Modelling of optical emissions enhanced by the HF pumping of the ionospheric F-region

Strong enhancement of the optical emissions with excitation threshold from 1.96 eV (630.0 nm from O( 1 D)) up to 18.75 eV (427.8 nm from N 2 + (1NG)) have been observed during experiments of the ionosphere modification by high power HF radio waves. Analysis of the optical emission ratios showed clea...

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Published in:Annales Geophysicae
Main Authors: Sergienko, T., Gustavsson, B., Brändström, U., Axelsson, K.
Format: Text
Language:English
Published: 2018
Subjects:
Online Access:https://doi.org/10.5194/angeo-30-885-2012
https://angeo.copernicus.org/articles/30/885/2012/
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spelling ftcopernicus:oai:publications.copernicus.org:angeo13960 2023-05-15T16:04:47+02:00 Modelling of optical emissions enhanced by the HF pumping of the ionospheric F-region Sergienko, T. Gustavsson, B. Brändström, U. Axelsson, K. 2018-09-27 application/pdf https://doi.org/10.5194/angeo-30-885-2012 https://angeo.copernicus.org/articles/30/885/2012/ eng eng doi:10.5194/angeo-30-885-2012 https://angeo.copernicus.org/articles/30/885/2012/ eISSN: 1432-0576 Text 2018 ftcopernicus https://doi.org/10.5194/angeo-30-885-2012 2020-07-20T16:25:48Z Strong enhancement of the optical emissions with excitation threshold from 1.96 eV (630.0 nm from O( 1 D)) up to 18.75 eV (427.8 nm from N 2 + (1NG)) have been observed during experiments of the ionosphere modification by high power HF radio waves. Analysis of the optical emission ratios showed clearly that a significant part of the ionospheric electrons have to be accelerated to energies above 30 eV and more in the region where the HF radio wave effectively interacts with the ionospheric plasma. The Monte-Carlo model of electron transport and the optical emission model were used to study the dependence of the optical emission intensity on the acceleration electron parameters. We obtained the following results from analysis of the enhanced intensities of the four optical emissions (630.0, 557.7, 844.6 and 427.8 nm) observed in the EISCAT heating experiment on 10 March 2002. The 630.0 emission with an excitation threshold of 1.96 eV is formed predominately by the thermal electrons, where the accelerated electrons play a minor role in the excitation of this emission. In order to explain the experimentally observed intensity ratios, the accelerated electrons must gain energies of more than 60 eV. For accelerated electrons with a power law energy dependence, the efficiency of the optical emission excitation depends on the exponent defining the shape of the electron spectra. However, an agreement with the observed emission intensities is achieved for exponent values not less than zero. Moreover, increasing the exponent to higher values does not affect the emission intensity ratios. Text EISCAT Copernicus Publications: E-Journals Annales Geophysicae 30 5 885 895
institution Open Polar
collection Copernicus Publications: E-Journals
op_collection_id ftcopernicus
language English
description Strong enhancement of the optical emissions with excitation threshold from 1.96 eV (630.0 nm from O( 1 D)) up to 18.75 eV (427.8 nm from N 2 + (1NG)) have been observed during experiments of the ionosphere modification by high power HF radio waves. Analysis of the optical emission ratios showed clearly that a significant part of the ionospheric electrons have to be accelerated to energies above 30 eV and more in the region where the HF radio wave effectively interacts with the ionospheric plasma. The Monte-Carlo model of electron transport and the optical emission model were used to study the dependence of the optical emission intensity on the acceleration electron parameters. We obtained the following results from analysis of the enhanced intensities of the four optical emissions (630.0, 557.7, 844.6 and 427.8 nm) observed in the EISCAT heating experiment on 10 March 2002. The 630.0 emission with an excitation threshold of 1.96 eV is formed predominately by the thermal electrons, where the accelerated electrons play a minor role in the excitation of this emission. In order to explain the experimentally observed intensity ratios, the accelerated electrons must gain energies of more than 60 eV. For accelerated electrons with a power law energy dependence, the efficiency of the optical emission excitation depends on the exponent defining the shape of the electron spectra. However, an agreement with the observed emission intensities is achieved for exponent values not less than zero. Moreover, increasing the exponent to higher values does not affect the emission intensity ratios.
format Text
author Sergienko, T.
Gustavsson, B.
Brändström, U.
Axelsson, K.
spellingShingle Sergienko, T.
Gustavsson, B.
Brändström, U.
Axelsson, K.
Modelling of optical emissions enhanced by the HF pumping of the ionospheric F-region
author_facet Sergienko, T.
Gustavsson, B.
Brändström, U.
Axelsson, K.
author_sort Sergienko, T.
title Modelling of optical emissions enhanced by the HF pumping of the ionospheric F-region
title_short Modelling of optical emissions enhanced by the HF pumping of the ionospheric F-region
title_full Modelling of optical emissions enhanced by the HF pumping of the ionospheric F-region
title_fullStr Modelling of optical emissions enhanced by the HF pumping of the ionospheric F-region
title_full_unstemmed Modelling of optical emissions enhanced by the HF pumping of the ionospheric F-region
title_sort modelling of optical emissions enhanced by the hf pumping of the ionospheric f-region
publishDate 2018
url https://doi.org/10.5194/angeo-30-885-2012
https://angeo.copernicus.org/articles/30/885/2012/
genre EISCAT
genre_facet EISCAT
op_source eISSN: 1432-0576
op_relation doi:10.5194/angeo-30-885-2012
https://angeo.copernicus.org/articles/30/885/2012/
op_doi https://doi.org/10.5194/angeo-30-885-2012
container_title Annales Geophysicae
container_volume 30
container_issue 5
container_start_page 885
op_container_end_page 895
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