Polar Ion Temperature Variations During the 22 January 2012 Magnetic Storm

We study the 22 January 2012 magnetic storm, during which some localized neutral density (DN) increases developed, and its polar ion temperature (Ti) variations in terms of the earthward Poynting flux (S||) deposited into the coupled ionosphere‐thermosphere system. We investigate the storm's nature, some flow channel events that are the ionospheric signatures of flux transfer events triggered by magnetic reconnections, and the resultant thermospheric responses. We utilize solar and interplanetary magnetic field data and multi‐instrument topside ionospheric and thermospheric measurements. Results reveal the presence of antisunward propagating solar wind Alfven waves during the various storm phases triggering flux transfer events/flow channel events and launching atmospheric gravity waves whose Ti signatures appeared as episodic Ti variations. Various scenarios demonstrate the direct correlation between S|| and DN and the irregular Ti responses within/above flow channels that we explain in terms of frictional heating (Tfrc). We identify Ti responses during various flow channel events as (1) direct/intermittent and (2) opposite, with S|| and DN reflecting the respective underlying flow channel development at the time of detection as (1) early stage when Tfrc was high due to the still large velocity differences between ions and neutrals and as (2) late stage when Tfrc ceased since ions and neutrals moved together. Ti oscillations are observed to be originating from polar or auroral flow channels and propagating across the polar cap toward the equator. We conclude that antisunward solar wind Alfven waves had a significant impact on Ti variability during this storm by modulating magnetic reconnection and launching atmospheric gravity waves.

[1]  E. Sutton,et al.  Occurrence Locations, Dipole Tilt Angle Effects, and Plasma Cloud Drift Paths of Polar Cap Neutral Density Anomalies , 2018 .

[2]  E. Sutton,et al.  High‐Latitude Neutral Mass Density Maxima , 2017 .

[3]  W. Wan,et al.  Alfvén waves as a solar-interplanetary driver of the thermospheric disturbances , 2016, Scientific Reports.

[4]  M. Lester,et al.  Substorm Current Wedge Revisited , 2015 .

[5]  X. Fang,et al.  Ionization due to electron and proton precipitation during the August 2011 storm , 2014 .

[6]  E. Sutton,et al.  Energy coupling during the August 2011 magnetic storm , 2013 .

[7]  Stanley W. H. Cowley,et al.  Magnetosphere‐Ionosphere Interactions: A Tutorial Review , 2013 .

[8]  H. Carlson,et al.  First‐principles physics of cusp/polar cap thermospheric disturbances , 2012 .

[9]  C. Farrugia,et al.  The pulsed nature of the nightside contribution to polar cap convection: repetitive substorm activity under steady interplanetary driving , 2012 .

[10]  R. Roble,et al.  Height distribution of Joule heating and its influence on the thermosphere , 2012 .

[11]  C. Farrugia,et al.  Plasma flows, Birkeland currents and auroral forms in relation to the Svalgaard-Mansurov effect , 2012 .

[12]  J. Meriwether,et al.  The phases and amplitudes of gravity waves propagating and dissipating in the thermosphere: Application to measurements over Alaska , 2012 .

[13]  M. Nicolls,et al.  The phases and amplitudes of gravity waves propagating and dissipating in the thermosphere: Theory , 2012 .

[14]  J. Wild,et al.  A statistical comparison of solar wind propagation delays derived from multispacecraft techniques , 2012 .

[15]  C. Farrugia,et al.  Substorms and polar cap convection: the 10 January 2004 interplanetary CME case , 2012 .

[16]  C. Farrugia,et al.  Dayside and nightside contributions to cross-polar cap potential variations: The 20 March 2001 ICME case , 2011 .

[17]  Kazue Takahashi,et al.  Review of Pi2 Models , 2011 .

[18]  G. Crowley,et al.  Extreme Poynting flux in the dayside thermosphere: Examples and statistics , 2011 .

[19]  G. W. Prölss Density Perturbations in the Upper Atmosphere Caused by the Dissipation of Solar Wind Energy , 2011 .

[20]  A. Richmond On the ionospheric application of Poynting's theorem , 2010 .

[21]  Eelco Doornbos,et al.  Neutral Density and Crosswind Determination from Arbitrarily Oriented Multiaxis Accelerometers on Satellites , 2010 .

[22]  G. Crowley,et al.  Thermospheric density enhancements in the dayside cusp region during strong BY conditions , 2010 .

[23]  S. Oyama,et al.  Ion heating in high‐speed flow channel within the duskside cell of the polar cap ion convection under large IMF‐By condition , 2009 .

[24]  C. Farrugia,et al.  Plasma flow channels at the dawn/dusk polar cap boundaries: momentum transfer on old open field lines and the roles of IMF B y and conductivity gradients , 2008 .

[25]  Stein Haaland,et al.  What is the best method to calculate the solar wind propagation delay , 2008 .

[26]  P. Stauning A new index for the interplanetary merging electric field and geomagnetic activity: Application of the unified polar cap indices , 2007 .

[27]  W. J. Burke,et al.  Prompt thermospheric response to the 6 November 2001 magnetic storm , 2007 .

[28]  C. Farrugia,et al.  Spatiotemporal structure of the reconnecting magnetosphere under By‐dominated interplanetary magnetic cloud conditions , 2006 .

[29]  C. Russell,et al.  Statistics of a parallel Poynting vector in the auroral zone as a function of altitude using Polar EFI and MFE data and Astrid-2 EMMA data , 2005 .

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

[31]  C. Farrugia,et al.  Detailed dayside auroral morphology as a function of local time for southeast IMF orientation: implications for solar wind-magnetosphere coupling , 2004 .

[32]  H. Carlson,et al.  The dynamics and relationships of precipitation, temperature and convection boundaries in the dayside auroral ionosphere , 2004 .

[33]  W. J. Burke,et al.  Transient sheets of field-aligned current observed by DMSP during the main phase of a magnetic superstorm , 2004 .

[34]  G. Sofko,et al.  Solar wind Alfvén waves: a source of pulsed ionospheric convection and atmospheric gravity waves , 2004 .

[35]  L. Grunwaldt,et al.  Thermospheric up‐welling in the cusp region: Evidence from CHAMP observations , 2004 .

[36]  X. Pi,et al.  Case study of the 15 July 2000 magnetic storm effects on the ionosphere-driver of the positive ionospheric storm in the winter hemisphere , 2003 .

[37]  William J. Burke,et al.  SAPS: A new categorization for sub‐auroral electric fields , 2002 .

[38]  T. Yeoman,et al.  Ionospheric cusp flows pulsed by solar wind Alfvén waves , 2002 .

[39]  G. Sofko,et al.  Eastward convection jet at the poleward boundary of the nightside auroral oval , 2000 .

[40]  C. Russell,et al.  Cusp field‐aligned currents and ion outflows , 2000 .

[41]  D. P. Steele,et al.  Observations of polar patches generated by solar wind Alfvén wave coupling to the dayside magnetosphere , 1999 .

[42]  T. Yeoman,et al.  The influence of the IMF By component on the location of pulsed flows in the dayside ionosphere observed by an HF radar , 1999 .

[43]  S. Milan,et al.  CUTLASS Finland radar observations of the ionospheric signatures of flux transfer events and the resulting plasma flows , 1998 .

[44]  W. J. Burke,et al.  Dynamics of the inner magnetosphere near times of substorm onsets , 1996 .

[45]  F. S. Johnson,et al.  Gravity waves near 300 km over the polar caps , 1995 .

[46]  H. Carlson,et al.  Interplanetary magnetic field dependency of stable Sun-aligned polar cap arcs , 1994 .

[47]  Frederick J. Rich,et al.  Large-scale convection patterns observed by DMSP , 1994 .

[48]  Raymond A. Greenwald,et al.  Observations of an enhanced convection channel in the cusp ionosphere , 1993 .

[49]  R. A. Mewaldt,et al.  The Advanced Composition Explorer , 1988 .

[50]  M. Lockwood,et al.  The modelled occurrence of non-thermal plasma in the ionospheric F-region and the possible consequences for ion outflows into the magnetosphere , 1987 .

[51]  H. G. Mayr,et al.  Global excitation of wave phenomena in a dissipative multiconstituent medium: 2. Impulsive perturbations in the Earth's thermosphere , 1984 .

[52]  H. G. Mayr,et al.  Global excitation of wave phenomena in a dissipative multiconstituent medium: 1. Transfer function of the Earth's thermosphere , 1984 .

[53]  J. St.‐Maurice,et al.  The interplanetary electric field, cleft currents and plasma convection in the polar caps , 1984 .

[54]  H. G. Mayr,et al.  Global excitation of wave phenomena in a dissipative multiconstituent medium. I - Transfer function of the earth's thermosphere. II - Impulsive perturbations in the earth's thermosphere , 1984 .

[55]  M. Baron,et al.  F region ion temperature enhancements resulting from Joule heating , 1983 .

[56]  Robert W. Schunk,et al.  Ion‐neutral momentum coupling near discrete high‐latitude ionospheric features , 1981 .

[57]  C. T. Russell,et al.  Initial ISEE magnetometer results: magnetopause observations , 1978 .

[58]  Christopher T. Russell,et al.  Initial ISEE magnetometer results - Magnetopause observations , 1978 .

[59]  Peter M. Banks,et al.  Observations of joule and particle heating in the auroral zone , 1977 .

[60]  J. Dungey Interplanetary Magnetic Field and the Auroral Zones , 1961 .

[61]  E. Sutton,et al.  Ionosphere-thermosphere (IT) response to solar wind forcing during magnetic storms , 2016 .

[62]  M. Kivelson,et al.  Dynamical polar cap: A unifying approach , 1997 .

[63]  C. E. Valladares,et al.  Experimental evidence for the formation and entry of patches into the polar cap , 1994 .

[64]  H. Volland,et al.  Possible evidence for coronal Alfvén waves , 1982 .