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Observational constraints on secret neutrino interactions from big bang nucleosynthesis

Observational constraints on secret neutrino interactions from big bang nucleosynthesis


Titill: Observational constraints on secret neutrino interactions from big bang nucleosynthesis
Höfundur: Huang, Guo-yuan
Ohlsson, Tommy   orcid.org/0000-0002-3525-8349
Zhou, Shun
Útgáfa: 2018-04-05
Tungumál: Enska
Umfang: 075009
Háskóli/Stofnun: Háskóli Íslands
University of Iceland
Svið: Verkfræði- og náttúruvísindasvið (HÍ)
School of Engineering and Natural Sciences (UI)
Deild: Raunvísindastofnun (HÍ)
Science Institute (UI)
Birtist í: Physical Review D;97(7)
ISSN: 2470-0010
2470-0029 (eISSN)
DOI: 10.1103/PhysRevD.97.075009
Efnisorð: Big bang nucleosynthesis; Neutrino interactions; Neutrinos; Miklihvellur; Heimsfræði; Atóm; Kjarneðlisfræði
URI: https://hdl.handle.net/20.500.11815/972

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Tilvitnun:

Huang, G.-y., Ohlsson, T., & Zhou, S. (2018). Observational constraints on secret neutrino interactions from big bang nucleosynthesis. Physical Review D, 97(7), 075009. doi:10.1103/PhysRevD.97.075009

Útdráttur:

We investigate possible interactions between neutrinos and massive scalar bosons via g ϕ ¯ ν ν ϕ (or massive vector bosons via g V ¯ ν γ μ ν V μ ) and explore the allowed parameter space of the coupling constant g ϕ (or g V ) and the scalar (or vector) boson mass m ϕ (or m V ) by requiring that these secret neutrino interactions (SNIs) should not spoil the success of big bang nucleosynthesis (BBN). Incorporating the SNIs into the evolution of the early Universe in the BBN era, we numerically solve the Boltzmann equations and compare the predictions for the abundances of light elements with observations. It turns out that the constraint on g ϕ and m ϕ in the scalar-boson case is rather weak, due to a small number of degrees of freedom (d.o.f.). However, in the vector-boson case, the most stringent bound on the coupling g V ≲ 6 × 10 − 10 at 95% confidence level is obtained for m V ≃ 1     MeV , while the bound becomes much weaker g V ≲ 8 × 10 − 6 for smaller masses m V ≲ 10 − 4     MeV . Moreover, we discuss in some detail how the SNIs affect the cosmological evolution and the abundances of the lightest elements.

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Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article’s title, journal citation, and DOI.

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