Complexity in the high latitude HF radar spectral width boundary region

SuperDARN radars are sensitive to the collective Doppler characteristics of decametre-scale irregularities in the high latitude ionosphere. The radars routinely observe a distinct transition from large spectral width (&gt;100 m s<sup>&minus;1</sup>) located at higher latitudes...

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Main Authors: M. L. Parkinson, K. M. Hannah, P. L. Dyson
Format: Article
Language:English
Published: Copernicus Publications 2008-05-01
Series:Annales Geophysicae
Online Access:https://www.ann-geophys.net/26/877/2008/angeo-26-877-2008.pdf
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author M. L. Parkinson
K. M. Hannah
P. L. Dyson
author_facet M. L. Parkinson
K. M. Hannah
P. L. Dyson
author_sort M. L. Parkinson
collection DOAJ
description SuperDARN radars are sensitive to the collective Doppler characteristics of decametre-scale irregularities in the high latitude ionosphere. The radars routinely observe a distinct transition from large spectral width (&gt;100 m s<sup>&minus;1</sup>) located at higher latitudes to low spectral width (&lt;50 m s<sup>&minus;1</sup>) located at lower latitudes. Because of its equatorward location, the TIGER Tasmanian radar is very sensitive to the detection of the spectral width boundary (SWB) in the nightside auroral ionosphere. An analysis of the line-of-sight velocities and 2-D beam-swinging vectors suggests the meso-scale (~100 km) convection is more erratic in the high spectral width region, but slower and more homogeneous in the low spectral width region. The radar autocorrelation functions are better modelled using Lorentzian Doppler spectra in the high spectral width region, and Gaussian Doppler spectra in the low spectral width region. However, paradoxically, Gaussian Doppler spectra are associated with the largest spectral widths. Application of the Burg maximum entropy method suggests the occurrence of double-peaked Doppler spectra is greater in the high spectral width region, implying the small-scale (~10 km) velocity fluctuations are more intense above the SWB. These observations combined with collective wave scattering theory imply there is a transition from a fast flowing, turbulent plasma with a correlation length of velocity fluctuations less than the scattering wavelength, to a slower moving plasma with a correlation length greater than the scattering wavelength. Peak scaling and structure function analysis of fluctuations in the SWB itself reveals approximately scale-free behaviour across temporal scales of ~10 s to ~34 min. Preliminary scaling exponents for these fluctuations, &alpha;<sub>GSF</sub>=0.18&plusmn;0.02 and &alpha;<sub>GSF</sub>=0.09&plusmn;0.01, are even smaller than that expected for MHD turbulence.
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spelling doaj.art-6870eb4f1d4245f289333298a66e38232022-12-21T19:45:38ZengCopernicus PublicationsAnnales Geophysicae0992-76891432-05762008-05-012687789210.5194/angeo-26-877-2008Complexity in the high latitude HF radar spectral width boundary regionM. L. Parkinson0K. M. Hannah1P. L. Dyson2Department of Physics, La Trobe University, Victoria 3086, AustraliaDepartment of Physics, La Trobe University, Victoria 3086, AustraliaDepartment of Physics, La Trobe University, Victoria 3086, AustraliaSuperDARN radars are sensitive to the collective Doppler characteristics of decametre-scale irregularities in the high latitude ionosphere. The radars routinely observe a distinct transition from large spectral width (&gt;100 m s<sup>&minus;1</sup>) located at higher latitudes to low spectral width (&lt;50 m s<sup>&minus;1</sup>) located at lower latitudes. Because of its equatorward location, the TIGER Tasmanian radar is very sensitive to the detection of the spectral width boundary (SWB) in the nightside auroral ionosphere. An analysis of the line-of-sight velocities and 2-D beam-swinging vectors suggests the meso-scale (~100 km) convection is more erratic in the high spectral width region, but slower and more homogeneous in the low spectral width region. The radar autocorrelation functions are better modelled using Lorentzian Doppler spectra in the high spectral width region, and Gaussian Doppler spectra in the low spectral width region. However, paradoxically, Gaussian Doppler spectra are associated with the largest spectral widths. Application of the Burg maximum entropy method suggests the occurrence of double-peaked Doppler spectra is greater in the high spectral width region, implying the small-scale (~10 km) velocity fluctuations are more intense above the SWB. These observations combined with collective wave scattering theory imply there is a transition from a fast flowing, turbulent plasma with a correlation length of velocity fluctuations less than the scattering wavelength, to a slower moving plasma with a correlation length greater than the scattering wavelength. Peak scaling and structure function analysis of fluctuations in the SWB itself reveals approximately scale-free behaviour across temporal scales of ~10 s to ~34 min. Preliminary scaling exponents for these fluctuations, &alpha;<sub>GSF</sub>=0.18&plusmn;0.02 and &alpha;<sub>GSF</sub>=0.09&plusmn;0.01, are even smaller than that expected for MHD turbulence.https://www.ann-geophys.net/26/877/2008/angeo-26-877-2008.pdf
spellingShingle M. L. Parkinson
K. M. Hannah
P. L. Dyson
Complexity in the high latitude HF radar spectral width boundary region
Annales Geophysicae
title Complexity in the high latitude HF radar spectral width boundary region
title_full Complexity in the high latitude HF radar spectral width boundary region
title_fullStr Complexity in the high latitude HF radar spectral width boundary region
title_full_unstemmed Complexity in the high latitude HF radar spectral width boundary region
title_short Complexity in the high latitude HF radar spectral width boundary region
title_sort complexity in the high latitude hf radar spectral width boundary region
url https://www.ann-geophys.net/26/877/2008/angeo-26-877-2008.pdf
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