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Domain Wall Dominated Universes

Richard A. Battye, Martin Bucher, David Spergel

Abstract

We consider a cosmogony with a dark matter component consisting of a network of frustrated domain walls. Such a network provides a solid dark matter component with $p=-(2/3)ρ$ that remains unclustered on small scales and with $Ω_{\rm dw}\approx 0.7$ can reconcile a spatially flat universe with the many observations indicating $Ω_{\rm m}\approx 0.3.$ Because of its large negative pressure, this component can explain the recent observations indicating an accelerating universe without recourse to a non-vanishing cosmological constant. We explore the viability of this proposal and prospects for distinguishing it from other kinds of proposed dark matter with significant negative pressure.

Domain Wall Dominated Universes

Abstract

We consider a cosmogony with a dark matter component consisting of a network of frustrated domain walls. Such a network provides a solid dark matter component with that remains unclustered on small scales and with can reconcile a spatially flat universe with the many observations indicating Because of its large negative pressure, this component can explain the recent observations indicating an accelerating universe without recourse to a non-vanishing cosmological constant. We explore the viability of this proposal and prospects for distinguishing it from other kinds of proposed dark matter with significant negative pressure.

Paper Structure

This paper contains 1 equation, 2 figures, 1 table.

Figures (2)

  • Figure 1: Rescaled CMB Moments for SDM Models. In the first four panels $\ell (\ell +1)C_\ell$ versus $\ell$ is plotted for $w=-1/3, -1/2, -2/3, -5/6$ for several values of the longitudinal sound speed for a universe with $\Omega_{\rm m}=0.3, \Omega_{\rm sdm}=0.7.$ The solid curve corresponds to $c_s=0.0$ and $c_s=0.2, 0.4, 0.6, 0.8$ are indicated by the line styles dotted, dashed, dot-dash, and dot-dot-dash, respectively. rescaled so that the horizon size at recombination subtends the same angle in the sky today as for a $w=-1$ model with the same $\Omega _{\rm m}.$ The bottom middle panel indicates the rescaled and renormalized moments for the quintessence models with $w=-1/3, -1/2, -2/3, -5/6,$ and the bottom right panel shows all models of the previous panels for comparison.
  • Figure 2: Domain wall dominated models compatible with constraints on $\sigma_8$ from X-ray clusters. The solid line indicates the stringent lower limit and the dotted line the upper limit, which can be weakened by including a tensor component. The vertical and horizontal axes are $h$ and $\Omega_{\rm m},$ respectively. The left and right panels indicate the spectral indices $n=1.0$ and $n=1.1$, respectively. In both cases the longitudinal sound speed is $c_s=0.2.$