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arXiv · astro-ph/0501021

Long-range interactions between dark-matter particles in a model with a cosmological, spontaneously-broken chiral symmetry

Abstract

In a cosmological model with a chiral symmetry, there are two, dynamically-related spin-zero fields, a scalar $ϕ$ and a pseudoscalar $b$. These fields have self-interactions. Spontaneous symmetry breaking results in a very massive scalar particle with $m_ϕ\cong 5 \times 10^{11}\GeV$, and a nearly massless, (Goldstone-like) pseudoscalar particle with $0< m_b <~ 2.7\times 10^{-6}\eV$. One or both particles can be part of dark matter. There are coherent long-range interactions (at range $\sim 1/m_b \simgt 10\cm$), from exchange of a $b$ particle between a pair of $b$ particles, a pair of $ϕ$ particles, and between a $ϕ$ and a $b$. We compare the strength of potentials for the different pairs to the corresponding gravitational potentials (within the same range $\sim 1/m_b$), and show that the new force dominates between a b pair, that gravitation dominates between a $ϕ$ pair, and that the potentials are comparable for a $ϕ$-$b$ pair. The new interaction strength between a $b$ pair is comparable to the gravitational interaction between a $ϕ$ pair; its possibly greater coherent effect originates in the possibility that the number density of a very light $b$ can be greater than that of a massive $ϕ$. We consider these results in the context of recent speculations concerning possible effects of special forces between dark-matter particles on certain galactic, and inter-galactic, properties.

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BibTeXRIS

Saul Barshay, Georg Kreyerhoff. 2005-04-19. Long-range interactions between dark-matter particles in a model with a cosmological, spontaneously-broken chiral symmetry. https://doi.org/10.1142/s0217732305017329

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