Partial and complete observables for canonical general relativity (original) (raw)

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Abstract

In this work we will consider the concepts of partial and complete observables for canonical general relativity. These concepts provide a method to calculate Dirac observables. The central result of this work is that one can compute Dirac observables for general relativity by dealing with just one constraint. For this we have to introduce spatial diffeomorphism invariant Hamiltonian constraints. It will turn out that these can be made to be Abelian. Furthermore the methods outlined here provide a connection between observables in the spacetime picture, i.e. quantities invariant under spacetime diffeomorphisms, and Dirac observables in the canonical picture.

Publication:

Classical and Quantum Gravity

Pub Date:

November 2006

DOI:

10.1088/0264-9381/23/22/006

10.48550/arXiv.gr-qc/0507106

arXiv:

arXiv:gr-qc/0507106

Bibcode:

2006CQGra..23.6155D

Keywords:

E-Print:

33 pages