At the end of Wieland's thesis there is a section (pages 136, 137) on future research interests.
It's worth seeing how they are laid out. One very interesting section (which I'll skip) is on the "flatness problem." Another section is on INCLUSION OF MATTER which is interesting enough that I want to quote in full:
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http://tel.archives-ouvertes.fr/docs/00/95/24/98/PDF/diss.pdf pages 136-137==
Inclusion of matter
To aim at a phenomenology of loop quantum gravity [201–203], strong enough to turn it falsifiable, we need to better understand how matter (our “rulers” and “clocks”) couples to the theory. Unfortunately, after decades of research, we still cannot say much about this issue. To overcome this trouble, I can see four roads to attack the problem, three of which I would like to study by myself:
(i) At first, there is what has been always tried in loop quantum gravity when it comes to this problem. Take any standard matter described by some Lagrangian, put in on an irregular lattice corresponding to a spin network state and canonically quantise. Although this approach was tried for all kinds of matter it led to very little physical insight. I think it is time to try different strategies.
(ii) The first idea that comes to my mind originates from an old paper by t’ Hooft [204]. I think it is a logical possibility that loop quantum gravity already contains a certain form of matter. If we look at the curvature of our models we find it is concentrated on the two-dimensional surfaces of the spinfoam faces. This curvature has a non-vanishing Ricci part which we can use (employing Einstein’s equations) to assign an energy momentum tensor to the spinfoam face. Following this logic one may then be able to reformulate the dynamics of spinfoam gravity as a scattering process of these two-dimensional worldsheets (that now carry energy-momentum) in a locally flat ambient space.
(iii) Loop quantum gravity is a theory of quantised area-angle-variables. I think this suggests not to start from the standard model that couples matter to tetrad (i.e. length-angle) variables. Instead we should take the fundamental discreteness of loop quantum gravity seriously, and try to add matter fields to the natural geometrical structures appearing, e.g. the two-dimensional spinfoam faces. In fact, when looking at the kinetic term of the action (3.46) a candidate immediately appears. We could just replace the commuting (π, ω) spinors by anti-commuting Weyl (Majorana) spinors, yielding a simple coupling of uncharged spin 1/2 particles to a spinfoam.
(iv) The recent understanding of loop quantum gravity in terms of twistors is mirrored [205–209] by similar developments in the study of scattering amplitudes of e.g. N = 4 super Yang–Mills theory . It is tempting to say these results all point towards the same direction eventually yielding a twistorial framework for all interactions.
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