Daily and seasonal variations in the linear growth rate of the Rayleigh-Taylor instability in the ionosphere obtained with GAIA

AbstractThe linear growth rates of the Rayleigh-Taylor (R-T) instability in the ionosphere from 2011 to 2013 were obtained with a whole atmosphere-ionosphere coupled model GAIA (ground-to-topside model of atmosphere and ionosphere for aeronomy). The effects of thermospheric dynamics driven by atmospheric waves propagating from below on the R-T growth rate are included in the model by incorporating meteorological reanalysis data in the region below 30 km altitude. The daily maximum R-T growth rates for these periods are compared with the observed occurrence days of the equatorial plasma bubble (EPB) determined by the Equatorial Atmosphere Radar (EAR) and Global Positioning System (GPS) in West Sumatra, Indonesia. We found that a high R-T growth rate tends to correspond to the actual EPB occurrence, suggesting the possibility of predicting EPB occurrences with numerical models.

[1]  Qian Wu Longitudinal and seasonal variation of the equatorial flux tube integrated Rayleigh‐Taylor instability growth rate , 2015 .

[2]  G. Haerendel,et al.  Theory for modeling the equatorial evening ionosphere and the origin of the shear in the horizontal plasma flow , 1992 .

[3]  H. Fujiwara,et al.  Excitation mechanism of non-migrating tides , 2017 .

[4]  V. Sreeja,et al.  Impact and mitigation of space weather effects on GNSS receiver performance , 2016, Geoscience Letters.

[5]  M. Yamamoto,et al.  Altitude development of postmidnight F region field‐aligned irregularities observed using Equatorial Atmosphere Radar in Indonesia , 2016 .

[6]  R. Sridharan,et al.  Local time dependent response of postsunset ESF during geomagnetic storms , 2008 .

[7]  S. Zalesak,et al.  Nonlinear equatorial spread F: dependence on altitude of the F peak and bottomside background electron density gradient scale length. Interim report , 1978 .

[8]  J. Marshall Shepherd,et al.  Aerosol relationships to warm season clouds and rainfall at monthly scales over east China: Urban land versus ocean , 2008 .

[9]  Chaosong Huang Occurrence of Equatorial Plasma Bubbles during Intense Magnetic Storms , 2011 .

[10]  Tadahiko Ogawa,et al.  VHF radar observations of nighttime F-region field-aligned irregularities over Kototabang, Indonesia , 2009 .

[11]  H. Fujiwara,et al.  A global view of gravity waves in the thermosphere simulated by a general circulation model , 2014 .

[12]  H. Fujiwara,et al.  Gravity Waves in the Thermosphere Simulated by a General Circulation Model , 2008 .

[13]  H. Fujiwara,et al.  Excitation mechanism of intraseasonal oscillation in the equatorial mesosphere and lower thermosphere , 2006 .

[14]  T. Yokoyama,et al.  Spatial relationship of equatorial plasma bubbles and field‐aligned irregularities observed with an all‐sky airglow imager and the Equatorial Atmosphere Radar , 2004 .

[15]  S. Basu,et al.  Response of the equatorial ionosphere at dusk to penetration electric fields during intense magnetic storms , 2007 .

[16]  Tadahiko Ogawa,et al.  Equatorial Ionospheric Scintillations and Zonal Irregularity Drifts Observed with Closely-Spaced GPS Receivers in Indonesia( CPEA-Coupling Processes in the Equatorial Atmosphere) , 2006 .

[17]  Hiroshi Oya,et al.  Occurrence Characteristics of Low Latitude Ionosphere Irregularities Observed by Impedance Probe on Board the Hinotori Satellite , 1986 .

[18]  Keith M. Groves,et al.  Ionospheric scintillation effects on single frequency GPS , 2008 .

[19]  D. Hysell,et al.  Three‐dimensional numerical simulation of equatorial F region plasma irregularities with bottomside shear flow , 2010 .

[20]  Mamoru Yamamoto,et al.  Eastward traverse of equatorial plasma plumes observed with the Equatorial Atmosphere Radar in Indonesia , 2006 .

[21]  H. Fujiwara,et al.  Global distribution of the thermospheric disturbances produced by effects from the upper and lower regions: simulations by a whole atmosphere GCM , 2009 .

[22]  P. J. Sultan,et al.  Linear theory and modeling of the Rayleigh‐Taylor instability leading to the occurrence of equatorial spread F , 1996 .

[23]  L. C. Gentile,et al.  Equatorial plasma bubbles observed by DMSP satellites during a full solar cycle: Toward a global climatology , 2002 .

[24]  L. C. Gentile,et al.  Longitudinal variability of equatorial plasma bubbles observed by DMSP and ROCSAT‐1 , 2004 .

[25]  J. Huba,et al.  Equatorial spread F modeling: Multiple bifurcated structures, secondary instabilities, large density ‘bite‐outs,’ and supersonic flows , 2007 .

[26]  T. Yokoyama,et al.  Nonlinear growth, bifurcation, and pinching of equatorial plasma bubble simulated by three‐dimensional high‐resolution bubble model , 2014 .

[27]  Raymond G. Roble,et al.  A thermosphere/ionosphere general circulation model with coupled electrodynamics , 1992 .

[28]  H. Fujiwara,et al.  Response of migrating tides to the stratospheric sudden warming in 2009 and their effects on the ionosphere studied by a whole atmosphere-ionosphere model GAIA with COSMIC and TIMED/SABER observations , 2012 .

[29]  Huixin Liu,et al.  Wave-4 structure of the neutral density in the thermosphere and its relation to atmospheric tides , 2012 .

[30]  T. Yokoyama,et al.  Explicit characteristics of evolutionary‐type plasma bubbles observed from Equatorial Atmosphere Radar during the low to moderate solar activity years 2010–2012 , 2015 .

[31]  Patrick A. Roddy,et al.  Occurrence probability and amplitude of equatorial ionospheric irregularities associated with plasma bubbles during low and moderate solar activities (2008–2012) , 2013 .

[32]  Qian Wu Solar effect on the Rayleigh-Taylor instability growth rate as simulated by the NCAR TIEGCM , 2017 .

[33]  H. Jin,et al.  Electrodynamics of the formation of ionospheric wave number 4 longitudinal structure , 2008 .

[34]  T. Yokoyama,et al.  First observations of the spatial structure of F region 3‐m‐scale field‐aligned irregularities with the Equatorial Atmosphere Radar in Indonesia , 2004 .

[35]  L. C. Gentile,et al.  Seasonal-longitudinal variability of equatorial plasma bubbles , 2004 .

[36]  T. Yokoyama,et al.  West wall structuring of equatorial plasma bubbles simulated by three-dimensional HIRB model: WEST WALL STRUCTURING OF PLASMA BUBBLE , 2015 .

[37]  Sidney L. Ossakow,et al.  Nonlinear equatorial spread F: The effect of neutral winds and background Pedersen conductivity , 1982 .

[38]  W. J. Burke,et al.  A climatology of equatorial plasma bubbles from DMSP 1989–2004 , 2006 .

[39]  B. Basu On the linear theory of equatorial plasma instability: Comparison of different descriptions , 2002 .

[40]  Keith M. Groves,et al.  Geomagnetic control of equatorial plasma bubble activity modeled by the TIEGCM with Kp , 2014 .

[41]  Naoki Terada,et al.  Vertical connection from the tropospheric activities to the ionospheric longitudinal structure simulated by a new Earth's whole atmosphere-ionosphere coupled model , 2011 .

[42]  H. Fujiwara,et al.  Morphological features and variations of temperature in the upper thermosphere simulated by a whole atmosphere GCM , 2010 .

[43]  Hitoshi Fujiwara,et al.  Day‐to‐day variations of migrating diurnal tide simulated by a GCM from the ground surface to the exobase , 2003 .

[44]  Mamoru Yamamoto,et al.  On the fresh development of equatorial plasma bubbles around the midnight hours of June solstice , 2016 .

[45]  E. Ott Theory of Rayleigh-Taylor bubbles in the equatorial ionosphere , 1978 .

[46]  T. Yokoyama,et al.  West wall structuring of equatorial plasma bubbles simulated by three‐dimensional HIRB model , 2015 .

[47]  Ronald F. Woodman,et al.  Radar observations of F region equatorial irregularities , 1976 .

[48]  Ken T. Murata,et al.  On post‐midnight field‐aligned irregularities observed with a 30.8‐MHz radar at a low latitude: Comparison withF‐layer altitude near the geomagnetic equator , 2012 .

[49]  M. Hairston,et al.  The postsunset vertical plasma drift and its effects on the generation of equatorial plasma bubbles observed by the C/NOFS satellite , 2014 .

[50]  Takuji Nakamura,et al.  Equatorial GPS ionospheric scintillations over Kototabang, Indonesia and their relation to atmospheric waves from below , 2009 .

[51]  J. Randerson,et al.  The influence of burn severity on postfire vegetation recovery and albedo change during early succession in North American boreal forests , 2011 .

[52]  K. Shiokawa,et al.  VHF radar observations of post-midnight F-region field-aligned irregularities over Indonesia during solar minimum , 2012 .

[53]  Anthony J. Scannapieco,et al.  Nonlinear equatorial spread F , 1976 .

[54]  Kefei Zhang,et al.  An analysis of the quiet time day‐to‐day variability in the formation of postsunset equatorial plasma bubbles in the Southeast Asian region , 2014 .

[55]  L. Paxton,et al.  Global bubble distribution seen from ROCSAT-1 and its association with the evening prereversal enhancement , 2009 .

[56]  Takuya Tsugawa,et al.  Occurrence characteristics of plasma bubble derived from global ground‐based GPS receiver networks , 2007 .