2017
DOI: 10.48550/arxiv.1706.09833
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Cosmological Effective Hamiltonian from full Loop Quantum Gravity Dynamics

Andrea Dapor,
Klaus Liegener
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Cited by 35 publications
(75 citation statements)
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“…As a full theory of quantum gravity is not available, these are still open questions. In the case of cosmology, symmetry reduced models of loop quantum gravity (LQG), so called loop quantum cosmology (LQC), were able to describe spacetime in the Planck regime [6][7][8][9] (nevertheless note recent criticism [10]). Similar efforts have been taken within the framework of spherically symmetric and static black holes, which are still simple due to a high amount of symmetries.…”
Section: Introductionmentioning
confidence: 99%
“…As a full theory of quantum gravity is not available, these are still open questions. In the case of cosmology, symmetry reduced models of loop quantum gravity (LQG), so called loop quantum cosmology (LQC), were able to describe spacetime in the Planck regime [6][7][8][9] (nevertheless note recent criticism [10]). Similar efforts have been taken within the framework of spherically symmetric and static black holes, which are still simple due to a high amount of symmetries.…”
Section: Introductionmentioning
confidence: 99%
“…The most important effect caused by the holonomy correction is that the cosmological singularity is replaced by a bounce; and this result holds irrespective of the choice of quantization prescription, i.e. the bounce exists no matter we choose the standard holonomy quantization prescription in which the Euclidean term and Lorentz term of the Hamiltonian constraint are treated on the same footing [7,8] or the modified holonomy quantization in which the Euclidean term and Lorentz term are treated differently in the way which mimics the quantization prescription of the Hamiltonian constraint of loop quantum gravity [9][10][11]. Despite the uniform existence of bounce, different choice of holonomy quantization prescription can lead to essentially different behaviors in the effective dynamics.…”
Section: Introductionmentioning
confidence: 96%
“…Instead, the operator which we obtain is defined on the Hilbert space of a fixed cubical graph, and so it has to be interpreted in the context of some suitable framework or a model which is based on the formalism of full loop quantum gravity, but where the restriction to a cubical graph is taken as an assumption. Such models include quantum-reduced loop gravity [12][13][14] -a simplified model of loop quantum gravity, which is derived from the full theory through a procedure representing a gauge fixing to a diagonal densitized triad -and the effective dynamics approach [15][16][17], where the expectation value of the Hamiltonian with respect to a family of semiclassical states is considered as an effective Hamiltonian generating evolution on a classical phase space. From a more theoretical standpoint, algebraic quantum gravity [18,19] constitutes a framework in which the use of a single fixed graph (which one can take to be e.g.…”
Section: Introductionmentioning
confidence: 99%