Statistical description of massless excitations within a sphere with a linear equation of state and the dark energy case
arXiv:1805.03037 · doi:10.1142/S0217751X18500744
Abstract
In this paper we continue the investigations present in \cite{1}-\cite{3}. In particular, we extend the theorem proved in \cite{3} to any massless excitation in a given spherical box. As a first interesting result, we show that it is possible, contrary to the black hole case studied in detail in \cite{1,2,3}, to build macroscopic configurations with a dark energy equation of state. To this purpose, by requiring a stable configuration, a macroscopic dark fluid is obtained with an internal energy scaling as the volume , but with a fundamental correction looking like motivated by quantum fluctuations. Thanks to the proposition in section 3 (and in \cite{3} for gravitons), one can depict the dark energy in terms of massless excitations with a discrete spectrum. This fact open the possibility to test a possible physical mechanism converting usual radiation into dark energy in a macroscopic configuration, also in a cosmological context. In fact, for example, in a Friedmann flat universe with a cosmological constant particles are marginally trapped at the Hubble horizon for any given comoving observer.
Accepted for publication on Int. J. Mod. Phys. A
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