Nonmigrating tidal signature in the distributions of equatorial plasma bubbles and prereversal enhancement

Some wave-like features in the longitudinal distribution of equatorial plasma bubbles understood in association with diurnal eastward propagating zonal wave number 3 nonmigrating tide (DE3) in the dayside. However, whether or not the wave features are the daytime DE3 signature has not yet been rigorously investigated. This study investigates (1) the existence of the DE3 signature in the longitudinal distribution of bubbles by analyzing the first Republic of China (ROCSAT-1) satellite data acquired in 2000–2002 and (2) the role of daytime DE3 in the creation of bubbles by examining the linear growth rate of the generalized Rayleigh-Taylor (R-T) instability. The linear growth rate is derived from the “Sami2 is Another Model of the Ionosphere” model simulation results. In the longitudinal distribution of bubbles derived from ROCSAT-1 observations, the wave number 4 component, the representative characteristic of DE3, is a weak feature. In addition, the amplitude and phase of the wave number 4 component do not show a consistent behavior in comparison with those of DE3. Our numerical calculation results show that the linear growth rate of the R-T instability is not sensitive to the variation of the daytime vertical plasma drift. These results indicate that the DE3 signature in the occurrence rate of bubbles is not obvious and the effect of daytime DE3 on the creation of bubbles is negligible.

[1]  Jeffrey M. Forbes,et al.  Migrating and nonmigrating diurnal tides in the middle and upper atmosphere excited by tropospheric latent heat release , 2002 .

[2]  Chao Xiong,et al.  Comparing plasma bubble occurrence rates at CHAMP and GRACE altitudes during high and low solar activity , 2010 .

[3]  T. Hagfors,et al.  Earth's Ionosphere , 2001 .

[4]  Glenn Joyce,et al.  Sami2 is Another Model of the Ionosphere (SAMI2): A new low-latitude ionosphere model , 2000 .

[5]  Georgios Balasis,et al.  Magnetic signatures of equatorial spread F as observed by the CHAMP satellite , 2006 .

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

[7]  E. R. Paula,et al.  Effects of the vertical plasma drift velocity on the generation and evolution of equatorial spread F , 1999 .

[8]  L. Paxton,et al.  Longitudinal structure of the vertical E × B drift and ion density seen from ROCSAT‐1 , 2007 .

[9]  A. Hedin MSIS‐86 Thermospheric Model , 1987 .

[10]  Chi-Kuang Chao,et al.  Distribution characteristics of topside ionospheric density irregularities: Equatorial versus midlatitude regions , 2006 .

[11]  Larry J. Paxton,et al.  Morphology of the equatorial anomaly and equatorial plasma bubbles using image subspace analysis of Global Ultraviolet imager data , 2005 .

[12]  R. Heelis,et al.  Global Distribution of Density Irregularities in the Equatorial Ionosphere , 1998 .

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

[14]  N. W. Spencer,et al.  Revised global model of thermosphere winds using satellite and ground‐based observations , 1991 .

[15]  L. Paxton,et al.  Wave structures of the plasma density and vertical E × B drift in low‐latitude F region , 2008 .

[16]  Ludger Scherliess,et al.  Radar and satellite global equatorial F-region vertical drift model , 1999 .

[17]  R. Heelis,et al.  The ROCSAT-1 IPEI Preliminary Results: Vertical Ion Drift Statistics , 1999 .

[18]  A. Hedin Extension of the MSIS Thermosphere Model into the middle and lower atmosphere , 1991 .

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

[20]  J. Huba,et al.  Impact of meridional winds on equatorial spread F: Revisited , 2013 .

[21]  Xinan Yue,et al.  Correlative study of plasma bubbles, evening equatorial ionization anomaly, and equatorial prereversal E × B drifts at solar maximum , 2008 .

[22]  L. Paxton,et al.  Causal Link of Longitudinal Plasma Density Structure to Vertical Plasma Drift and Atmospheric Tides – A Review , 2011 .

[23]  Larry J. Paxton,et al.  High-resolution vertical E × B drift model derived from ROCSAT-1 data , 2009 .

[24]  Michael C. Kelley,et al.  The earth's ionosphere , 1989 .

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

[26]  J. Forbes,et al.  Tidal variability in the ionospheric dynamo region , 2008 .

[27]  R. Heelis,et al.  Topside signature of medium-scale traveling ionospheric disturbances , 2014 .

[28]  Larry J. Paxton,et al.  Control of equatorial ionospheric morphology by atmospheric tides , 2006 .

[29]  S. Zalesak,et al.  Three-dimensional simulation of equatorial spread-F with meridional wind effects , 2009 .

[30]  John M. Retterer,et al.  Longitudinal and seasonal dependence of nighttime equatorial plasma density irregularities during solar minimum detected on the C/NOFS satellite , 2011 .

[31]  T. Killeen,et al.  Diurnal nonmigrating tides from TIMED Doppler Interferometer wind data: Monthly climatologies and seasonal variations , 2006 .