Two solar proton fluence models based on ground level enhancement observations

dc.contributor.authorOsku Raukunen
dc.contributor.authorRami Vainio
dc.contributor.authorAllan J. Tylka
dc.contributor.authorWilliam F. Dietrich
dc.contributor.authorPiers Jiggens
dc.contributor.authorDaniel Heynderickx
dc.contributor.authorMark Dierckxsens
dc.contributor.authorNorma Crosby
dc.contributor.authorUrs Ganse
dc.contributor.authorRobert Siipola
dc.contributor.organizationfi=avaruustutkimuslaboratorio|en=Space Research Laboratory|
dc.contributor.organizationfi=fysiikan ja tähtitieteen laitos|en=Department of Physics and Astronomy|
dc.contributor.organization-code1.2.246.10.2458963.20.47833719389
dc.contributor.organization-code1.2.246.10.2458963.20.55477946762
dc.contributor.organization-code2606702
dc.converis.publication-id30619825
dc.converis.urlhttps://research.utu.fi/converis/portal/Publication/30619825
dc.date.accessioned2022-10-28T13:24:52Z
dc.date.available2022-10-28T13:24:52Z
dc.description.abstract<p>Solar energetic particles (SEPs) constitute an important component of the radiation environment in interplanetary space. Accurate modeling of SEP events is crucial for the mitigation of radiation hazards in spacecraft design. In this study we present two new statistical models of high energy solar proton fluences based on ground level enhancement (GLE) observations during solar cycles 19–24. As the basis of our modeling, we utilize a four parameter double power law function (known as the Band function) fits to integral GLE fluence spectra in rigidity. In the first model, the integral and differential fluences for protons with energies between 10 MeV and 1 GeV are calculated using the fits, and the distributions of the fluences at certain energies are modeled with an exponentially cut-off power law function. In the second model, we use a more advanced methodology: by investigating the distributions and relationships of the spectral fit parameters we find that they can be modeled as two independent and two dependent variables. Therefore, instead of modeling the fluences separately at different energies, we can model the shape of the fluence spectrum. We present examples of modeling results and show that the two methodologies agree well except for a short mission duration (1 year) at low confidence level. We also show that there is a reasonable agreement between our models and three well-known solar proton models (JPL, ESP and SEPEM), despite the differences in both the modeling methodologies and the data used to construct the models.<br /></p>
dc.identifier.eissn2115-7251
dc.identifier.jour-issn2115-7251
dc.identifier.olddbid181920
dc.identifier.oldhandle10024/165014
dc.identifier.urihttps://www.utupub.fi/handle/11111/39014
dc.identifier.urnURN:NBN:fi-fe2021042718978
dc.language.isoen
dc.okm.affiliatedauthorRaukunen, Osku
dc.okm.affiliatedauthorVainio, Rami
dc.okm.affiliatedauthorSiipola, Robert
dc.okm.discipline115 Astronomy and space scienceen_GB
dc.okm.discipline115 Avaruustieteet ja tähtitiedefi_FI
dc.okm.internationalcopublicationinternational co-publication
dc.okm.internationalityInternational publication
dc.okm.typeA1 ScientificArticle
dc.publisherEDP Sciences
dc.publisher.countryFranceen_GB
dc.publisher.countryRanskafi_FI
dc.publisher.country-codeFR
dc.relation.articlenumberA04
dc.relation.doi10.1051/swsc/2017031
dc.relation.ispartofjournalJournal of Space Weather and Space Climate
dc.relation.volume8
dc.source.identifierhttps://www.utupub.fi/handle/10024/165014
dc.titleTwo solar proton fluence models based on ground level enhancement observations
dc.year.issued2018

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