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Problems and Alternatives to Lambda Cold Dark Matter - Berkeley ...

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Extra Symmetries<br />

A. de la Macorra, C. Stephan-Ot<strong>to</strong>, Phys. Rev. Lett. 87 (2001) 271301<br />

The starting point is a dark gauge group “DG” whose particles interact with the<br />

st<strong>and</strong>ard model only via gravity.<br />

The gauge coupling constant becomes strong at lower energies, it will bind the<br />

elementary dark fields <strong>to</strong>gether at the phase transition or condensation scale Λc.<br />

Above this scale the particles are massless <strong>and</strong> at the condensation scale Λc they<br />

acquire a mass of the order of Λc.<br />

The elementary fields will form gauge invariant particles due <strong>to</strong> the strong coupling.<br />

These particles are dark “mesons” <strong>and</strong> dark “baryons”.<br />

Ej: The model with SU(3) gauge group has 6 chiral + antichiral fields with<br />

97.5 degrees of freedom, a condensation scale Λc = 42 eV <strong>and</strong> an<br />

inverse power potential with V = Λ , n = 2/3.<br />

This model gives a warm DM with a free streaming scale λfs < 0.6 Mpc<br />

<strong>and</strong> an equation of state parameter for the DE wDEo=−0.9 with Ωm = 0.27,<br />

ΩDEo = 0.73.<br />

4+n<br />

c φ −n<br />

45

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