Cosmological perturbations on the Phantom brane
arXiv:1603.01277 · doi:10.1088/1475-7516/2016/07/038
Abstract
We obtain a closed system of equations for scalar perturbations in a multi-component braneworld. Our braneworld possesses a phantom-like equation of state at late times, , but no big-rip future singularity. In addition to matter and radiation, the braneworld possesses a new effective degree of freedom - the 'Weyl fluid' or 'dark radiation'. Setting initial conditions on super-Hubble spatial scales at the epoch of radiation domination, we evolve perturbations of radiation, pressureless matter and the Weyl fluid until the present epoch. We observe a gradual decrease in the amplitude of the Weyl-fluid perturbations after Hubble-radius crossing, which results in a negligible effect of the Weyl fluid on the evolution of matter perturbations on spatial scales relevant for structure formation. Consequently, the quasi-static approximation of Koyama and Maartens provides a good fit to the exact results during the matter-dominated epoch. We find that the late-time growth of density perturbations on the brane proceeds at a faster rate than in CDM. Additionally, the gravitational potentials and evolve differently on the brane than in CDM, for which . On the brane, by contrast, the ratio exceeds unity during the late matter-dominated epoch (). These features emerge as "smoking gun" tests of phantom brane cosmology and allow predictions of this scenario to be tested against observations of galaxy clustering and large-scale structure.
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Cited by in corpus (10)
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- Constraining phantom braneworld model from cosmic structure sizes
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- What if gravity becomes really repulsive in the future?
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