On the Relation Between Soft Electron Precipitations in the Cusp Region and Solar Wind Coupling Functions

In this study, the correlations between the fluxes of precipitating soft electrons in the cusp region and solar wind coupling functions are investigated utilizing the Lyon‐Fedder‐Mobarry global magnetosphere model simulations. We conduct two simulation runs during periods from 20 March 2008 to 16 April 2008 and from 15 to 24 December 2014, which are referred as “Equinox Case” and “Solstice Case,” respectively. The simulation results of Equinox Case show that the plasma number density in the high‐latitude cusp region scales well with the solar wind number density (ncusp/nsw=0.78), which agrees well with the statistical results from the Polar spacecraft measurements. For the Solstice Case, the plasma number density of high‐latitude cusp in both hemispheres increases approximately linearly with upstream solar wind number density with prominent hemispheric asymmetry. Due to the dipole tilt effect, the average number density ratio ncusp/nsw in the Southern (summer) Hemisphere is nearly 3 times that in the Northern (winter) Hemisphere. In addition to the solar wind number density, 20 solar wind coupling functions are tested for the linear correlation with the fluxes of precipitating cusp soft electrons. The statistical results indicate that the solar wind dynamic pressure p exhibits the highest linear correlation with the cusp electron fluxes for both equinox and solstice conditions, with correlation coefficients greater than 0.75. The linear regression relations for equinox and solstice cases may provide an empirical calculation for the fluxes of cusp soft electron precipitation based on the upstream solar wind driving conditions.

[1]  Roger H. Varney,et al.  Influence of ion outflow in coupled geospace simulations: 1. Physics‐based ion outflow model development and sensitivity study , 2016 .

[2]  J. Lyon,et al.  Influence of ion outflow in coupled geospace simulations: 2. Sawtooth oscillations driven by physics‐based ion outflow , 2016 .

[3]  D. Welling,et al.  Density variations in the Earth's magnetospheric cusps , 2016 .

[4]  J. Lyon,et al.  Pathways of F region thermospheric mass density enhancement via soft electron precipitation , 2015 .

[5]  R. McPherron,et al.  An optimum solar wind coupling function for the AL index , 2015 .

[6]  M. Wiltberger,et al.  Modeling the interaction between convection and nonthermal ion outflows , 2015 .

[7]  J. Lyon,et al.  Electron precipitation models in global magnetosphere simulations , 2015 .

[8]  Larry J. Paxton,et al.  OVATION Prime‐2013: Extension of auroral precipitation model to higher disturbance levels , 2014 .

[9]  M. Liemohn,et al.  Outflow in global magnetohydrodynamics as a function of a passive inner boundary source , 2014 .

[10]  J. Lyon,et al.  Predicting the location of polar cusp in the Lyon‐Fedder‐Mobarry global magnetosphere simulation , 2013 .

[11]  Joseph E. Borovsky,et al.  Physical improvements to the solar wind reconnection control function for the Earth's magnetosphere , 2013 .

[12]  Ramon Lopez,et al.  Theoretical study: Influence of different energy sources on the cusp neutral density enhancement , 2013 .

[13]  J. Lyon,et al.  Enhancement of thermospheric mass density by soft electron precipitation , 2012 .

[14]  H. Carlson,et al.  On the relationship between flux transfer events, temperature enhancements, and ion upflow events in the cusp ionosphere , 2011 .

[15]  M. Wiltberger,et al.  Magnetosphere Sawtooth Oscillations Induced by Ionospheric Outflow , 2011, Science.

[16]  J. Lyon,et al.  Effects of the low-latitude ionospheric boundary condition on the global magnetosphere , 2010 .

[17]  T. Yeoman,et al.  Thermal ion upflow in the cusp ionosphere and its dependence on soft electron energy flux , 2010 .

[18]  Patrick T. Newell,et al.  Diffuse, monoenergetic, and broadband aurora: The global precipitation budget , 2009 .

[19]  S. Rentz The Upper Atmospheric Fountain Effect in the Polar Cusp Region , 2009 .

[20]  R. Elphic,et al.  Factors controlling ionospheric outflows as observed at intermediate altitudes , 2005 .

[21]  John Lyon,et al.  The Lyon-Fedder-Mobarry (LFM) global MHD magnetospheric simulation code , 2004 .

[22]  S. Nozawa,et al.  Simultaneous EISCAT Svalbard radar and DMSP observations of ion upflow in the dayside polar ionosphere , 2003 .

[23]  Joseph P. Skura,et al.  OVATION: Oval variation, assessment, tracking, intensity, and online nowcasting , 2002 .

[24]  C. Russell,et al.  The polar cusp location and its dependence on dipole tilt , 1999 .

[25]  B. Anderson,et al.  The diffuse aurora: A significant source of ionization in the middle atmosphere , 1997 .

[26]  M. F. Smith,et al.  Earth's magnetospheric cusps , 1996 .

[27]  J. Wahlund,et al.  EISCAT observations of topside ionospheric ion outflows during auroral activity: Revisited , 1992 .

[28]  C. Russell,et al.  Proxy studies of energy transfer to the magnetosphere , 1991 .

[29]  C. Meng,et al.  Some low‐altitude cusp dependencies on the interplanetary magnetic field , 1989 .

[30]  Raymond G. Roble,et al.  An auroral model for the NCAR thermospheric general circulation model (TGCM) , 1987 .

[31]  R. Eather Polar cusp dynamics , 1985 .

[32]  F. Mozer,et al.  Comparison of S3-3 polar cap potential drops with the interplanetary magnetic field and models of magnetopause reconnection , 1983 .

[33]  G. Siscoe,et al.  Scaling relations governing magnetospheric energy transfer , 1982 .

[34]  Lou‐Chuang Lee,et al.  Energy coupling function and solar wind‐magnetosphere dynamo , 1979 .

[35]  V. L. Patel,et al.  A study of geomagnetic storms , 1975 .

[36]  C. D. Anger,et al.  The diffuse aurora , 1973 .

[37]  J. Winningham,et al.  Penetration of magnetosheath plasma to low altitudes through the dayside magnetospheric cusps , 1971 .

[38]  Frederick J. Rich,et al.  A nearly universal solar wind-magnetosphere coupling function inferred from 10 magnetospheric state variables , 2007 .

[39]  V. Lazarev ABSORPTION OF THE ENERGY OF AN ELECTRON BEAM IN THE UPPER ATMOSPHERE. , 1967 .