Using machine learning to compress the matter transfer function T (k)

Detalhes bibliográficos
Autor(a) principal: Orjuela-Quintana, J. Bayron
Data de Publicação: 2023
Outros Autores: Nesseris, Savvas, Cardona, Wilmar [UNESP]
Tipo de documento: Artigo
Idioma: eng
Título da fonte: Repositório Institucional da UNESP
Texto Completo: http://dx.doi.org/10.1103/PhysRevD.107.083520
http://hdl.handle.net/11449/248801
Resumo: The linear matter power spectrum P(k,z) connects theory with large scale structure observations in cosmology. Its scale dependence is entirely encoded in the matter transfer function T(k), which can be computed numerically by Boltzmann solvers, and can also be computed semianalytically by using fitting functions such as the well-known Bardeen-Bond-Kaiser-Szalay (BBKS) and Eisenstein-Hu (EH) formulas. However, both the BBKS and EH formulas have some significant drawbacks. On the one hand, although BBKS is a simple expression, it is only accurate up to 10%, which is well above the 1% precision goal of forthcoming surveys. On the other hand, while EH is as accurate as required by upcoming experiments, it is a rather long and complicated expression. Here, we use the genetic algorithms (GAs), a particular machine learning technique, to derive simple and accurate fitting formulas for the transfer function T(k). When the effects of massive neutrinos are also considered, our expression slightly improves over the EH formula, while being notably shorter in comparison.
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spelling Using machine learning to compress the matter transfer function T (k)The linear matter power spectrum P(k,z) connects theory with large scale structure observations in cosmology. Its scale dependence is entirely encoded in the matter transfer function T(k), which can be computed numerically by Boltzmann solvers, and can also be computed semianalytically by using fitting functions such as the well-known Bardeen-Bond-Kaiser-Szalay (BBKS) and Eisenstein-Hu (EH) formulas. However, both the BBKS and EH formulas have some significant drawbacks. On the one hand, although BBKS is a simple expression, it is only accurate up to 10%, which is well above the 1% precision goal of forthcoming surveys. On the other hand, while EH is as accurate as required by upcoming experiments, it is a rather long and complicated expression. Here, we use the genetic algorithms (GAs), a particular machine learning technique, to derive simple and accurate fitting formulas for the transfer function T(k). When the effects of massive neutrinos are also considered, our expression slightly improves over the EH formula, while being notably shorter in comparison.Departamento de Física Universidad Del Valle Ciudad Universitaria MeléndezInstituto de Física Teórica UAM-CSIC Universidad Autonóma de Madrid, CantoblancoICTP South American Institute for Fundamental Research Instituto de Física Teórica Universidade Estadual PaulistaICTP South American Institute for Fundamental Research Instituto de Física Teórica Universidade Estadual PaulistaCiudad Universitaria MeléndezUniversidad Autonóma de MadridUniversidade Estadual Paulista (UNESP)Orjuela-Quintana, J. BayronNesseris, SavvasCardona, Wilmar [UNESP]2023-07-29T13:54:06Z2023-07-29T13:54:06Z2023-04-15info:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/articlehttp://dx.doi.org/10.1103/PhysRevD.107.083520Physical Review D, v. 107, n. 8, 2023.2470-00292470-0010http://hdl.handle.net/11449/24880110.1103/PhysRevD.107.0835202-s2.0-85158875982Scopusreponame:Repositório Institucional da UNESPinstname:Universidade Estadual Paulista (UNESP)instacron:UNESPengPhysical Review Dinfo:eu-repo/semantics/openAccess2023-07-29T13:54:06Zoai:repositorio.unesp.br:11449/248801Repositório InstitucionalPUBhttp://repositorio.unesp.br/oai/requestopendoar:29462023-07-29T13:54:06Repositório Institucional da UNESP - Universidade Estadual Paulista (UNESP)false
dc.title.none.fl_str_mv Using machine learning to compress the matter transfer function T (k)
title Using machine learning to compress the matter transfer function T (k)
spellingShingle Using machine learning to compress the matter transfer function T (k)
Orjuela-Quintana, J. Bayron
title_short Using machine learning to compress the matter transfer function T (k)
title_full Using machine learning to compress the matter transfer function T (k)
title_fullStr Using machine learning to compress the matter transfer function T (k)
title_full_unstemmed Using machine learning to compress the matter transfer function T (k)
title_sort Using machine learning to compress the matter transfer function T (k)
author Orjuela-Quintana, J. Bayron
author_facet Orjuela-Quintana, J. Bayron
Nesseris, Savvas
Cardona, Wilmar [UNESP]
author_role author
author2 Nesseris, Savvas
Cardona, Wilmar [UNESP]
author2_role author
author
dc.contributor.none.fl_str_mv Ciudad Universitaria Meléndez
Universidad Autonóma de Madrid
Universidade Estadual Paulista (UNESP)
dc.contributor.author.fl_str_mv Orjuela-Quintana, J. Bayron
Nesseris, Savvas
Cardona, Wilmar [UNESP]
description The linear matter power spectrum P(k,z) connects theory with large scale structure observations in cosmology. Its scale dependence is entirely encoded in the matter transfer function T(k), which can be computed numerically by Boltzmann solvers, and can also be computed semianalytically by using fitting functions such as the well-known Bardeen-Bond-Kaiser-Szalay (BBKS) and Eisenstein-Hu (EH) formulas. However, both the BBKS and EH formulas have some significant drawbacks. On the one hand, although BBKS is a simple expression, it is only accurate up to 10%, which is well above the 1% precision goal of forthcoming surveys. On the other hand, while EH is as accurate as required by upcoming experiments, it is a rather long and complicated expression. Here, we use the genetic algorithms (GAs), a particular machine learning technique, to derive simple and accurate fitting formulas for the transfer function T(k). When the effects of massive neutrinos are also considered, our expression slightly improves over the EH formula, while being notably shorter in comparison.
publishDate 2023
dc.date.none.fl_str_mv 2023-07-29T13:54:06Z
2023-07-29T13:54:06Z
2023-04-15
dc.type.status.fl_str_mv info:eu-repo/semantics/publishedVersion
dc.type.driver.fl_str_mv info:eu-repo/semantics/article
format article
status_str publishedVersion
dc.identifier.uri.fl_str_mv http://dx.doi.org/10.1103/PhysRevD.107.083520
Physical Review D, v. 107, n. 8, 2023.
2470-0029
2470-0010
http://hdl.handle.net/11449/248801
10.1103/PhysRevD.107.083520
2-s2.0-85158875982
url http://dx.doi.org/10.1103/PhysRevD.107.083520
http://hdl.handle.net/11449/248801
identifier_str_mv Physical Review D, v. 107, n. 8, 2023.
2470-0029
2470-0010
10.1103/PhysRevD.107.083520
2-s2.0-85158875982
dc.language.iso.fl_str_mv eng
language eng
dc.relation.none.fl_str_mv Physical Review D
dc.rights.driver.fl_str_mv info:eu-repo/semantics/openAccess
eu_rights_str_mv openAccess
dc.source.none.fl_str_mv Scopus
reponame:Repositório Institucional da UNESP
instname:Universidade Estadual Paulista (UNESP)
instacron:UNESP
instname_str Universidade Estadual Paulista (UNESP)
instacron_str UNESP
institution UNESP
reponame_str Repositório Institucional da UNESP
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repository.name.fl_str_mv Repositório Institucional da UNESP - Universidade Estadual Paulista (UNESP)
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