Tensorial Structure of the LQG graviton propagator
arXiv:0802.1201 · doi:10.1142/S0217751X0804007X
Abstract
We review the construction of the tensorial structure of the graviton propagator in the context of loop quantum gravity and spinfoam formalism. The main result of this analysis is that applying the same strategy used to compute the diagonal terms, the Barrett-Crane vertex is unable to yield the correct propagator in the long distance limit. The problem is in the intertwiner-independence of the Barrett-Crane vertex. We also review the asymptotic behavior of an alternative vertex that is able to give the correct propagator.
arXiv comment4 pages,; to appear in the proceedings of the II Stueckelberg Workshop, Int.J.Mod.Phys.A
References in corpus (12)
- LQG vertex with finite Immirzi parameter
- Group Field Theory: An overview
- Flipped spinfoam vertex and loop gravity
- The complete LQG propagator: I. Difficulties with the Barrett-Crane vertex
- The complete LQG propagator: II. Asymptotic behavior of the vertex
- Lorentzian LQG vertex amplitude
- Spin foam model from canonical quantization
- Numerical evidence of regularized correlations in spin foam gravity
- A semiclassical tetrahedron
- The perturbative Regge-calculus regime of Loop Quantum Gravity
- Numerical indications on the semiclassical limit of the flipped vertex
- Compatibility of radial, Lorenz and harmonic gauges
Cited by in corpus (7)
- Asymptotic analysis of the EPRL four-simplex amplitude
- Linking covariant and canonical LQG: new solutions to the Euclidean Scalar Constraint
- Anomalous dimension in semiclassical gravity
- LQG propagator: III. The new vertex
- Spin-Foam Models and the Physical Scalar Product
- Asymptotics of LQG fusion coefficients
- Semi-Classical Holomorphic Transition Amplitudes in Covariant Loop Quantum Gravity