exiting from ducts, they penetrated the ionosphere and are trapped in Earth-ionosphere waveguide and thereafter propagating in the waveguide they are received at our low latitude Indian ground stations. The wave normal angle (lying in the range of 0.2 - 2.3 0 )at the entrance into the waveguide is such that they propagated towards the equator and are received at low latitude Indian ground stations (Singh et al., 2008, 2009, 2010, 2011).
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基于印度地面站哨声和VLF发射分析的地磁风暴对低纬度VLF波的影响:综述
。本文基于对印度低纬度地面站近40年来收集的风暴时间甚低频(VLF)数据的频谱分析,综述了地磁风暴对低纬度地区甚低频(VLF)波(哨声和辐射)的影响。本文首先介绍了口哨和甚低频辐射的特性,以及风暴时甚高频事件对等离子体物理理论知识发展的重要性。接下来是四个不同的部分(2-5),以便理解和解释磁暴期间在低纬度观测到的VLF事件的物理现象。第2节描述了哨声管道和地磁活动的所有方面,而第3节处理VLF波(哨声和发射)活动和哨声弥散。第4节介绍了在本文报道的风暴时间VLF数据的光谱分析中使用的口哨风管、风管寿命和VLF发射源的分析方法。第5节简要介绍了在我们的印度地面站记录VLF数据所使用的实验装置,并介绍了一些选定的风暴时间哨子和发射,以及对观测到的显著特征的详细光谱分析。利用我们印度站点的VLF数据对风暴时哨声和排放物进行光谱分析,得出以下结果(第6节):在高𝐿-值的赤道地区,通过多普勒偏移回旋共振机制产生的中高纬度辐射,在磁暴扰动形成的不同管道中沿较高场线传播,从管道中出来后,穿透电离层,被困在地球-电离层波导中,在波导中传播后,被低纬度地面站记录。(3)磁暴期间哨声和发射活动强度的增加是由于高能电子通量的增强在磁暴期间形成了额外的管道。以及他们的分散分析。对上述印度站点观测到的风暴时哨子的色散分析表明,在磁暴期间记录到不寻常的高色散哨子,其色散范围约为15 - 250 s /2。利用Dowder-Allcock方法(Dowden and Allcock, 1971)和Tarcsai曲线拟合技术对这些观测到的风暴时高色散哨子进行色散分析,我们发现这些哨子在𝐿-值为2.88 ~ 6.52的不同管道中沿较高的地磁场线传播。因此可以推断,低纬度记录的风暴时间哨声属于中高纬度地区,这些哨声可能沿着较高的𝐿值在不同的管道中传播,从管道中出来后,它们穿过电离层并被困在地球电离层波导中,然后在我们低纬度印度地面站接收到的波导中传播。在波导入口处的波法向角(位于0.2 - 2.3 0范围内)使得它们向赤道传播,并在低纬度的印度地面站接收(Singh等人,2008,2009,2010,2011)。
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