2018
DOI: 10.4236/ojer.2018.73010
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On the Tempo-Spatial Evolution of the Lower Ionospheric Perturbation for the 2016 Kumamoto Earthquakes from Comparisons of VLF Propagation Data Observed at Multiple Stations with Wave-Hop Theoretical Computations

Abstract: There have been published many papers on VLF (very low frequency) characteristics to study seismo-ionospheric perturbations. Usually VLF records (amplitude and/or phase) are used to investigate mainly the temporal evolution of VLF propagation anomalies with special attention to one particular propagation path. The most important advantage of this paper is the simultaneous use of several propagation paths. A succession of earthquakes (EQs) happened in the Kumamoto area in Kyusyu Island; two strong foreshocks wi… Show more

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Cited by 16 publications
(40 citation statements)
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“…In this paper, we have compared the stratospheric oscillations with the corresponding lower ionospheric perturbation for the 2016 Kumamoto EQs (Asano & Hayakawa, ). First of all, the temporal evolution indicates that the stratospheric gravity wave activity over the EQ epicenter is clearly seen on the days from 8 April to 14 April, which is found to be in complete consistence with the lower ionospheric perturbation as detected by the VLF network.…”
Section: Discussionmentioning
confidence: 99%
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“…In this paper, we have compared the stratospheric oscillations with the corresponding lower ionospheric perturbation for the 2016 Kumamoto EQs (Asano & Hayakawa, ). First of all, the temporal evolution indicates that the stratospheric gravity wave activity over the EQ epicenter is clearly seen on the days from 8 April to 14 April, which is found to be in complete consistence with the lower ionospheric perturbation as detected by the VLF network.…”
Section: Discussionmentioning
confidence: 99%
“…In their paper, they have assumed that the shape of the ionospheric perturbation is quasi-circular, even though nobody knows its exact shape. Another important conclusion of Asano and Hayakawa (2018) is that the radius of perturbation is about 100 km on 2 April and it expands to 550 km on 10 April. The expansion speed is about 50-60 km/day during the development, and we can expect that even above Tokyo the ionosphere is…”
Section: Ionospheric Perturbationmentioning
confidence: 99%
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“…Asano and Hayakawa (2017) [34] have made further detailed analysis on the basis of VLF data observed at all 8 stations in Japan on the assumption that the ionospheric perturbation appears first above the EQ epicenter and it is assumed to develop temporally and spatially (horizontally and vertically), we compute the temporal evolutions of amplitude changes at all stations by changing independently the reflection height of one-hop sky wave and that of the second-hop wave close to the transmitter side of the relevant path, and we compare those theoretical values based on the wave-hop method with the observational results in order to infer extensively the spatio-temporal evolution of the ionospheric perturbation. Details on the results will be published elsewhere, but we indicate the following conclusion that the ionospheric perturbations appears about two weeks before the EQ, then it seems to develop by expanding horizontally and vertically (its reflection height becomes lower), and the most perturbed perturbation happens on 10 -12 April (in UT), followed by a decay.…”
Section: ) Vlf Monitoringmentioning
confidence: 99%
“…Asano and Hayakawa (2017) [28] have tried to compare the observational VLF amplitude with the wave-hop theoretical amplitude estimation by changing the reflection heights of 1 hop and 2 hop sky waves for the relevant propagation path, in order to investigate the detailed spatio-temporal evolution of the properties of ionospheric perturbation for the recent 2016 Kumamoto EQ. By using the similar wave-hop computations (details will be published elsewhere), Figure 6 illustrates the area of perturbation (with the VLF reflection height being lowered Figure 6.…”
Section: Discussionmentioning
confidence: 99%