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Approaches to Quantum Gravity

Approaches to Quantum Gravity

Approaches to Quantum Gravity

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Categorical geometry and the mathematical foundations of <strong>Quantum</strong> <strong>Gravity</strong> 93In my view, the implications of this idea should be studied for physical geometry.Does it mean, for example, that the physical real numbers contain infinitesimals?6.3.3 Application of decoherent his<strong>to</strong>ries <strong>to</strong> the BC modelThissectionisworkinprogress.We would like <strong>to</strong> explore classical his<strong>to</strong>ries in the BC model. The goal of this is<strong>to</strong> show that consistent his<strong>to</strong>ries exist for the model which closely approximate thegeometry of pseudo-Riemannian manifolds, and that the decoherence functionalconcentrates around solutions of Einstein’s equation.The natural choice for macroscopic variables in the BC model would be theoverall geometry of regions composing a number of simplices in the underlyingcomplex of the model. It is easier <strong>to</strong> choose the regions themselves <strong>to</strong> be simpliceswhich we call large <strong>to</strong> distinguish them from the fundamental simplices of whichthey are composed.The program for showing that the geometric data on the internal small simplicesdecoheres the overall geometry of the large ones involves two steps.In the first, we use microlocal analysis <strong>to</strong> construct a basis of states in whichall the geometrical variables of the large simplices are simultaneously sharp <strong>to</strong> asmall inaccuracy. These would combine <strong>to</strong> give a set of projection opera<strong>to</strong>rs whoseimages correspond <strong>to</strong> pseudo-Riemannian geometries on the complex, now though<strong>to</strong>f as a triangulated manifold.This problem is mathematically similar <strong>to</strong> finding a wavepacket for a particle.The symplectic space for the tetrahedron turns out <strong>to</strong> be equivalent <strong>to</strong> thesymplectic structure on the space of Euclidean quadrilaterals in the Euclidean signaturecase, and <strong>to</strong> have an interesting hyper-Kahler structure in the case of theLorentzian signature. This allows us <strong>to</strong> use powerful mathematical simplifications,which make me believe the problem is quite solvable.The second step would be <strong>to</strong> show the decoherence functional which arises fromaveraging over the small variables causes the large variables <strong>to</strong> decohere, and thatthe decoherence functional concentrates around solutions of Einstein’s equation.This is quite analogous <strong>to</strong> known results for material systems such as the pis<strong>to</strong>n.The existence of a Brownian motion approximation for the internal variablesmakes me hopeful that this will work out, similarly <strong>to</strong> the case of the pis<strong>to</strong>n, wherean ideal gas approximation is the key <strong>to</strong> the calculation.A more challenging problem would be <strong>to</strong> work out the <strong>to</strong>pos theoretic interpretationof the decoherence program in the case of the BC model.The site of this <strong>to</strong>pos would be the category whose objects are the “large”triangulations, and whose morphisms are coarse grainings.

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