2004
DOI: 10.1088/0264-9381/21/22/012
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Hamiltonian analysis of Plebanski theory

Abstract: We study the Hamiltonian formulation of Plebanski theory in both the Euclidean and Lorentzian cases. A careful analysis of the constraints shows that the system is non regular, i.e. the rank of the Dirac matrix is non-constant on the non-reduced phase space. We identify the gravitational and topological sectors which are regular sub-spaces of the non-reduced phase space. The theory can be restricted to the regular subspace which contains the gravitational sector. We explicitly identify first and second class c… Show more

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Cited by 90 publications
(240 citation statements)
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“…The term C(B) includes polynomial constraints, reducing topological BF to GR. 5 Typically, it gives the set of second class constraints expressing B in terms of the tetrad field (or vierbein) and leading to GR in the first order formalism (for a detailed canonical analysis of (43), see [17]). The BF theory can be quantized as described in Section 2, discretizing the spacetime manifold with a Regge triangulation (or more generally a cellular decomposition), and then evaluating the partition function (2), where the variables are the representations j t and intertwiners i τ .…”
Section: Towards the Quantum Gravity Amplitudementioning
confidence: 99%
“…The term C(B) includes polynomial constraints, reducing topological BF to GR. 5 Typically, it gives the set of second class constraints expressing B in terms of the tetrad field (or vierbein) and leading to GR in the first order formalism (for a detailed canonical analysis of (43), see [17]). The BF theory can be quantized as described in Section 2, discretizing the spacetime manifold with a Regge triangulation (or more generally a cellular decomposition), and then evaluating the partition function (2), where the variables are the representations j t and intertwiners i τ .…”
Section: Towards the Quantum Gravity Amplitudementioning
confidence: 99%
“…It is based on a passive interpretation where the (diffeomorphism) gauge transformations do not change the discretization, but rather values of the fields. Explicit calculations in the case of gravity, however, so far look complicated and we will not pursue a calculation of the amplitudes here [22]. Nevertheless, one can hope that at least their asymptotic behavior for large labels can be found easily, which would allow us to see whether or not the state sum will be finite.…”
Section: Spin Foam Measurementioning
confidence: 99%
“…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. The result of the Gaussian integral is an interesting determinant that displays the full non linearity of Einstein's theory.…”
Section: The Holst Spin Foam Model Via Cubulationsmentioning
confidence: 88%
“…As it was shown in [96], if such constraints are taken into account, the measure present in the partition function should be augmented with a Jacobian coming from the Dirac brackets of the second class constraints.…”
Section: Spin Foam Models Through Bf Theorymentioning
confidence: 99%