Abstract
In the previous chapter, we have seen some aspects of spatial quantum geometry, with its characteristic discrete spectra, emerge even in isotropic models. Now, these spatial structures have to fit into a consistent quantum space–time which in a certain sense reduces to a solution of Einstein’s equation in a semiclassical or low-curvature limit. Only completing this most challenging step will make the theory one of quantum gravity, rather than of spatial quantum geometry.
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Notes
- 1.
Notice that this sense of regularity does not by itself imply UV-finiteness in the usual meaning of quantum field theory. To test finiteness, one would have to compute scattering amplitudes of particle excitations on a quantum geometry state, which is difficult. It thus remains open how exactly a fundamentally finite version of loop quantum gravity could resolve non-renormalizability issues of perturbative quantum gravity.
- 2.
These cannot be all contributions because higher-derivative terms of the metric do not arise by the holonomy replacement. See Chap. 13 for a general treatment of effective canonical dynamics which introduces new quantum degrees of freedom analogously to higher-derivative actions.
- 3.
In such commutators in the full theory, a single \(V_v\) gives the same contribution as the volume operator of all of space: contributions from vertices not lying on the edges used for the holonomy in the commutator cancel. But this observation does not change the fact that inverse-triad operators receive contributions only from local vertex contributions of the volume operator. In reduced models, homogeneity implies that all vertex contributions must contribute equally; one can properly capture the full behavior only by using single vertex or plaquette contributions from the outset.
- 4.
These models were initially introduced under the name “improved” quantization [37, 38], indicating advantages in certain regimes of low curvature and large volume. However, the modifications introduced in these models turned out to be rather ad-hoc. (To appreciate this realization, the models are sometimes called “improvised.”) By now, what goes by the name “improved dynamics” is under strong pressure from different types of inconsistencies. The improved dynamics is itself to be improved, giving the name a rather misleading connotation.
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Bojowald, M. (2011). Dynamics: Changing Atoms of Space–Time. In: Quantum Cosmology. Lecture Notes in Physics, vol 835. Springer, New York, NY. https://doi.org/10.1007/978-1-4419-8276-6_4
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