Deriving Global Convection Maps From SuperDARN Measurements

A new statistical modeling technique for determining the global ionospheric convection is described. The Principal Component Regression (PCR) based technique is based on SuperDARN observations and is an advanced version of the principal component regression technique that Waters et al. [2015] used for the SuperMAG data. While SuperMAG ground magnetic field perturbations are vector measurements, SuperDARN provides line-of-sight (LOS) measurements of the ionospheric convection flow. Each LOS flow has a known azimuth (or direction) which must be converted into the actual vector flow. However, the component perpendicular to the azimuth direction is unknown. Our method uses historical data from the SuperDARN data base and Principal Component Regression to determine a fill-in model convection distribution for any given Universal Time (UT). The fill-in data process is driven by a list of state descriptors (magnetic indices and the solar zenith angle). The final solution is then derived from a spherical cap harmonic fit to the SuperDARN measurements and the fill-in model. When compared with the standard SuperDARN fill-in model we find that our fill-in model provides improved solutions, and the final solutions are in better agreement with the SuperDARN measurements. Our solutions are far less dynamic than the standard SuperDARN solutions which we interpret as being due to a lack of Magnetosphere-Ionosphere inertia and communication delays in the standard SuperDARN technique while it is inherently included in our approach. Rather, we argue that the magnetosphere-ionosphere system has inertia that prevents the global convection from changing abruptly in response to an IMF change.

[1]  Shireen D. Geimer,et al.  Ultralow-frequency magnetohydrodynamics in boundary-constrained geomagnetic flux coordinates , 2002 .

[2]  G. V. Haines,et al.  Spherical cap harmonic analysis of Super Dual Auroral Radar Network (SuperDARN) observations for generating maps of ionospheric convection , 2010 .

[3]  J. Ruohoniemi,et al.  Electrostatic potential patterns in the high‐latitude ionosphere constrained by SuperDARN measurements , 2000 .

[4]  R. Greenwald,et al.  An HF phased‐array radar for studying small‐scale structure in the high‐latitude ionosphere , 1985 .

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

[6]  S. Wing,et al.  A new magnetic coordinate system for conjugate studies at high latitudes , 1989 .

[7]  Raymond A. Greenwald,et al.  Dependencies of high-latitude plasma convection: Consideration of interplanetary magnetic field, seasonal, and universal time factors in statistical patterns , 2005 .

[8]  J. Gjerloev,et al.  Global maps of ground magnetometer data , 2015 .

[9]  R. Hoffman,et al.  Response of the auroral electrojet indices to abrupt southward IMF turnings , 2010 .

[10]  Robert L. Lysak,et al.  Magnetosphere-ionosphere coupling by Alfvén waves at midlatitudes , 2004 .

[11]  J. M. Ruohoniemi,et al.  Ionospheric response to the interplanetary magnetic field southward turning: Fast onset and slow reconfiguration , 2002 .

[12]  J. Ruohoniemi,et al.  Principal component analysis of polar cap convection , 2012 .

[13]  C. Waters,et al.  Field line resonant frequencies and ionospheric conductance: Results from a 2‐D MHD model , 2008 .

[14]  J. M. Ruohoniemi,et al.  Large-scale imaging of high-latitude convection with Super Dual Auroral Radar Network HF radar observations , 1998 .

[15]  K. Kabin,et al.  Field-line resonances in arbitrary magnetic field topology , 2004 .

[16]  P. Newell,et al.  SuperMAG‐based partial ring current indices , 2012 .

[17]  Adrian Grocott,et al.  A quantitative deconstruction of the morphology of high-latitude ionospheric convection , 2012 .

[18]  Peter. Dyson,et al.  A decade of the Super Dual Auroral Radar Network (SuperDARN): scientific achievements, new techniques and future directions , 2007 .

[19]  Raymond A. Greenwald,et al.  Statistical patterns of high‐latitude convection obtained from Goose Bay HF radar observations , 1996 .

[20]  Colin L. Waters,et al.  Spectral width of SuperDARN echoes: measurement, use and physical interpretation , 2006 .

[21]  D. Marquardt An Algorithm for Least-Squares Estimation of Nonlinear Parameters , 1963 .

[22]  G. V. Haines Spherical cap harmonic analysis , 1985 .

[23]  Jesper Gjerloev,et al.  The SuperMAG data processing technique , 2012 .

[24]  Raymond A. Greenwald,et al.  Observations of IMF and seasonal effects in high‐latitude convection , 1995 .

[25]  Simon George Shepherd,et al.  A dynamical model of high‐latitude convection derived from SuperDARN plasma drift measurements , 2010 .

[26]  Tomoko Matsuo,et al.  Mesoscale and large‐scale variability in high‐latitude ionospheric convection: Dominant modes and spatial/temporal coherence , 2013 .

[27]  F. Menk,et al.  Factors determining spectral width of HF echoes from high latitudes , 2007 .