Multipoint Observations of Dispersive Scale Alfvénic Field‐Line Resonances Associated With Substorm Auroral Beads

We present a case study of the field‐aligned current (FAC) systems that transpire within the high‐altitude auroral acceleration region of an “auroral bead” initiated double oval substorm observed on 23 February 2001 by the Cluster fleet. Conjunctive Cluster measurements and auroral images from IMAGE reveal that auroral bead current system formation and evolution is a multi‐scale, injection‐mediated process. The FACs at large scales vary on substorm evolution time scales (∼minutes) in response to the injection and evolution of hotter denser magnetospheric plasma. Embedded within the large‐scale FACs are intense short‐scale (≲ few 10s of km) currents comprising dispersive scale Alfvén wave (DAW) fluctuations. The DAWs are a complex mixture of ingoing and reflected components that regularly interfere to form a broad spectrum of kinetic (dispersive) scale Alfvénic field‐line resonances (KFLRs). The Alfvénic currents appear as a nested series of upward and downward FAC densities with amplitudes reaching a few 100 nA/m2. Energized field‐aligned or counterstreaming electrons near keV energies and below are observed with parallel skews that vary in concert with variations in the DAW current sense. Positive correlations between DAW electric field energy densities and the energies of energized H+, He+, and O+ outflow are observed, indicative of ion energization within the DAW fields. Due to their L‐shell location (L ∼5.8–7.0) and associations with injections, the KFLRs are interpreted as the high‐altitude auroral zone analog of KFLRs observed in the equatorial inner magnetosphere.

[1]  G. Reeves,et al.  Correlations Between Dispersive Alfvén Wave Activity, Electron Energization, and Ion Outflow in the Inner Magnetosphere , 2020, Geophysical Research Letters.

[2]  G. Reeves,et al.  Dispersive Alfvén Wave Control of O+ Ion Outflow and Energy Densities in the Inner Magnetosphere , 2019, Geophysical Research Letters.

[3]  J. G. Sample,et al.  The Space Physics Environment Data Analysis System (SPEDAS) , 2019, Space Science Reviews.

[4]  I. J. Rae,et al.  A diagnosis of the plasma waves responsible for the explosive energy release of substorm onset , 2018, Nature Communications.

[5]  C. Chaston,et al.  Electron Distributions in Kinetic Scale Field Line Resonances: A Comparison of Simulations and Observations , 2018, Geophysical Research Letters.

[6]  N. Kalmoni The role of magnetospheric plasma instabilities in auroral and substorm dynamics , 2017 .

[7]  I. J. Rae,et al.  Statistical azimuthal structuring of the substorm onset arc: Implications for the onset mechanism , 2017 .

[8]  V. Angelopoulos,et al.  Statistical properties of substorm auroral onset beads/rays , 2016 .

[9]  G. Reeves,et al.  Driving ionospheric outflows and magnetospheric O+ energy density with Alfvén waves , 2016 .

[10]  H. Frey,et al.  The “Alfvénic surge” at substorm onset/expansion and the formation of “Inverted Vs”: Cluster and IMAGE observations , 2016 .

[11]  I. J. Rae,et al.  Statistical characterization of the growth and spatial scales of the substorm onset arc , 2015, Journal of geophysical research. Space physics.

[12]  V. Angelopoulos,et al.  Ionospheric flow structures associated with auroral beading at substorm auroral onset , 2014 .

[13]  I. J. Rae,et al.  In situ spatiotemporal measurements of the detailed azimuthal substructure of the substorm current wedge , 2014, Journal of geophysical research. Space physics.

[14]  F. Mozer,et al.  Observations of kinetic scale field line resonances , 2014 .

[15]  P. Lindqvist,et al.  Cluster multipoint study of the acceleration potential pattern and electrodynamics of an auroral surge and its associated horn arc , 2012 .

[16]  P. Damiano,et al.  Electron acceleration in a geomagnetic Field Line Resonance , 2012 .

[17]  Jesper Gjerloev,et al.  Evaluation of SuperMAG auroral electrojet indices as indicators of substorms and auroral power , 2011 .

[18]  V. Angelopoulos,et al.  Substorm triggering by poleward boundary intensification and related equatorward propagation , 2011 .

[19]  P. Lindqvist,et al.  Evolution in space and time of the quasi‐static acceleration potential of inverted‐V aurora and its interaction with Alfvénic boundary processes , 2011 .

[20]  F. Mozer,et al.  Time development of field‐aligned currents, potential drops, and plasma associated with an auroral poleward boundary intensification , 2010 .

[21]  C. Escoubet,et al.  Cluster Active Archive: Overview , 2010 .

[22]  Harri Laakso,et al.  The Cluster active archive : studying the Earth's space plasma environment , 2010 .

[23]  V. Angelopoulos,et al.  Equatorward moving auroral signatures of a flow burst observed prior to auroral onset , 2009 .

[24]  V. Angelopoulos,et al.  Reply to comment by Harald U. Frey on “Substorm triggering by new plasma intrusion: THEMIS all‐sky imager observations” , 2009 .

[25]  I. J. Rae,et al.  Near‐Earth initiation of a terrestrial substorm , 2009 .

[26]  M. Henderson Observational evidence for an inside-out substorm onset scenario , 2009 .

[27]  V. Angelopoulos,et al.  Intensification of preexisting auroral arc at substorm expansion phase onset: Wave‐like disruption during the first tens of seconds , 2008 .

[28]  I. Dandouras,et al.  EISCAT and Cluster observations in the vicinity of the dynamical polar cap boundary , 2008 .

[29]  Martin Connors,et al.  The THEMIS all-sky imaging array—system design and initial results from the prototype imager , 2006 .

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

[31]  R. Ergun,et al.  Auroral ion acceleration in dispersive Alfvén waves , 2004 .

[32]  C. Chaston Reply to “Comment by P. K. Shukla and L. Stenflo on ‘Kinetic effects in the acceleration of auroral electrons in small scale Alfvén waves: A FAST case study’” , 2004 .

[33]  N. Østgaard,et al.  FAST and IMAGE-FUV observations of a substorm onset , 2003 .

[34]  R. Ergun,et al.  Kinetic effects in the acceleration of auroral electrons in small scale Alfven waves: A FAST case study , 2003 .

[35]  J. Sauvaud,et al.  Motion of auroral ion outflow structures observed with CLUSTER and IMAGE FUV , 2002 .

[36]  David Rudrauf,et al.  Estimating the time-course of coherence between single-trial brain signals: an introduction to wavelet coherence , 2002, Neurophysiologie Clinique/Clinical Neurophysiology.

[37]  R. Treumann,et al.  Auroral Plasma Physics , 2002 .

[38]  J. Johnson,et al.  Stochastic ion heating at the magnetopause due to kinetic Alfvén waves , 2001 .

[39]  Etienne Renotte,et al.  Far ultraviolet imaging from the IMAGE spacecraft. 1. System design , 2000 .

[40]  P. Webster,et al.  Interdecadal changes in the ENSO-monsoon system , 1999 .

[41]  R. Elphic,et al.  Species dependent energies in upward directed ion beams over auroral arcs as observed with FAST TEAMS , 1998 .

[42]  P. Daly,et al.  Analysis methods for multi-spacecraft data , 1998 .

[43]  C. Torrence,et al.  A Practical Guide to Wavelet Analysis. , 1998 .

[44]  Mario H. Acuna,et al.  THE CLUSTER MAGNETIC FIELD INVESTIGATION , 1997 .

[45]  J. M. Nappa,et al.  The Cluster Spatio-Temporal Analysis of Field Fluctuations (STAFF) Experiment , 1997 .

[46]  J. Rouzaud,et al.  THE CLUSTER ION SPECTROMETRY (CIS) EXPERIMENT , 1997 .

[47]  Manuel Grande,et al.  PEACE: A PLASMA ELECTRON AND CURRENT EXPERIMENT , 1997 .

[48]  Per-Arne Lindqvist,et al.  THE ELECTRIC FIELD AND WAVE EXPERIMENT FOR THE CLUSTER MISSION , 1997 .

[49]  G. Guo,et al.  Reply to the comment , 1997, quant-ph/9710014.

[50]  D. Klumpar,et al.  Observations in the vicinity of substorm onset: Implications for the substorm process , 1995 .

[51]  R. Hoffman,et al.  Characteristics of the field-aligned current system in the nighttime sector during auroral substorms , 1994 .

[52]  P. Anderson,et al.  Electrodynamic parameters in the nighttime sector during auroral substorms , 1994 .

[53]  W. I. Axford,et al.  RAPID – The Imaging Energetic Particle Spectrometer on Cluster , 1993 .

[54]  K. Cole Effects of crossed magnetic and (spatially dependent) electric fields on charged particle motion , 1976 .

[55]  G. Lothian,et al.  Spectral Analysis , 1971, Nature.