Influence of a planar boundary on the electric field emitted by a particle shower

The radio detection of cosmic rays consists in the estimation of the properties of a primary cosmic ray by observing the electric field emitted by the extensive air shower (EAS) created when the primary cosmic ray enters the atmosphere. This technique is fully operative nowadays and presents a good...

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Main Authors: García-Fernández, Daniel, Revenu, Benoît, Escudie, Antony, Martin, Lilian
Format: Text
Language:unknown
Published: arXiv 2018
Subjects:
Online Access:https://dx.doi.org/10.48550/arxiv.1811.11003
https://arxiv.org/abs/1811.11003
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spelling ftdatacite:10.48550/arxiv.1811.11003 2023-05-15T18:23:00+02:00 Influence of a planar boundary on the electric field emitted by a particle shower García-Fernández, Daniel Revenu, Benoît Escudie, Antony Martin, Lilian 2018 https://dx.doi.org/10.48550/arxiv.1811.11003 https://arxiv.org/abs/1811.11003 unknown arXiv https://dx.doi.org/10.1103/physrevd.99.063009 arXiv.org perpetual, non-exclusive license http://arxiv.org/licenses/nonexclusive-distrib/1.0/ High Energy Astrophysical Phenomena astro-ph.HE FOS Physical sciences article-journal Article ScholarlyArticle Text 2018 ftdatacite https://doi.org/10.48550/arxiv.1811.11003 https://doi.org/10.1103/physrevd.99.063009 2022-04-01T08:54:03Z The radio detection of cosmic rays consists in the estimation of the properties of a primary cosmic ray by observing the electric field emitted by the extensive air shower (EAS) created when the primary cosmic ray enters the atmosphere. This technique is fully operative nowadays and presents a good degree of maturity. In addition, several projects intend to employ this technique for the detection of neutrinos. In order for the technique to be useful, accurate methods for computing the electric field created by a particle shower in the context of a particular experiment must exist. Although current ground-based radio experiments lie on the air-soil interface and some planned experiments on the South Pole envision antennas near the air-ice interface, most of the analytical approaches and Monte Carlo codes used for calculating the electric field either do not take into account the effect of the boundary or calculate the radiation fields only (direct, reflected and transmitted radiation fields). When the particle shower and the antenna are close to the boundary, compared to the observation wavelength, the far-field approximation breaks down, which is the case for the low-frequency EXTASIS experiment, for instance. We present in this work a new formula for calculating the exact field emitted by a particle track in two semi-infinite media separated by a planar boundary. We also explore the validity of the far-field approximation and make some predictions for EAS using a simple shower model. Text South pole DataCite Metadata Store (German National Library of Science and Technology) South Pole
institution Open Polar
collection DataCite Metadata Store (German National Library of Science and Technology)
op_collection_id ftdatacite
language unknown
topic High Energy Astrophysical Phenomena astro-ph.HE
FOS Physical sciences
spellingShingle High Energy Astrophysical Phenomena astro-ph.HE
FOS Physical sciences
García-Fernández, Daniel
Revenu, Benoît
Escudie, Antony
Martin, Lilian
Influence of a planar boundary on the electric field emitted by a particle shower
topic_facet High Energy Astrophysical Phenomena astro-ph.HE
FOS Physical sciences
description The radio detection of cosmic rays consists in the estimation of the properties of a primary cosmic ray by observing the electric field emitted by the extensive air shower (EAS) created when the primary cosmic ray enters the atmosphere. This technique is fully operative nowadays and presents a good degree of maturity. In addition, several projects intend to employ this technique for the detection of neutrinos. In order for the technique to be useful, accurate methods for computing the electric field created by a particle shower in the context of a particular experiment must exist. Although current ground-based radio experiments lie on the air-soil interface and some planned experiments on the South Pole envision antennas near the air-ice interface, most of the analytical approaches and Monte Carlo codes used for calculating the electric field either do not take into account the effect of the boundary or calculate the radiation fields only (direct, reflected and transmitted radiation fields). When the particle shower and the antenna are close to the boundary, compared to the observation wavelength, the far-field approximation breaks down, which is the case for the low-frequency EXTASIS experiment, for instance. We present in this work a new formula for calculating the exact field emitted by a particle track in two semi-infinite media separated by a planar boundary. We also explore the validity of the far-field approximation and make some predictions for EAS using a simple shower model.
format Text
author García-Fernández, Daniel
Revenu, Benoît
Escudie, Antony
Martin, Lilian
author_facet García-Fernández, Daniel
Revenu, Benoît
Escudie, Antony
Martin, Lilian
author_sort García-Fernández, Daniel
title Influence of a planar boundary on the electric field emitted by a particle shower
title_short Influence of a planar boundary on the electric field emitted by a particle shower
title_full Influence of a planar boundary on the electric field emitted by a particle shower
title_fullStr Influence of a planar boundary on the electric field emitted by a particle shower
title_full_unstemmed Influence of a planar boundary on the electric field emitted by a particle shower
title_sort influence of a planar boundary on the electric field emitted by a particle shower
publisher arXiv
publishDate 2018
url https://dx.doi.org/10.48550/arxiv.1811.11003
https://arxiv.org/abs/1811.11003
geographic South Pole
geographic_facet South Pole
genre South pole
genre_facet South pole
op_relation https://dx.doi.org/10.1103/physrevd.99.063009
op_rights arXiv.org perpetual, non-exclusive license
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
op_doi https://doi.org/10.48550/arxiv.1811.11003
https://doi.org/10.1103/physrevd.99.063009
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