2009
DOI: 10.1007/s10714-009-0892-9
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Spin foam quantization and anomalies

Abstract: Abstract. The most common spin foam models of gravity are widely believed to be discrete path integral quantizations of the Plebanski action. However, their derivation in present formulations is incomplete and lower dimensional simplex amplitudes are left open to choice. Since their large-spin behavior determines the convergence properties of the state-sum, this gap has to be closed before any reliable conclusion about finiteness can be reached. It is shown that these amplitudes are directly related to the pat… Show more

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Cited by 45 publications
(93 citation statements)
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“…This in particular means that the boundary of each face contains each edge at most once. With certain choices for amplitudes, this condition can be relaxed slightly; see, for example, [85][86][87].…”
Section: Endnotesmentioning
confidence: 99%
“…This in particular means that the boundary of each face contains each edge at most once. With certain choices for amplitudes, this condition can be relaxed slightly; see, for example, [85][86][87].…”
Section: Endnotesmentioning
confidence: 99%
“…In [75] we gave a rigorous expression where the correct measure factor [22], resulting from the second class constraints involved in the Holst action, was included. This inclusion made sure that the path integral qualified as a reduced phase space quantisation of the theory, as it has been stressed in [95]. A similar analysis has been carried out for the Plebanski theory in [96], however, the resulting measure factor is widely ignored in the SFM literature.…”
Section: The Holst Spin Foam Model Via Cubulationsmentioning
confidence: 87%
“…For theories with constraints and some interacting theories, this aim is non-trivial to obtain, and usually is not given by the heuristic Lebesgue measure. The obtention of the measure, has been a relevant step in developing of spin-foam models, which can be thought of as a path integral version of LQG [12,[35][36][37]. To cut a long story short (see e.g.…”
Section: {F{x)g{y)]d = {F{x)g{y)] -Jdudv{a{x)9'^{u)}d-'ß{mentioning
confidence: 99%
“…Nevertheless, the problem of the dynamics of the full theory has remained unsettled. In this respect, there are open issues as for instance how general relativity (GR) arises from LQG as a semiclassical limit of the quantum theory, and the fact that the algebra of quantum constraints, though free of anomalies, does not correspond to the algebra of classical constraints completely [12]. Purthermore, other problems are centered about the Hamiltonian constraint [13] which generates the dynamics of the system, unlike the gauge constraints associated with spatial diffeomorphisms and the internal gauge group remaining under control.…”
Section: Introductionmentioning
confidence: 99%