Global distribution characteristics of

  • role: First author第一作者
  • Affiliation:

    武汉大学电子信息学院 电离层实验室,武汉,430072

刘祎1,  
  • Affiliation:

    武汉大学电子信息学院 电离层实验室,武汉,430072

  • No information about the author is available
孙睿迪1,  
  • Affiliation:

    武汉大学电子信息学院 电离层实验室,武汉,430072

  • No information about the author is available
周晨1,  
  • Affiliation:

    中国地震局地震预测研究所,北京,100036

  • No information about the author is available
赵庶凡2,  
  • Affiliation:

    中国地震局地震预测研究所,北京,100036

  • No information about the author is available
张学民2,  
  • Affiliation:

    中国地震局地壳应力研究所,北京,100085

  • No information about the author is available
申旭辉3,  
  • Affiliation:

    武汉大学电子信息学院 电离层实验室,武汉,430072

  • No information about the author is available
赵正予1

resumen

The ionosphere is an atmospheric region ionized by solar radiation, cosmic rays, and various particle radiations ranging from 60 km to 1000 km above the earth. Numerous free electrons and ions in the ionosphere can interfere with radio signals. Ionospheric parameters, especially F2 layer critical frequency (f0F2) and electron density peak height (hmF2), play an important role in the propagation of HF waves. Therefore, the study of f0F2 and hmF2, especially its global distribution, is important.The overall objective of this paper is to study the annual, diurnal, and seasonal variations of f0F2 and hmF2 in the world on the basis of GNSS occulation datasets and to compare the values f0F2 obtained by GNSS occultation and digisondes from all stations in Japan.COSMIC, GRACE, and CHAMP electron density profile datasets and digisonde datasets in Wakkanai, Kokubunji, Yamagawa, and Okinawa for 2002—2016 are selected as the data sources. The maximum electron density NmF2 and hmF2 is obtained by using the electron density profile. Compared with ionosonde f0F2 datasets, the latitude and longitude of the selected NmF2 are within 5 degrees of ionosondes, and the time of the selected NmF2 is within 15 minutes of ionosondes.Results show that the annual variation of f0F2 and hmF2 has a significant positive correlation with solar activity and geomagnetic activity and significant spatial distribution characteristics. The maximum value of f0F2 distribution on both sides of the magnetic equator is approximately 15 degrees, and the maximum value of hmF2 distribution in the equatorial region and the northern and southern hemisphere peak heights is not symmetrical. In addition, the peak value of f0F2 and hmF2 appears during LT 14:00—16:00, and hmF2 exhibits significant equatorial ionization anomaly recovery after sunset. The f0F2 has obvious seasonal characteristics; the peak value of f0F2 appears in spring and autumn at middle and low latitudes, and is evident in abnormal winter phenomenon. However, the seasonal distribution of hmF2 evidently change. The values f0F2, which were obtained by occultation and digisondes from all stations in Japan, were compared, and results indicate that the ionospheric parameters obtained by the two detection methods have acceptable correlation. The correlation in the Okinawa station is the best, with a correlation coefficient of 0.88. The correlation in the Wakkanai station is poor, with a correlation coefficient of 0.75. The correlation between Yamagawa and Kokubunji stations is close at 0.84 and 0.85, respectively.The preliminary study shows that the global f0F2 and hmF2 distribution is affected by many factors, including solar activity, geomagnetic activity, electric field, and wind and high-energy particle sedimentation.The values f0F2 obtained by occultation and digisondes from all stations in Japan were compared, and results show that the ionospheric parameters obtained by the two detection methods have acceptable correlation. However, some evident differences were observed; these differences may be due to the electron density gradient and satellite retrieval technology.

palabra clave

annual variation of;f;0;F;2;and;h;m;2;diurnal variation of;2;seasonal variation of;2;digisondes;GNSS

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