The dark polar ionosphere: Progress and future challenges

Since the end of the 1970s, we have seen enormous progress in our understanding of the polar ionosphere and its structuring. With this benchmark issue of Radio Science it is appropriate to reflect briefly on that passage and some key questions that lie ahead. The discussion here will concentrate on the winter hemisphere, in keeping with the conditions under which most of the data studied to date have been gathered. The polar ionosphere alternates between two states, depending on whether the interplanetary magnetic field (IMF) is southward or northward. The former state is characterized by ∼100–1000 km islands of enhanced F region plasma, originating in sunlit upper midlatitudes, entering and traversing the polar cap. They become highly structured and produce severe scintillation. Despite much progress on the source, evolution, and ultimate fate of this polar plasma, we remain challenged by the process(es) which chop entering plasma into such islands. For northward IMF we have learned much about the near-Earth processes determining the character of polar cap arcs, velocity structure and electrodynamics, and energetics. A remaining challenge is to relate these structures to the topology and driving physical processes in the magnetosphere and solar wind. Here we sketch the principles behind the progress and the context of several key problem areas ahead.

[1]  D. Gurnett,et al.  The theta aurora , 1986 .

[2]  T. C. Moyer,et al.  Regional compositional variations of Late Tertiary bimodal rhyolite lavas across the Basin and Range/Colorado Plateau Boundary in western Arizona , 1989 .

[3]  John A. Klobuchar,et al.  Recent studies of the structure and morphology of auroral zone F region irregularities , 1983 .

[4]  R. G. Musgrove,et al.  Ionospheric convection associated with discrete levels of particle precipitation , 1986 .

[5]  P. Fougere,et al.  Simultaneous density and electric field fluctuation spectra associated with velocity shears in the auroral oval , 1988 .

[6]  J. Heppner Empirical models of high latitude electric fields , 1977 .

[7]  M. Gussenhoven Extremely high latitude auroras , 1982 .

[8]  Paul F. Fougere,et al.  Velocity shears and sub‐km scale irregularities in the nighttime auroral F‐region , 1986 .

[9]  H. Carlson,et al.  Thermal response of the F region ionosphere in artificial modification experiments by HF radio waves , 1981 .

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

[11]  J. V. Evans,et al.  Millstone hill incoherent scatter observations of auroral convection over 60° ≤Λ ≤75° 2. Initial results , 1980 .

[12]  N. Maynard,et al.  Empirical high‐latitude electric field models , 1987 .

[13]  H. Carlson,et al.  Coherent mesoscale convection patterns during northward interplanetary magnetic field , 1988 .

[14]  S. Basu,et al.  Irregularity structures in the cusp/cleft and polar cap regions , 1994 .

[15]  Tsunoda,et al.  High-latitude F-region irregularities: a review and synthesis. Technical report, 1 January 1986-1 July 1987 , 1988 .

[16]  R. Livingston,et al.  Polar cap F layer patches: Structure and dynamics , 1986 .

[17]  Jules Aarons,et al.  UHF scintillation activity over polar latitudes , 1981 .

[18]  L. Cogger,et al.  Characteristics of polar cap Sun‐aligned arcs , 1977 .

[19]  E. J. Weber,et al.  Polar cap F‐layer auroras , 1981 .

[20]  R. Heelis,et al.  Origin of density enhancements in the winter polar cap ionosphere , 1988 .

[21]  R. W. Spiro,et al.  A model of the high‐latitude ionospheric convection pattern , 1982 .

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

[23]  S. Zalesak,et al.  Nonlinear evolution of the Kelvin-Helmholtz instability in the high-latitude ionosphere. Interim report , 1987 .

[24]  T. Killeen,et al.  Thermosphere dynamics: Contributions from the first 5 years of the Dynamics Explorer Program , 1988 .

[25]  R. Schunk,et al.  A comparison of model predictions for plasma convection in the northern and southern polar regions , 1980 .

[26]  H. Carlson,et al.  The electrodynamic, thermal, and energetic character of intense Sun-aligned arcs in the polar cap , 1991 .

[27]  H. Carlson,et al.  Production of polar cap electron density patches by transient magnetopause reconnection , 1992 .

[28]  S. Basu,et al.  Plasma structuring by the gradient drift instability at high latitudes and comparison with velocity shear driven processes , 1990 .

[29]  Bodo W. Reinisch,et al.  F layer ionization patches in the polar cap , 1983 .

[30]  W. J. Burke,et al.  Electric and magnetic field characteristics of discrete arcs in the polar cap , 1982 .

[31]  Emanoel Costa,et al.  250 MHz/GHz Scintillation Parameters in the Equatorial, Polar, and Auroral Environments , 1986, IEEE J. Sel. Areas Commun..

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

[33]  H. Carlson Dynamics of the quiet polar cap. , 1990 .

[34]  R. Robinson,et al.  Sources of F region ionization enhancements in the nighttime auroral zone , 1985 .

[35]  R. Sheehan,et al.  Coordinated measurements of auroral zone plasma enhancements , 1985 .

[36]  R. Heelis The effects of interplanetary magnetic field orientation on dayside high‐latitude ionospheric convection , 1984 .

[37]  Charles L Rino,et al.  Chatanika/Triad observations of unstable ionization enhancements in the auroral F‐region , 1980 .