Why do we observe a small but non zero cosmological constant?

Padmanabhan, T. (2002) Why do we observe a small but non zero cosmological constant? Classical and Quantum Gravity, 19 (17). L167-L174. ISSN 0264-9381

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Official URL: http://iopscience.iop.org/0264-9381/19/17/102

Related URL: http://dx.doi.org/10.1088/0264-9381/19/17/102

Abstract

The current observations seem to suggest that the universe has a positive cosmological constant of the order of H20 while the most natural value for the cosmological constant will be L-2P, where LP = (Għ/c3)½ is the Planck length. This reduction of the cosmological constant from L-2P to L-2P(LPH0)2 may be interpreted as due to the ability of quantum microstructure of spacetime to readjust itself and absorb bulk vacuum energy densities. Being a quantum-mechanical process, such a cancellation cannot be exact and the residual quantum fluctuations appear as the 'small' cosmological constant. I describe the features of a toy model for the spacetime microstructure which could allow for the bulk vacuum energy densities to be cancelled leaving behind a small residual value of the correct magnitude. Some other models (such as those based on the canonical ensemble for the 4-volume or quantum fluctuations of the horizon size) lead to an insignificantly small value of H20(LPH0)n with n = 0.5-1 showing that obtaining the correct order of magnitude for the residual fluctuations in the cosmological constant is a nontrivial task, because of the existence of the small dimensionless number H0LP.

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