Neutrinos massivos em cosmologia: geometria e crescimento de estruturas
DOI:
https://doi.org/10.47456/Cad.Astro.v7n1.51840Palavras-chave:
cosmologia, neutrinos, geometria, crescimento de estruturasResumo
Neutrinos são as partículas mais abundantes do Universo depois dos fótons, mas suas massas ainda não são conhecidas. Neste artigo mostramos como a cosmologia moderna permite investigar essa propriedade fundamental por meio da Radiação Cósmica de Fundo, das oscilações acústicas bariônicas e do crescimento das estruturas em larga escala. Discutimos como neutrinos, relativísticos no Universo primordial e não relativísticos em épocas tardias, deixam assinaturas tanto na história da expansão quanto na formação da teia cósmica. Mostramos também como dados recentes de levantamentos de galáxias, como o DESI, combinados com simulações cosmológicas, permitem impor limites cada vez mais precisos sobre a soma das massas dos neutrinos, tornando o Universo um poderoso detector dessas partículas.
Referências
[1] W. Pauli, Dear radioactive ladies and gentlemen, Phys. Today 31N9, 27 (1978).
[2] S. Navas et al., Review of particle physics, Phys. Rev. D 110 (3), 030001 (2024).
[3] M. R. Krishnaswamy et al., THE KGF NUCLEON DECAY EXPERIMENT, Prog. Math. Phys. 9, 25 (1983).
[4] Y. Fukuda et al., Evidence for oscillation of atmospheric neutrinos, Phys. Rev. Lett. 81, 1562 (1998). ArXiv: hep-ex/9807003.
[5] K. Eguchi et al., First Results from KamLAND: Evidence for Reactor Antineutrino Disappearance, Phys. Rev. Lett. 90, 021802 (2003).
[6] F. P. An et al., Observation of electronantineutrino disappearance at Daya Bay, Phys. Rev. Lett. 108, 171803 (2012). ArXiv: 1203.1669.
[7] P. Adamson et al., First measurement of electron neutrino appearance in NOvA, Phys. Rev. Lett. 116 (15), 151806 (2016). ArXiv:1601.05022.
[8] J. K. Ahn et al., Observation of Reactor Electron Antineutrino Disappearance in the RENO Experiment, Phys. Rev. Lett. 108, 191802 (2012). ArXiv:1204.0626.
[9] K. Abe et al., Indication of Electron Neutrino Appearance from an Accelerator-produced Off-axis Muon Neutrino Beam, Phys. Rev. Lett. 107, 041801 (2011). ArXiv: 1106.2822.
[10] K. Lande e P. Wildenhain, The Homestake chlorine solar neutrino experiment: Past, present and future, Nucl. Phys. B Proc. Suppl. 118, 49 (2003).
[11] A. Bellerive et al., The Sudbury Neutrino Observatory, Nucl. Phys. B 908, 30 (2016). ArXiv:1602.02469.
[12] N. Aghanim et al., Planck 2018 results. VI. Cosmological parameters, Astron. Astrophys. 641, A6 (2020), [Erratum: Astron. Astrophys. 652, C4 (2021)]. ArXiv: 1807.06209.
[13] S. Dodelson e F. Schmidt, Modern Cosmology (Academic Press, 2020).
[14] J. Lesgourgues e S. Pastor, Massive neutrinos and cosmology, Phys. Rept. 429, 307 (2006). ArXiv: astro-ph/0603494.
[15] Y. Y. Y. Wong, Neutrino mass in cosmology: status and prospects, Ann. Rev. Nucl. Part. Sci. 61, 69 (2011). ArXiv:1111.1436.
[16] P. J. E. Peebles, Principles of Physical Cosmology (Princeton University Press, 2020).
[17] L. Amendola e S. Tsujikawa, Dark Energy: Theory and Observations (Cambridge University Press, 2015).
[18] DESI Collaboration et al., Data Release 1 of the Dark Energy Spectroscopic Instrument, arXiv e-prints arXiv:2503.14745 (2025). Ar Xiv:2503.14745.
[19] M. Abdul Karim et al., DESI DR2 results. II. Measurements of baryon acoustic oscillations and cosmological constraints, Phys. Rev. D 112 (8), 083515 (2025). ArXiv: 2503.14738.
[20] M. Chevallier e D. Polarski, Accelerating universes with scaling dark matter, Int. J. Mod. Phys. D 10, 213 (2001). ArXiv: gr-qc/0009 008.
[21] E. V. Linder, Exploring the expansion history of the universe, Phys. Rev. Lett. 90, 091301 (2003). ArXiv: astro-ph/0208512.
[22] E. Di Valentino, S. Gariazzo e O. Mena, Most constraining cosmological neutrino mass bounds, Phys. Rev. D 104 (8), 083504 (2021). ArXiv:2106.15267.
[23] W. Elbers et al., Negative neutrino masses as a mirage of dark energy, Phys. Rev. D 111 (6), 063534 (2025). ArXiv:2407.10965.
[24] D. Wang et al., Updating neutrino mass constraints with background measurements, Phys. Rev. D 110 (10), 103536 (2024). Ar Xiv:2405.03368.
[25] W. Hu, Covariant linear perturbation formalism, ICTP Lect. Notes Ser. 14, 145 (2003). ArXiv: astro-ph/0402060.
[26] P. Zhang e Y. Cai, BOSS full-shape analysis from the EFTofLSS with exact time dependence, JCAP 01 (01), 031 (2022). ArXiv: 2111.05739.
[27] P. Zhang et al., BOSS Correlation Function analysis from the Effective Field Theory of Large-Scale Structure, JCAP 02 (02), 036 (2022). ArXiv:2110.07539.
[28] T. Colas et al., Efficient Cosmological Analysis of the SDSS/BOSS data from the Effective Field Theory of Large-Scale Structure, JCAP 06, 001 (2020). ArXiv:1909.07951.
[29] G. D’Amico et al., The Cosmological Analysis of the SDSS/BOSS data from the Effective Field Theory of Large-Scale Structure, JCAP 05, 005 (2020). ArXiv:1909.05271.
[30] O. H. E. Philcox et al., Determining the Hubble Constant without the Sound Horizon: Measurements from Galaxy Surveys, Phys. Rev. D 103 (2), 023538 (2021). ArXiv: 2008.08084.
[31] M. M. Ivanov, M. Simonović e M. Zaldarriaga, Cosmological Parameters from the BOSS Galaxy Power Spectrum, JCAP 05, 042 (2020). ArXiv:1909.05277.
[32] F. Bernardeau et al., Large-scale structure of the universe and cosmological perturbation theory, Phys. Rept. 367, 1 (2002). ArXiv: astro-ph/0112551.
[33] R. W. Hockney e J. W. Eastwood, Computer simulation using particles (1988).
[34] F. Villaescusa-Navarro et al., The Quijote Simulations, ApJS 250 (1), 2 (2020). ArXiv: 1909.05273.
Downloads
Publicado
Edição
Seção
Licença
Copyright (c) 2026 Guilherme Brando

Este trabalho está licenciado sob uma licença Creative Commons Attribution 4.0 International License.



