PlanetPhysics/Quantum Geometry 3

This is a contributed topic on [[../SR/|spacetime]] [[../MoyalDeformation/|quantization]] and loop quantum gravity often descibed as quantum geometry.

Quantum Geometry

In 4 dimensions, one of the attractive [[../SupercomputerArchitercture/|programs]] of spacetime quantization is "quantum geometry", often represented as "loop quantum gravity" . Loop quantum gravity starts with a [[../Hamiltonian2/|Hamiltonian]] formulation of the first order formalism, with constraints, written in analogy to the (3+1)-dimensional case that take the form:

$D_i{E}^{ia}=0,$ $E_a^i{R}_{ij}^a=0,$ and ${ϵ}_{abc}{E}^{ib}{E}^{jc}{R}_{ij}^a=0,$

where the indices $i,j$ and $k$ are the spatial indices on a surface of constant time, $E^{ia}={ϵ}^{ij}{e}_j^a,$ $D_i$ is the $SO(2,1)$ gauge-covariant derivative for the connection $\omega$, and the $R_{ij}^a$ are the spatial components of the curvature two-form.

Lattice methods and Spin Foams

Ponzano-Regge and Turaev-Viro models are examples of "spin foam" models that is, they are models based on [[../PiecewiseLinear/|simplicial complexes]] with faces, edges, and vertices labeled by [[../GroupRepresentations/|group representations]] and intertwiners. [[../ComplexOfSpinNetworks/|spin foam]] models are based on a fixed triangulation of spacetime, with edge lengths serving as the basic gravitational variables. An alternative scheme is "dynamical triangulation", in which edge lengths are fixed and the path integral is represented as a sum over triangulations.

Dynamical triangulation is a useful alternative to [[../SimplicialCWComplex/|spin foams]] that has been shown to provide a useful method in [[../CoriolisEffect/|two-dimensional]] gravity.

Discussion

Several [[../QuantumOperatorAlgebra5/|quantum observables]] whose expectation values generally give [[../CoIntersections/|topological]] information about the nature of quantized spacetime have been already considered but-- with very few exceptions-- the results in this area has remain largely mathematical in nature; thus, surprisingly little is understood about the physics of such [[../QuantumSpinNetworkFunctor2/|observables]], although some are most likely to be related to length and perhaps [[../Volume/|volumes]], whereas other observables are connected to scattering amplitudes for quantum paricles.

"Perhaps the most important lesson of (2+1)-dimensional quantum gravity is that general relativity can, in fact, be quantized." (download here a concise online review)