Radar imaging with EISCAT 3D

A new incoherent scatter radar called EISCAT 3D is being constructed in northern Scandinavia. It will have the capability to produce volumetric images of ionospheric plasma parameters using aperture synthesis radar imaging. This study uses the current design of EISCAT 3D to explore the theoretical r...

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Published in:Annales Geophysicae
Main Authors: J. Stamm, J. Vierinen, J. M. Urco, B. Gustavsson, J. L. Chau
Format: Article in Journal/Newspaper
Language:English
Published: Copernicus Publications 2021
Subjects:
Online Access:https://doi.org/10.5194/angeo-39-119-2021
https://doaj.org/article/7f9b99eb24e4460392572606bfcc67f5
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author J. Stamm
J. Vierinen
J. M. Urco
B. Gustavsson
J. L. Chau
author_facet J. Stamm
J. Vierinen
J. M. Urco
B. Gustavsson
J. L. Chau
author_sort J. Stamm
collection Directory of Open Access Journals: DOAJ Articles
container_issue 1
container_start_page 119
container_title Annales Geophysicae
container_volume 39
description A new incoherent scatter radar called EISCAT 3D is being constructed in northern Scandinavia. It will have the capability to produce volumetric images of ionospheric plasma parameters using aperture synthesis radar imaging. This study uses the current design of EISCAT 3D to explore the theoretical radar imaging performance when imaging electron density in the E region and compares numerical techniques that could be used in practice. Of all imaging algorithms surveyed, the singular value decomposition with regularization gave the best results and was also found to be the most computationally efficient. The estimated imaging performance indicates that the radar will be capable of detecting features down to approximately 90×90 m at a height of 100 km , which corresponds to a <math xmlns="http://www.w3.org/1998/Math/MathML" id="M4" display="inline" overflow="scroll" dspmath="mathml"><mrow><mo>≈</mo><mn mathvariant="normal">0.05</mn><msup><mi/><mo>∘</mo></msup></mrow></math> <svg:svg xmlns:svg="http://www.w3.org/2000/svg" width="38pt" height="11pt" class="svg-formula" dspmath="mathimg" md5hash="7b2ab9850ba1c59fd035d756f43deafe"><svg:image xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="angeo-39-119-2021-ie00001.svg" width="38pt" height="11pt" src="angeo-39-119-2021-ie00001.png"/></svg:svg> angular resolution. The temporal resolution is dependent on the signal-to-noise ratio and range resolution. The signal-to-noise ratio calculations indicate that high-resolution imaging of auroral precipitation is feasible. For example, with a range resolution of 1500 m , a time resolution of 10 s, and an electron density of <math xmlns="http://www.w3.org/1998/Math/MathML" id="M6" display="inline" overflow="scroll" dspmath="mathml"><mrow><mn mathvariant="normal">2</mn><mo>×</mo><msup><mn mathvariant="normal">10</mn><mn ...
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spelling ftdoajarticles:oai:doaj.org/article:7f9b99eb24e4460392572606bfcc67f5 2025-01-16T21:42:00+00:00 Radar imaging with EISCAT 3D J. Stamm J. Vierinen J. M. Urco B. Gustavsson J. L. Chau 2021-02-01T00:00:00Z https://doi.org/10.5194/angeo-39-119-2021 https://doaj.org/article/7f9b99eb24e4460392572606bfcc67f5 EN eng Copernicus Publications https://angeo.copernicus.org/articles/39/119/2021/angeo-39-119-2021.pdf https://doaj.org/toc/0992-7689 https://doaj.org/toc/1432-0576 doi:10.5194/angeo-39-119-2021 0992-7689 1432-0576 https://doaj.org/article/7f9b99eb24e4460392572606bfcc67f5 Annales Geophysicae, Vol 39, Pp 119-134 (2021) Science Q Physics QC1-999 Geophysics. Cosmic physics QC801-809 article 2021 ftdoajarticles https://doi.org/10.5194/angeo-39-119-2021 2022-12-31T07:34:04Z A new incoherent scatter radar called EISCAT 3D is being constructed in northern Scandinavia. It will have the capability to produce volumetric images of ionospheric plasma parameters using aperture synthesis radar imaging. This study uses the current design of EISCAT 3D to explore the theoretical radar imaging performance when imaging electron density in the E region and compares numerical techniques that could be used in practice. Of all imaging algorithms surveyed, the singular value decomposition with regularization gave the best results and was also found to be the most computationally efficient. The estimated imaging performance indicates that the radar will be capable of detecting features down to approximately 90×90 m at a height of 100 km , which corresponds to a <math xmlns="http://www.w3.org/1998/Math/MathML" id="M4" display="inline" overflow="scroll" dspmath="mathml"><mrow><mo>≈</mo><mn mathvariant="normal">0.05</mn><msup><mi/><mo>∘</mo></msup></mrow></math> <svg:svg xmlns:svg="http://www.w3.org/2000/svg" width="38pt" height="11pt" class="svg-formula" dspmath="mathimg" md5hash="7b2ab9850ba1c59fd035d756f43deafe"><svg:image xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="angeo-39-119-2021-ie00001.svg" width="38pt" height="11pt" src="angeo-39-119-2021-ie00001.png"/></svg:svg> angular resolution. The temporal resolution is dependent on the signal-to-noise ratio and range resolution. The signal-to-noise ratio calculations indicate that high-resolution imaging of auroral precipitation is feasible. For example, with a range resolution of 1500 m , a time resolution of 10 s, and an electron density of <math xmlns="http://www.w3.org/1998/Math/MathML" id="M6" display="inline" overflow="scroll" dspmath="mathml"><mrow><mn mathvariant="normal">2</mn><mo>×</mo><msup><mn mathvariant="normal">10</mn><mn ... Article in Journal/Newspaper EISCAT Directory of Open Access Journals: DOAJ Articles Annales Geophysicae 39 1 119 134
spellingShingle Science
Q
Physics
QC1-999
Geophysics. Cosmic physics
QC801-809
J. Stamm
J. Vierinen
J. M. Urco
B. Gustavsson
J. L. Chau
Radar imaging with EISCAT 3D
title Radar imaging with EISCAT 3D
title_full Radar imaging with EISCAT 3D
title_fullStr Radar imaging with EISCAT 3D
title_full_unstemmed Radar imaging with EISCAT 3D
title_short Radar imaging with EISCAT 3D
title_sort radar imaging with eiscat 3d
topic Science
Q
Physics
QC1-999
Geophysics. Cosmic physics
QC801-809
topic_facet Science
Q
Physics
QC1-999
Geophysics. Cosmic physics
QC801-809
url https://doi.org/10.5194/angeo-39-119-2021
https://doaj.org/article/7f9b99eb24e4460392572606bfcc67f5