Structured subauroral polarization streams and related auroral undulations occurring on the storm day of 21 January 2005

We investigate structured subauroral polarization streams (SAPS) and their impacts on the midlatitude trough and auroral regions during the 21–22 January 2005 geomagnetic storm. This was a storm with two sudden commencements occurring under varying interplanetary magnetic field (IMF) conditions and three main phases, two of them unfolding during northward IMF. Its onset at ~1700 UT allowed us to investigate SAPS wave structures (WS) and their impacts during the local evening hours under both southward and northward IMF conditions in the American sector. Results suggest that during southward IMF, SAPS‐WS might be related with standing (toroidal) Alfven waves and structured most intensively the stagnation trough. During northward IMF, the trough was created by SAPS electric (E) field effects only and became less structured by SAPS‐WS that were of Alfvenic origin. Auroral wave structures and undulations occurred in the structured and unstructured oval regions, respectively, and triggered the subauroral region's response to produce SAPS‐WS. Spectrogram images (only one shown) confirmed ring current injections implying magnetotail reconnections during the four SAPS‐WS events investigated. Periodic tail connections are also evidenced by the periodic increases seen in both the solar wind‐magnetosphere coupling function (ε) and the energy input efficiency. Finally, we conclude for the time period investigated that (1) the nature of SAPS‐WS was informative of IMF orientation, (2) plasma stagnation enhanced SAPS E field and SAPS‐WS development, and (3) more efficient energy input into the magnetosphere contributed to the better development of auroral undulations and SAPS‐WS.

[1]  V. Kalegaev,et al.  Dynamics of the magnetosphere during geomagnetic storms on January 21–22, 2005 and December 14–15, 2006 , 2015 .

[2]  J. Richardson,et al.  Solar wind‐magnetosphere energy coupling function fitting: Results from a global MHD simulation , 2014 .

[3]  C. Farrugia,et al.  M–I coupling across the auroral oval at dusk and midnight: repetitive substorm activity driven by interplanetary coronal mass ejections (CMEs) , 2014 .

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

[5]  E. Mishin Interaction of substorm injections with the subauroral geospace: 1. Multispacecraft observations of SAID , 2013 .

[6]  Hongqiao Hu,et al.  Direct Observations of the Evolution of Polar Cap Ionization Patches , 2013, Science.

[7]  E. Mishin,et al.  Irregularities within Subauroral Polarization Stream‐Related Troughs and GPS Radio Interference at Midlatitudes , 2013 .

[8]  E. W. Hones Plasma Sheet Behavior During Substorms , 2013 .

[9]  B. Tsurutani,et al.  Comments on "interplanetary and geomagnetic parameters during January 16-26, 2005" by R.P. Kane , 2012 .

[10]  W. Xu,et al.  Characteristics of magnetospheric energetics during geomagnetic storms , 2012 .

[11]  Y. Xiong,et al.  Wave‐particle interaction in a plasmaspheric plume observed by a Cluster satellite , 2012 .

[12]  E. Amata,et al.  Super fast plasma streams as drivers of transient and anomalous magnetospheric dynamics , 2012 .

[13]  Jann‐Yenq Liu,et al.  The ionospheric midlatitude trough observed by FORMOSAT‐3/COSMIC during solar minimum , 2011 .

[14]  I. Mann,et al.  Start-to-end global imaging of a sunward propagating, SAPS-associated giant undulation event , 2010 .

[15]  S. Morley,et al.  Multipoint observations of Pc1-2 waves in the afternoon sector , 2009 .

[16]  R. Horne,et al.  Simulation of EMIC wave excitation in a model magnetosphere including structured high-density plumes , 2009 .

[17]  A. Keiling Alfvén Waves and Their Roles in the Dynamics of the Earth’s Magnetotail: A Review , 2009 .

[18]  B. Tsurutani,et al.  Anomalous geomagnetic storm of 21-22 January 2005: A storm main phase during northward IMFs , 2008 .

[19]  M. Spasojević,et al.  Modeling the electromagnetic ion cyclotron wave‐induced formation of detached subauroral proton arcs , 2007 .

[20]  V. Mishin,et al.  Prompt response of SAPS to stormtime substorms , 2007 .

[21]  G. W. Prölss Subauroral electron temperature enhancement in the nighttime ionosphere , 2006 .

[22]  W. Rideout,et al.  Multiradar observations of the polar tongue of ionization , 2005 .

[23]  W. J. Burke,et al.  Stormtime coupling of the ring current, plasmasphere, and topside ionosphere: Electromagnetic and plasma disturbances , 2005 .

[24]  A. Komjathy,et al.  Dayside global ionospheric response to the major interplanetary events of October 29–30, 2003 “Halloween Storms” , 2005 .

[25]  W. J. Burke,et al.  Stormtime subauroral density troughs: Ion‐molecule kinetics effects , 2004 .

[26]  S. Basu,et al.  Midlatitude sub‐auroral ionospheric small scale structure during a magnetic storm , 2004 .

[27]  J. Chau,et al.  Variations of low‐latitude geomagnetic fields and Dst index caused by magnetospheric substorms , 2004 .

[28]  Philip J. Erickson,et al.  Stormtime observations of the flux of plasmaspheric ions to the dayside cusp/magnetopause , 2004 .

[29]  A. Streltsov,et al.  Electrodynamics of the magnetosphere–ionosphere coupling in the nightside subauroral zone , 2004 .

[30]  A. Streltsov,et al.  Numerical modeling of localized electromagnetic waves in the nightside subauroral zone , 2003 .

[31]  W. J. Burke,et al.  Electromagnetic wave structures within subauroral polarization streams , 2003 .

[32]  J. Foster,et al.  Average characteristics and activity dependence of the subauroral polarization stream , 2002 .

[33]  J. Ruohoniemi,et al.  Global ULF disturbances during a stormtime substorm on 25 September 1998 , 2002 .

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

[35]  Timothy Fuller-Rowell,et al.  Storm-time changes in the upper atmosphere at low latitudes , 2002 .

[36]  Philip J. Erickson,et al.  Ionospheric signatures of plasmaspheric tails , 2002 .

[37]  T. Gombosi,et al.  Interchange instability in the inner magnetosphere associated with geosynchronous particle flux decreases , 2002 .

[38]  P. Erickson,et al.  Inferred electric field variability in the polarization jet from Millstone Hill E region coherent scatter observations , 2002 .

[39]  P. Anderson,et al.  Multisatellite observations of rapid subauroral ion drifts (SAID) , 2001 .

[40]  J. Foster,et al.  Westward plasma drift in the midlatitude ionospheric F region in the midnight‐dawn sector , 2001 .

[41]  B. J. Fraser,et al.  Is the plasmapause a preferred source region of electromagnetic ion cyclotron waves in the magnetosphere , 2001 .

[42]  F. Rich,et al.  Polar cap index (PC) as a proxy for ionospheric electric field in the near‐pole region , 2000 .

[43]  Christopher T. Russell,et al.  A new functional form to study the solar wind control of the magnetopause size and shape , 1997 .

[44]  H. Hayakawa,et al.  Cross polar cap diameter and voltage as a function of PC index and interplanetary quantities , 1996 .

[45]  C. Meng,et al.  Morphology of nightside precipitation , 1996 .

[46]  M. Mendillo,et al.  Coordinated stable auroral red arc observations: Relationship to plasma convection , 1994 .

[47]  P. Anderson,et al.  A proposed production model of rapid subauroral ion drifts and their relationship to substorm evolution , 1993 .

[48]  J. Foster Storm time plasma transport at middle and high latitudes , 1993 .

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

[50]  R. Treumann,et al.  Plasma waves at the dayside magnetopause , 1988 .

[51]  M. Kelley Intense sheared flow as the origin of large‐scale undulations of the edge of the diffuse aurora , 1986 .

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

[53]  S. Quegan,et al.  The mid-latitude trough in the electron concentration of the ionospheric F-layer: a review of observations and modelling , 1983 .

[54]  R. Heelis,et al.  Rapid subauroral ion drifts observed by Atmosphere Explorer C , 1979 .

[55]  L. H. Brace,et al.  The high‐latitude winter F region at 300 km: Thermal plasma observations from AE‐C , 1978 .

[56]  H. Volland A model of the magnetospheric electric convection field , 1978 .

[57]  R. Schunk,et al.  Effects of electric fields and other processes upon the nighttime high-latitude F layer , 1976 .

[58]  J. Winningham,et al.  The latitudinal morphology of 10‐eV to 10‐keV electron fluxes during magnetically quiet and disturbed times in the 2100–0300 MLT sector , 1975 .

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

[60]  D. Stern The motion of a proton in the equatorial magnetosphere , 1975 .

[61]  W. C. Knudsen Magnetospheric convection and the high‐latitude F 2 ionosphere , 1974 .

[62]  J. Winningham,et al.  Polar cap auroral electron fluxes observed with Isis 1 , 1974 .

[63]  D. B. Muldrew,et al.  F‐layer ionization troughs deduced from Alouette data , 1965 .

[64]  J. Borovsky,et al.  A linkage between polar patches and plasmaspheric drainage plumes , 2001 .

[65]  C. Russell,et al.  Near-Earth magnetotail shape and size as determined from the magnetopause flaring angle , 1996 .

[66]  S. Quegan,et al.  The role of ion drift in the formation of ionisation troughs in the mid- and high-latitude ionosphere—a review , 1992 .

[67]  R. Schunk,et al.  Model and observation comparison of the universal time and IMF by dependence of the ionospheric polar hole , 1991 .

[68]  A. Nagy,et al.  Satellite observations of new particle and field signatures associated with SAR arc field lines at magnetospheric heights , 1987 .

[69]  Syun-Ichi Akasofu,et al.  Energy coupling between the solar wind and the magnetosphere , 1981 .

[70]  V. Ponomarev,et al.  Plasma convection in polar ionosphere , 1974 .