Here's what it says on page 3:
===quote===
The second consequence of the spin foam hypothesis follows from the work [7] where a new background independent approach to quantum gravity perturbation theory was proposed in the language of spin foam model. In this approach, the starting point is to write 4d gravity as a
perturbation of a topological BF theory based on the de-Sitter group for positive cosmological constant. The perturbation parameter G
NLambda is dimensionless and the perturbation theory transmutes gauge degree of freedom into physical degrees of freedom in a controlled way, order by order. In particular this means that the theory becomes topological in the limit G
N -> 0 . It has also been shown in this context that the coupling to matter particles can be explicitly performed by computing expectation value of Wilson lines observables [8], which are the most natural gauge invariant observables in this formulation.
The main consequence of interest to us from these works is the fact that, not only Feynman diagram amplitudes should be written as expectation values of certain natural observables in a spin foam model, but, moreover, the corresponding model should be a topological spin foam model based on a Poincaré BF theory.
So in summary, the spin foam hypothesis implies that usual Feynman graph can be expressed as the expectation value of certain observables in a topological spin foam model based on the Poincaré group. The validity of such a statement is for us a non-trivial check in support of the spin foam hypothesis.
The check is fourfold:
first, spin foam should arise naturally in Feynman integrals;
second, the spin model should agree with the structure predicted by [7, 8];
third, it should confirm the idea that the limit G
N -> 0 is a limit where gravity becomes topological;
and fourth the Feynman diagram observables should be understood as a Wilson lines (or more generally spin networks) expectation value in this spin foam model.
In this paper, we show that the first three conditions are indeed satisfied...
...The idea of our derivation is to consistently erase the information about flat space geometry from the Feynman integral and encode this information in terms of a choice of quantum amplitudes that should be summed over, and which dynamically determine flat space geometry. In doing so, a triangulation, and a specific spin foam model living on it, are naturally found; this allows us to express usual field theory amplitude in
a background independent manner. The idea that spin foam models code, in a background independent manner, the integration measure viewed by Feynman diagrams was formulated for the first time in [9] and [10] in the context of 3d-gravity.
An analysis similar to the one done here has already been performed in 3d [12], where it has been shown that the corresponding spin foam model is constructed in terms of 6j symbols of the 3d Euclidean group for flat space. The deformation of this spin foam model using quantum group naturally leads to a formulation of Feynman diagram coupled to 3d quantum gravity amplitudes [10, 11]. This corresponds to a
deformation of field theory carrying a deformed action of the Poincaré group.
===endquote===
[8]
http://arxiv.org/abs/gr-qc/0607014
Particles as Wilson lines of gravitational field
L. Freidel, J. Kowalski--Glikman, A. Starodubtsev
19 pages, some number of comments and clarifications added, to be published in Phys. Rev. D
"Since the work of Mac-Dowell-Mansouri it is well known that gravity can be written as a gauge theory for the de Sitter group. In this paper we consider the coupling of this theory to the simplest gauge invariant observables that is, Wilson lines. The dynamics of these Wilson lines is shown to reproduce exactly the dynamics of relativistic particles coupled to gravity, the gauge charges carried by Wilson lines being the mass and spin of the particles. Insertion of Wilson lines breaks in a controlled manner the diffeomorphism symmetry of the theory and the gauge degree of freedom are transmuted to particles degree of freedom."
Maybe I am wrong. In any case this is what I have to check to see whether there is some implication that one should expect a QG dispersion effect.