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B2 Thickness Parameter Response to Equinoctial Geomagnetic Storms

The thickness parameters that most empirical models use are generally defined by empirical relations related to ionogram characteristics. This is the case with the NeQuick model that uses an inflection point below the F2 layer peak to define a thickness parameter of the F2 bottomside of the electron...

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Autores principales: Migoya-Orué, Yenca, Alazo-Cuartas, Katy, Kashcheyev, Anton, Amory-Mazaudier, Christine, Radicella, Sandro, Nava, Bruno, Fleury, Rolland, Ezquer, Rodolfo
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8588179/
https://www.ncbi.nlm.nih.gov/pubmed/34770676
http://dx.doi.org/10.3390/s21217369
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author Migoya-Orué, Yenca
Alazo-Cuartas, Katy
Kashcheyev, Anton
Amory-Mazaudier, Christine
Radicella, Sandro
Nava, Bruno
Fleury, Rolland
Ezquer, Rodolfo
author_facet Migoya-Orué, Yenca
Alazo-Cuartas, Katy
Kashcheyev, Anton
Amory-Mazaudier, Christine
Radicella, Sandro
Nava, Bruno
Fleury, Rolland
Ezquer, Rodolfo
author_sort Migoya-Orué, Yenca
collection PubMed
description The thickness parameters that most empirical models use are generally defined by empirical relations related to ionogram characteristics. This is the case with the NeQuick model that uses an inflection point below the F2 layer peak to define a thickness parameter of the F2 bottomside of the electron density profile, which is named B2. This study is focused on the effects of geomagnetic storms on the thickness parameter B2. We selected three equinoctial storms, namely 17 March 2013, 2 October 2013 and 17 March 2015. To investigate the behavior of the B2 parameter before, during and after those events, we have analyzed variations of GNSS derived vertical TEC (VTEC) and maximum electron density (NmF2) obtained from manually scaled ionograms over 20 stations at middle and low latitudes of Asian, Euro-African and American longitude sectors. The results show two main kinds of responses after the onset of the geomagnetic events: a peak of B2 parameter prior to the increase in VTEC and NmF2 (in ~60% of the cases) and a fluctuation in B2 associated with a decrease in VTEC and NmF2 (~25% of the cases). The behavior observed has been related to the dominant factor acting after the CME shocks associated with positive and negative storm effects. Investigation into the time delay of the different measurements according to location showed that B2 reacts before NmF2 and VTEC after the onset of the storms in all the cases. The sensitivity shown by B2 during the studied storms might indicate that experimentally derived thickness parameter B2 could be incorporated into the empirical models such as NeQuick in order to adapt them to storm situations that represent extreme cases of ionospheric weather-like conditions.
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spelling pubmed-85881792021-11-13 B2 Thickness Parameter Response to Equinoctial Geomagnetic Storms Migoya-Orué, Yenca Alazo-Cuartas, Katy Kashcheyev, Anton Amory-Mazaudier, Christine Radicella, Sandro Nava, Bruno Fleury, Rolland Ezquer, Rodolfo Sensors (Basel) Article The thickness parameters that most empirical models use are generally defined by empirical relations related to ionogram characteristics. This is the case with the NeQuick model that uses an inflection point below the F2 layer peak to define a thickness parameter of the F2 bottomside of the electron density profile, which is named B2. This study is focused on the effects of geomagnetic storms on the thickness parameter B2. We selected three equinoctial storms, namely 17 March 2013, 2 October 2013 and 17 March 2015. To investigate the behavior of the B2 parameter before, during and after those events, we have analyzed variations of GNSS derived vertical TEC (VTEC) and maximum electron density (NmF2) obtained from manually scaled ionograms over 20 stations at middle and low latitudes of Asian, Euro-African and American longitude sectors. The results show two main kinds of responses after the onset of the geomagnetic events: a peak of B2 parameter prior to the increase in VTEC and NmF2 (in ~60% of the cases) and a fluctuation in B2 associated with a decrease in VTEC and NmF2 (~25% of the cases). The behavior observed has been related to the dominant factor acting after the CME shocks associated with positive and negative storm effects. Investigation into the time delay of the different measurements according to location showed that B2 reacts before NmF2 and VTEC after the onset of the storms in all the cases. The sensitivity shown by B2 during the studied storms might indicate that experimentally derived thickness parameter B2 could be incorporated into the empirical models such as NeQuick in order to adapt them to storm situations that represent extreme cases of ionospheric weather-like conditions. MDPI 2021-11-05 /pmc/articles/PMC8588179/ /pubmed/34770676 http://dx.doi.org/10.3390/s21217369 Text en © 2021 by the authors. https://creativecommons.org/licenses/by/4.0/Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Article
Migoya-Orué, Yenca
Alazo-Cuartas, Katy
Kashcheyev, Anton
Amory-Mazaudier, Christine
Radicella, Sandro
Nava, Bruno
Fleury, Rolland
Ezquer, Rodolfo
B2 Thickness Parameter Response to Equinoctial Geomagnetic Storms
title B2 Thickness Parameter Response to Equinoctial Geomagnetic Storms
title_full B2 Thickness Parameter Response to Equinoctial Geomagnetic Storms
title_fullStr B2 Thickness Parameter Response to Equinoctial Geomagnetic Storms
title_full_unstemmed B2 Thickness Parameter Response to Equinoctial Geomagnetic Storms
title_short B2 Thickness Parameter Response to Equinoctial Geomagnetic Storms
title_sort b2 thickness parameter response to equinoctial geomagnetic storms
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8588179/
https://www.ncbi.nlm.nih.gov/pubmed/34770676
http://dx.doi.org/10.3390/s21217369
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