The quantization of gravity

In a former paper we proposed a model for the quantization of gravity by working in a bundle E where we realized the Hamilton constraint as the Wheeler-DeWitt equation. However, the corresponding operator only acts in the fibers and not in the base space. Therefore, we now discard the Wheeler-DeWitt...

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Bibliographic Details
Main Author: Gerhardt, Claus (Author)
Format: Article (Journal)
Language:English
Published: Oct 22 2018
In: Advances in theoretical and mathematical physics
Year: 2018, Volume: 22, Issue: 3, Pages: 709-757
ISSN:1095-0753
DOI:10.4310/ATMP.2018.v22.n3.a4
Online Access:Resolving-System, Volltext: http://dx.doi.org/10.4310/ATMP.2018.v22.n3.a4
Verlag, Volltext: http://intlpress.com/site/pub/pages/journals/items/atmp/content/vols/0022/0003/a004/index.html
Verlag, Volltext: https://www.math.uni-heidelberg.de/studinfo/gerhardt/preprints/qgravity2b.pdf
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Author Notes:Claus Gerhardt
Description
Summary:In a former paper we proposed a model for the quantization of gravity by working in a bundle E where we realized the Hamilton constraint as the Wheeler-DeWitt equation. However, the corresponding operator only acts in the fibers and not in the base space. Therefore, we now discard the Wheeler-DeWitt equation and express the Hamilton constraint differently, either with the help of the Hamilton equations or by employing a geometric evolution equation. There are two possible modifications possible which both are equivalent to the Hamilton constraint and which lead to two new models. In the first model we obtain a hyperbolic operator that acts in the fibers as well as in the base space and we can construct a symplectic vector space and a Weyl system.
Item Description:Gesehen am 31.10.2018
Physical Description:Online Resource
ISSN:1095-0753
DOI:10.4310/ATMP.2018.v22.n3.a4