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<dc:title xml:lang="en">New radiative transfer methods for the study of Reionisation</dc:title>
<dcterms:alternative xml:lang="fr">Nouvelles méthodes de transfert radiatif pour l’étude de la réionisation</dcterms:alternative>
<dc:subject xml:lang="fr">Transfert radiatif</dc:subject>
<dc:subject xml:lang="fr">Réionisation</dc:subject>
<dc:subject xml:lang="fr">Simulation cosmologique</dc:subject>
<dc:subject xml:lang="en">Radiative Transfer</dc:subject>
<dc:subject xml:lang="en">Reionisation</dc:subject>
<dc:subject xml:lang="en">Cosmological simulation</dc:subject>
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<tef:elementdEntree autoriteExterne="027842339" autoriteSource="Sudoc">Ionisation</tef:elementdEntree>
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<dcterms:abstract xml:lang="fr">Nous cherchons à étudier le modèle de transfert radiatif Pn afin d’observer si il est capable de corriger les tares du modèle couramment utilisé en astrophysique, M1. Pn est un modèle spectral ne garantissant pas la positivité de l’énergie, mais qui, utilisé dans des conditions optimales, permet de complètement corriger les problèmes de directionnalité de M1, au prix d’une exécution informatique plus coûteuse. En se servant d’une implémentation optimisée de Pn nommée RKMS, nous soumettons les deux modèles à une série de tests standardisés pour le transfert radiatif dans le cadre de la réionisation. Pn performe aussi bien que M1 sur les tests les plus basiques comme la sphère de Strömgren, tout en montrant de nettes améliorations dans d’autres. Notamment, le test de la carte cosmologique met les modèles en situation réaliste de simulation cosmologique, et permet de montrer clairement les artefacts omniprésents introduits par M1, que Pn gomme complètement.</dcterms:abstract>
<dcterms:abstract xml:lang="en">We are aiming at studying the radiative transfer model Pn to determine if it is able to correct the flaws of the most commonly used model in astrophysics, M1. Pn is a spectral model which doesn’t guarantee the positivity of energy but which, used in optimal conditions, allows to completely correct the directionality issues of M1, with a high computational cost. Using an optimised implementation of Pn called RKMS, we undergo a series of standardised tests to compare our two models in the context of reionisation. Pn performs as good as M1 on the more basic tests such as the strömgren sphere, while showing great improvements in others. Mainly, the cosmological map test put the two models in a realistic situation of cosmological simulation, and showcases very clearly the omnipresent artefacts introduced by M1, that Pn completely erases.</dcterms:abstract>
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