Spatial dependence of electromagnetic ion cyclotron waves triggered by solar wind dynamic pressure enhancements

In this paper, using the multisatellite (the Van Allen Probes and two GOES satellites) observations in the inner magnetosphere, we examine two electromagnetic ion cyclotron (EMIC) wave events that are triggered by Pdyn enhancements under prolonged northward interplanetary magnetic field quiet time preconditions. For both events, the impact of enhanced Pdyn causes EMIC waves at multiple points. However, we find a strong spatial dependence that EMIC waves due to enhanced Pdyn impact can occur at multiple points (likely globally but not necessarily everywhere) but with different wave properties. For Event 1, three satellites situated at a nearly same dawnside zone but at slightly different L shells see occurrence of EMIC waves but in different frequencies relative to local ion gyrofrequencies and with different polarizations. These waves are found inside or at the outer edge of the plasmasphere. Another satellite near noon observes no dramatic EMIC wave despite the strongest magnetic compression there. For Event 2, the four satellites are situated at widely separated magnetic local time zones when they see occurrence of EMIC waves. They are again found at different frequencies relative to local ion gyrofrequencies with different polarizations and all outside the plasmasphere. We propose two possible explanations that (i) if triggered by enhanced Pdyn impact, details of ion cyclotron instability growth can be sensitive to local plasma conditions related to background proton distributions, and (ii) there can be preexisting waves with a specific spatial distribution, which determines occurrence and specific properties of EMIC waves depending on satellite's relative position after an enhanced Pdyn arrives.

[1]  D. Baker,et al.  EMIC waves and associated relativistic electron precipitation on 25–26 January 2013 , 2016 .

[2]  R. Skoug,et al.  Van Allen Probes observations of electromagnetic ion cyclotron waves triggered by enhanced solar wind dynamic pressure , 2016 .

[3]  H. Spence,et al.  The dependence on geomagnetic conditions and solar wind dynamic pressure of the spatial distributions of EMIC waves observed by the Van Allen Probes , 2016 .

[4]  Chen Zhou,et al.  Resonant scattering of outer zone relativistic electrons by multiband EMIC waves and resultant electron loss time scales , 2015 .

[5]  D. Baker,et al.  Van Allen probes, NOAA, GOES, and ground observations of an intense EMIC wave event extending over 12 h in magnetic local time , 2015 .

[6]  Juan V. Rodriguez,et al.  Investigation of EMIC wave scattering as the cause for the BARREL 17 January 2013 relativistic electron precipitation event: A quantitative comparison of simulation with observations , 2014 .

[7]  Harlan E. Spence,et al.  Energetic, relativistic, and ultrarelativistic electrons: Comparison of long‐term VERB code simulations with Van Allen Probes measurements , 2014 .

[8]  R. Horne,et al.  Electron losses from the radiation belts caused by EMIC waves , 2014 .

[9]  L. Kistler,et al.  Simulation of Van Allen Probes plasmapause encounters , 2014 .

[10]  Zhenzhen Wang,et al.  Statistical characteristics of EMIC wave‐driven relativistic electron precipitation with observations of POES satellites: Revisit , 2014 .

[11]  M. Thomsen,et al.  In situ signatures of residual plasmaspheric plumes: Observations and simulation , 2014 .

[12]  Harlan E. Spence,et al.  Effect of EMIC waves on relativistic and ultrarelativistic electron populations: Ground‐based and Van Allen Probes observations , 2014 .

[13]  J. McCauley,et al.  The Electric Field and Waves Instruments on the Radiation Belt Storm Probes Mission , 2013 .

[14]  Daniel N. Baker,et al.  Unusual stable trapping of the ultrarelativistic electrons in the Van Allen radiation belts , 2013, Nature Physics.

[15]  Y. Xiong,et al.  Simultaneous observations of precipitating radiation belt electrons and ring current ions associated with the plasmaspheric plume , 2013 .

[16]  D. Crawford,et al.  The Electric and Magnetic Field Instrument Suite and Integrated Science (EMFISIS) on RBSP , 2013 .

[17]  R. Erlandson,et al.  Pc 1 Waves Generated by a Magnetospheric Compression During the Recovery Phase of a Geomagnetic Storm , 2013 .

[18]  C. Rodger,et al.  POES satellite observations of EMIC‐wave driven relativistic electron precipitation during 1998–2010 , 2013 .

[19]  I. Mann,et al.  Statistical analysis of EMIC waves in plasmaspheric plumes from Cluster observations , 2012 .

[20]  V. Angelopoulos,et al.  THEMIS observations of electromagnetic ion cyclotron wave occurrence: Dependence on AE, SYMH, and solar wind dynamic pressure , 2012 .

[21]  David G. Sibeck,et al.  Science Objectives and Rationale for the Radiation Belt Storm Probes Mission , 2012, Space Science Reviews.

[22]  S. Gary,et al.  Alfvén-cyclotron instability with singly ionized helium: Linear theory , 2012 .

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

[24]  J. Bortnik,et al.  The controlling effect of ion temperature on EMIC wave excitation and scattering , 2011 .

[25]  I. Mann,et al.  Warm plasma effects on electromagnetic ion cyclotron wave MeV electron interactions in the magnetosphere , 2011 .

[26]  D. Baker,et al.  Physical mechanisms of compressional EMIC wave growth , 2010 .

[27]  I. J. Rae,et al.  Conjugate ground and multisatellite observations of compression-related EMIC Pc1 waves and associated proton precipitation , 2010 .

[28]  H. Frey,et al.  Link between EMIC waves in a plasmaspheric plume and a detached sub‐auroral proton arc with observations of Cluster and IMAGE satellites , 2010 .

[29]  M. Spasojević,et al.  Temporal evolution of proton precipitation associated with the plasmaspheric plume , 2009 .

[30]  D. Baker,et al.  Modeling EMIC wave growth during the compression event of 29 June 2007 , 2009 .

[31]  Vassilis Angelopoulos,et al.  The Electric Field Instrument (EFI) for THEMIS , 2008 .

[32]  K. Shiokawa,et al.  Precipitation of radiation belt electrons by EMIC waves, observed from ground and space , 2008 .

[33]  R. Abiad,et al.  The THEMIS ESA Plasma Instrument and In-flight Calibration , 2008 .

[34]  I. J. Rae,et al.  Multipoint observations of magnetospheric compression‐related EMIC Pc1 waves by THEMIS and CARISMA , 2008 .

[35]  J. Weygand,et al.  Dynamic pressure enhancements as a cause of large‐scale stormtime substorms , 2008 .

[36]  V. Jordanova,et al.  Relativistic electron precipitation by EMIC waves from self‐consistent global simulations , 2008 .

[37]  N. Zolotukhina,et al.  Response of the inner and outer magnetosphere to solar wind density fluctuations during the recovery phase of a moderate magnetic storm , 2007 .

[38]  A. Yahnin,et al.  Energetic proton precipitation related to ion–cyclotron waves , 2007 .

[39]  P. Brandt,et al.  Energetic neutral atom response to solar wind dynamic pressure enhancements , 2007 .

[40]  J. Weygand,et al.  Reasons why some solar wind changes do not trigger substorms , 2007 .

[41]  G. Reeves,et al.  Comparison of geosynchronous energetic particle flux responses to solar wind dynamic pressure enhancements and substorms , 2005 .

[42]  S. Mende,et al.  Global auroral responses to abrupt solar wind changes: Dynamic pressure, substorm, and null events , 2005 .

[43]  C. Russell,et al.  Pc 1 waves and associated unstable distributions of magnetospheric protons observed during a solar wind pressure pulse , 2004 .

[44]  P. Anderson,et al.  Magnetospheric reconnection driven by solar wind pressure fronts , 2004 .

[45]  Richard M. Thorne,et al.  Statistical analysis of relativistic electron energies for cyclotron resonance with EMIC waves observed on CRRES , 2003 .

[46]  Richard M. Thorne,et al.  Relativistic electron pitch-angle scattering by electromagnetic ion cyclotron waves during geomagnetic storms , 2003 .

[47]  Mark B. Moldwin,et al.  Empirical plasmapause models from magnetic indices , 2003 .

[48]  Christopher T. Russell,et al.  Observations of two types of Pc 1-2 pulsations in the outer dayside magnetosphere , 2002 .

[49]  B. Anderson,et al.  Magnetic impulse events and associated Pc 1 bursts at dayside high latitudes , 1996 .

[50]  L. Yin,et al.  Electromagnetic proton cyclotron instability: Interactions with magnetospheric protons , 1995 .

[51]  B. Anderson,et al.  Electromagnetic ion cyclotron waves stimulated by modest magnetospheric compressions , 1993 .

[52]  J. Olson,et al.  Multistation correlation of ULF pulsation spectra associated with sudden impulses , 1986 .

[53]  Thomas E. Cravens,et al.  Effects of energetic heavy ions on electromagnetic ion cyclotron wave generation in the plasmapause region , 1984 .

[54]  Lou‐Chuang Lee,et al.  Pc1 wave generation by sudden impulses , 1983 .

[55]  S. Perraut,et al.  Wave‐particle interactions near ΩHe+ observed on GEOS 1 and 2 1. Propagation of ion cyclotron waves in He+‐rich plasma , 1981 .

[56]  J. Cornwall,et al.  TURBULENT LOSS OF RING-CURRENT PROTONS. , 1970 .

[57]  D. Baker,et al.  The role of Shabansky orbits in compression‐related electromagnetic ion cyclotron wave growth , 2012 .

[58]  Michelle F. Thomsen,et al.  Modeling ring current proton precipitation by electromagnetic ion cyclotron waves during the May 14–16, 1997, storm , 2001 .

[59]  C. Cocheci A statistical study of the dependence of the integrated wave power of geomagnetic pulsations between 01 Hz and 10 Hz upon the solar wind dynamic pressure , 2000 .

[60]  Charles F. Kennel,et al.  LIMIT ON STABLY TRAPPED PARTICLE FLUXES , 1966 .