2009
DOI: 10.1103/physrevd.80.064028
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Spin foam models for quantum gravity from lattice path integrals

Abstract: Spin foam models for quantum gravity are derived from lattice path integrals. The setting involves variables from both lattice BF theory and Regge calculus. The action consists in a Regge action, which depends on areas, dihedral angles and includes the Immirzi parameter. In addition, a measure is inserted to ensure a consistent gluing of simplices, so that the amplitude is dominated by configurations which satisfy the parallel transport relations. We explicitly compute the path integral as a sum over spin foam… Show more

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Cited by 79 publications
(102 citation statements)
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References 45 publications
(161 reference statements)
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“…• As we see in a moment, another important role played by δ 1 is to make deficit angles ε f of emergent Regge geometries to be small but nonzero, as a resolution of the "flatness problem" in SFM [21,[43][44][45]. The detailed discussion is given momentarily below Eq.…”
Section: Spin Sum and Regularizationmentioning
confidence: 99%
See 1 more Smart Citation
“…• As we see in a moment, another important role played by δ 1 is to make deficit angles ε f of emergent Regge geometries to be small but nonzero, as a resolution of the "flatness problem" in SFM [21,[43][44][45]. The detailed discussion is given momentarily below Eq.…”
Section: Spin Sum and Regularizationmentioning
confidence: 99%
“…(70) would imply strict flatness ε f = 0. This strict flatness has been proven to be one of the main obstacles for recovering classical gravity from SFMs [21,[43][44][45]. But if δ 1 is non-zero as above, then small excitations of ε f are allowed, and therefore arbitrary smooth curved geometries may emerge from refining triangulations while δ → 0.…”
Section: Equation Of Motion and Small Deficit Anglesmentioning
confidence: 99%
“…This is close to the state-sum language, and is the usual way in which spin foam models are written down. The dual (in the sense of Fourier transform) way of describing the amplitude is given by the left hand side of (4.13), and can be interpreted as path integral for a lattice theory, with some gauge-invariant action functional determined by the S f [25,27,28], depending on finitely many holonomies. In this formulation there is a direct connection to an action functional which is determined by the S f .…”
Section: Surjective P : Bf Theorymentioning
confidence: 99%
“…However, many questions remain unanswered. The most concerning one is the so-called flatness problem, firstly mentioned by Freidel and Conrady [24], and later explored by Bonzom [25] and Hellmann and Kaminski [26]. They argue that the EPRL partition function, in the semiclassical limit, is dominated by classical flat geometries.…”
Section: Introduction and Motivationsmentioning
confidence: 99%