Abstract

We study various production mechanisms of sterile neutrinos in the early universe beyond and within the standard model. We obtain the quantum kinetic equations for production and the distribution function of sterile-like neutrinos at freeze-out, from which we obtain free streaming lengths, equations of state and coarse grained phase space densities. In a simple extension beyond the standard model, in which neutrinos are Yukawa coupled to a Higgs-like scalar, we derive and solve the quantum kinetic equation for sterile production and analyze the freeze-out conditions and clustering properties of this dark matter constituent. We argue that in the mass basis, standard model processes that produce active neutrinos also yield sterile-like neutrinos, leading to various possible production channels. Hence, the final distribution function of sterile-like neutrinos is a result of the various kinematically allowed production processes in the early universe. As an explicit example, we consider production of light sterile neutrinos from pion decay after the QCD phase transition, obtaining the quantum kinetic equation and the distribution function at freeze-out. A sterile-like neutrino with a mass in the keV range produced by this process is a suitable warm dark matter candidate with a free-streaming length of the order of few kpc consistent with cores in dwarf galaxies.

Highlights

  • In the concordance ΛCDM standard cosmological model, dark matter (DM) is composed of primordial particles, which are cold and collisionless [1,2]

  • We have described alternative production mechanisms of sterile-like neutrinos beyond and within the standard model of particle physics

  • We began with a description of the dynamical properties of dark matter particles described by frozen distribution functions, such as effective equation of state, phase space density and the free-streaming length, which determines the cutoff in the dark matter power spectrum

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Summary

Introduction

In the concordance ΛCDM standard cosmological model, dark matter (DM) is composed of primordial particles, which are cold and collisionless [1,2]. The same type of N-body simulations predict a large number of dark matter dominated satellites surrounding a typical galaxy, which is inconsistent with current observations [11,12,13] (missing satellites problem) Both the missing satellites and core-cusp problem can be simultaneously resolved by allowing some fraction of the dark matter to be “warm” (WDM) [14,15,16,17,18,19] with a massive “sterile” neutrino being one popular candidate [20,21,22,23,24]—other examples include Kaluza–Klein excitations from string compactification or axions [4,25], baryonic physics may be part of the solution. The prospect of a keV sterile DM candidate continues to motivate theoretical and observational studies [46,48,50,51,52,53,62,63,64,65,66,67,68,69,70,71]

Cosmological Consequences of Decoupled Particles
Free Streaming Length
Coarse Grained Phase Space Densities
Production from Scalar Decay
Quantum Kinetic Equation for Production
H02 Ω M 2 V2
Production from Standard Model Processes
Sterile Neutrinos from Pion Decay
Equation of State and Free Streaming
ΩDMH2 2 V2
Findings
Conclusions
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