Difference between revisions of "Possible Quantum Gravity Effects in a Charged Bose Condensate Under Variable E.M. Field"
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In the weak field approximation to quantum gravity, a "local" positive cosmological term ?2 corresponds to a local negative squared mass term in the Lagrangian and may thus induce instability and local pinning of the gravitational field. Such a term can be produced by the coupling to an external Bose condensate. In the functional integral, the local pinning acts as a constraint on the field configurations. We discuss this model in detail and apply it to a phenomenological analysis of recent experimental results. | In the weak field approximation to quantum gravity, a "local" positive cosmological term ?2 corresponds to a local negative squared mass term in the Lagrangian and may thus induce instability and local pinning of the gravitational field. Such a term can be produced by the coupling to an external Bose condensate. In the functional integral, the local pinning acts as a constraint on the field configurations. We discuss this model in detail and apply it to a phenomenological analysis of recent experimental results. | ||
| − | [[Category:Scientific Paper]] | + | [[Category:Scientific Paper|possible quantum gravity effects charged bose condensate under variable e m field]] |
[[Category:Gravity]] | [[Category:Gravity]] | ||
Revision as of 10:55, 1 January 2017
| Scientific Paper | |
|---|---|
| Title | Possible Quantum Gravity Effects in a Charged Bose Condensate Under Variable E.M. Field |
| Author(s) | Giovanni Modanese |
| Keywords | Quantum Gravity, Bose-Einstein Condensate |
| Journal | ArXiv |
| No. of pages | 26 |
Abstract
In the weak field approximation to quantum gravity, a "local" positive cosmological term ?2 corresponds to a local negative squared mass term in the Lagrangian and may thus induce instability and local pinning of the gravitational field. Such a term can be produced by the coupling to an external Bose condensate. In the functional integral, the local pinning acts as a constraint on the field configurations. We discuss this model in detail and apply it to a phenomenological analysis of recent experimental results.
