Abstract
We present a generalized version of holographic dark energy arguing that it must be considered in the maximally subspace of a cosmological model. In the context of brane cosmology it leads to a bulk holographic dark energy which transfers its holographic nature to the effective 4D dark energy. As an application we use a single-brane model and we show that in the low energy limit the behavior of the effective holographic dark energy coincides with that predicted by conventional 4D calculations. However, a finite bulk can lead to radically different results.
Highlights
Holographic dark energy [1, 2, 3, 4, 5, 6, 7, 8, 9] is an interesting and ingenious idea of explaining the recently observed Universe acceleration [10]
Its framework is the black hole thermodynamics [15, 16] and the connection of the UV cut-of of a quantum field theory, which gives rise to the vacuum energy, with the largest distance of the theory [17]. Such a connection is necessary for the applicability of quantum field theory in large distances and results form the argument that the total energy of a system should not exceed the mass of a black hole of the same size, since in this case the system would collapse to a black hole violating the second law of thermodynamics
In this work we present holographic dark energy, restored to its natural foundations, and for a consistency test we apply it to a general braneworld model well studied in the literature
Summary
Holographic dark energy [1, 2, 3, 4, 5, 6, 7, 8, 9] is an interesting and ingenious idea of explaining the recently observed Universe acceleration [10]. Its framework is the black hole thermodynamics [15, 16] and the connection (known from AdS/CFT correspondence) of the UV cut-of of a quantum field theory, which gives rise to the vacuum energy, with the largest distance of the theory [17] Such a connection is necessary for the applicability of quantum field theory in large distances and results form the argument that the total energy of a system (which entropy is in general proportional to its volume) should not exceed the mass of a black hole of the same size (which entropy is proportional to its area), since in this case the system would collapse to a black hole violating the second law of thermodynamics. In IV we discuss the physical implications of our analysis and we summarize the obtained results
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