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Ultraweak excitations of the quantum vacuum as physical models of gravity

M Consoli

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It has been argued by several authors that the spacetime curvature observed in gravitational fields, and the same idea of forms of physical equivalence different from the Lorentz group, might emerge from the dynamical properties of the physical flat-space vacuum in a suitable hydrodynamic limit. To explore this idea, one could start by representing the physical vacuum as a Bose condensate of elementary quanta and look for vacuum excitations that, on a coarse grained scale, resemble the Newtonian potential. In this way, it is relatively easy to match the weak-field limit of classical general relativity or of some of its possible variants. The idea that Bose condensates can provide various forms of gravitational dynamics is not new. Here, I want to emphasize some genuine quantum field theoretical aspects that can help to understand (i) why infinitesimally weak, 1/r interactions can indeed arise from the same physical vacuum of electroweak and strong interactions and (ii) why, on a coarse-grained scale, their dynamical effects can be reabsorbed into an effective curved metric structure.


PACS

04.50.-h Higher-dimensional gravity and other theories of gravity

04.20.Gz Spacetime topology, causal structure, spinor structure

95.30.Lz Hydrodynamics

98.80.Es Observational cosmology (including Hubble constant, distance scale, cosmological constant, early Universe, etc)

04.20.Jb Exact solutions

95.30.Sf Relativity and gravitation

MSC

83C15 Exact solutions

81T20 Quantum field theory on curved space backgrounds

85A30 Hydrodynamic and hydromagnetic problems (See also 76Y05)

83F05 Cosmology

83C75 Space-time singularities, cosmic censorship, etc.

Subjects

Fluid dynamics

Gravitation and cosmology

Astrophysics and astroparticles

Dates

Issue 22 (21 November 2009)

Received 7 April 2009, in final form 16 September 2009

Published 20 October 2009



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