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The locations of transmitters and the Yushu earthquake. The blue squares represent the locations of the three transmitters (KRA, NOV, and KHA) in Russia. The epicenter of Yushu earthquake is denoted by the black star. The black square covers the region of the epicenter ±10 • , in which the data have been studied.

The locations of transmitters and the Yushu earthquake. The blue squares represent the locations of the three transmitters (KRA, NOV, and KHA) in Russia. The epicenter of Yushu earthquake is denoted by the black star. The black square covers the region of the epicenter ±10 • , in which the data have been studied.

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Earthquakes may disturb the lower ionosphere through various coupling mechanisms during the seismogenic and coseismic periods. The VLF (very low-frequency) signal radiated from ground-based transmitters will be affected when it penetrates the disturbed ionosphere above the epicenter area, and this anomaly can be recorded by low-Earth orbit satellit...

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... (1979) the preparation zone of the earthquake can reach ρ = 10 0.43M , where M is the magnitude of the earthquake and ρ is measured in kilometers. Considering the limited extension of the Ms 7.1 Yushu earthquake, the preparation zone ρ can reach to 1130 km; we mainly focused on the region within the region of the epicenter ±10 • (black square in Fig. 1). In this study, the nighttime PSD data of the electric field from the DEME-TER's survey mode observations were extracted study the perturbations of the VLF signal before and after the Yushu earthquake. As the VLF radio signals at daytime are too small to cause obvious SNR variation compared with those at nighttime, we did not use the ...
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... minimize the impact of other factors and confirm whether the SNR anomaly is caused by the earthquake and not the variation of the ionospheric background, we focus on SNR in the black square (shown in Fig. 1) of the same period in 2007-2009 as the background, when there are no large earthquakes and the data when the transmitter was turned off or affected by geomagnetic storms are eliminated. The mean value of all the data in each period has been obtained to get the time sequence shown in Fig. 3. In Fig. 3, the black dashed line represents ...
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... simulated results of the electric field at 120 km height with a different electron density along the magnetic meridian plane within 1000 km area around the transmitter NOV with 11.9 kHz transmitting frequency are shown in Fig. 10. The simulated results are similar when the transmitting frequency is 12.6 and 14.9 kHz. It can be seen that the wave mode interference in the waveguide has been mapped into the ionosphere in the electric field (Lehtinen and Inan, 2009), and the electric field increases when the electron density decreases, and vice versa (Fig. 10a, c). ...
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... are shown in Fig. 10. The simulated results are similar when the transmitting frequency is 12.6 and 14.9 kHz. It can be seen that the wave mode interference in the waveguide has been mapped into the ionosphere in the electric field (Lehtinen and Inan, 2009), and the electric field increases when the electron density decreases, and vice versa (Fig. 10a, c). Furthermore, the maximum value of the electric field varying with height is collected to study the influence of the electron disturbance. At nighttime, when i the variation of electron density is smaller, the variation of the electric field is also smaller (Fig. 10b, d). When the electron density increases by 4 times, the maximum ...
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... electric field increases when the electron density decreases, and vice versa (Fig. 10a, c). Furthermore, the maximum value of the electric field varying with height is collected to study the influence of the electron disturbance. At nighttime, when i the variation of electron density is smaller, the variation of the electric field is also smaller (Fig. 10b, d). When the electron density increases by 4 times, the maximum electric field decreases about 2 dB at 120 km (see Fig. 10d). The variation is also 2 dB at DEMETER's altitude (660 km) because of the linear reductions ( Lehtinen and Inan, 2009;Shao et al., 2012), which implies that the disturbed electric field decreased 20 % compared with ...
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... the electric field varying with height is collected to study the influence of the electron disturbance. At nighttime, when i the variation of electron density is smaller, the variation of the electric field is also smaller (Fig. 10b, d). When the electron density increases by 4 times, the maximum electric field decreases about 2 dB at 120 km (see Fig. 10d). The variation is also 2 dB at DEMETER's altitude (660 km) because of the linear reductions ( Lehtinen and Inan, 2009;Shao et al., 2012), which implies that the disturbed electric field decreased 20 % compared with the original electric field (Fig. 8b). In the short time interval of a few days before the earthquake, the background ...
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... affected intensively during the main phase of the geomagnetic storm, gradually returning to normal accompanying the recovery phase. To avoid the effect of geomagnetic storms, the data which Kp > 3 and Dst < −30 nT were excluded in this research, and the TEC anomaly detected in Fig. 6 was seen 1 d after the recovery phase of the geomagnetic storm (Fig. 11a). Furthermore, the change pattern of TEC is totally different from the one caused by an earthquake because the TEC anomalies caused by a geomagnetic storm expand from high latitudes to mid latitudes due to thermospheric neutral winds, E × B convection, and so on ( Pokhotelov et al., 2008). From Fig. 11b, we can see SNR on the whole ...
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... recovery phase of the geomagnetic storm (Fig. 11a). Furthermore, the change pattern of TEC is totally different from the one caused by an earthquake because the TEC anomalies caused by a geomagnetic storm expand from high latitudes to mid latitudes due to thermospheric neutral winds, E × B convection, and so on ( Pokhotelov et al., 2008). From Fig. 11b, we can see SNR on the whole orbit are large on 5-7 and 11 April during geomagnetic storms, especially at the higher latitudes. However, the SNR pattern on 13 April is totally different; SNRs on the orbit of 13 April only decrease in the abnormal TEC region. In sum, the TEC anomaly on 13 April should be unconcerned with the geomagnetic ...
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... this paper, the SNR of the electric field from a groundbased VLF transmitter observed by the DEMETER satellite was analyzed before and after the 2010 Ms 7.1 Yushu earthquake. The VLF signals from Russian VLF transmit- Figure 10. The total electric field excited by the ground-based VLF transmitter NOV with a transmitting frequency of f = 11.9 kHz and power of P = 500 kW. ...

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... At present, the signal-to-interference-to-noise ratio (SNR) method is used for detecting satellite VLF radio wave signals to obtain earthquake-related disturbances. Studies have found that the SNR of the VLF radio wave signal decreases significantly before earthquakes, with recovery after the event and similar variations observed by multiple stations [27][28][29][30][31][32][33]. Similarly, the amplitude method used to detect satellite VLF wave signals can show a significant decrease or increase in the amplitude of the VLF wave signal before an earthquake [31][32][33][34][35]. ...
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Ionospheric disturbances are mainly caused by solar and Earth surface activity. The electromagnetic data collected by the CSES (China Seismo-Electromagnetic Satellite, popularly known as the Zhangheng-1 satellite) can capture many space disturbances. Different spatial disturbances can exhibit distinctive shapes on spectrograms. Constant-frequency electromagnetic disturbances (CFEDs) such as artificially transmitted VLF radio waves, power line harmonics, and satellite platform disturbances can appear as horizontal lines on spectrograms. Therefore, we used computer vision and machine learning techniques to extract the frequency of global CFEDs and analyze their strong spatial signal characteristics. First, we obtained time-frequency spectrograms from CSES VLF electric-field waveform data using Fourier transform. Next, we employed an unsupervised clustering algorithm to automatically recognize CFED horizontal lines on spectrograms, merging horizontal lines from different spectrograms, to obtain the CFED horizontal-line frequency range. In the third stage, we verified the presence of CFEDs in power spectrograms, thus extracting their true frequency values. Finally, for strong CFED signals, we generated eight revisited periods, resulting in 10,230 power spectrograms for analyzing each CFED’s spatial characteristics using a combined periodic sequence and spatial region that included frequency offsets, frequency fluctuations, and signal non-observation areas. These findings contribute to enhancing the quality of CSES observational data and provides a theoretical basis for constructing global CFED spatial background fields and earthquake monitoring and early prediction systems.
... The first one is based on the physical mechanism of the seismic wave generation into the atmosphere [27]. The other relies on analyses of statistics and the probability of TEC anomalies in the epicenter regions and time of earthquake occurrences (mainshocks) [28]. However, there is no absolutely certain guarantee about the coincidence between observed ionospheric anomalies in the location and time of the earthquakes with other non-seismic activities. ...
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