New Variables for Classical and Quantum Gravity in all Dimensions IV. Matter Coupling
arXiv:1105.3706 · doi:10.1088/0264-9381/30/4/045004
Abstract
We employ the techniques introduced in the companion papers to derive a connection formulation of Lorentzian General Relativity coupled to Dirac fermions in dimensions D+1 > 2 with compact gauge group. The technique that accomplishes that is similar to the one that has been introduced in 3+1 dimensions already: First one performs a canonical analysis of Lorentzian General Relativity using the time gauge and then introduces an extension of the phase space analogous to the one employed in the first paper of this series to obtain a connection theory with SO(D+1) as the internal gauge group subject to additional constraints. The success of this method rests heavily on the strong similarity of the Lorentzian and Euclidean Clifford algebras. A quantisation of the Hamiltonian constraint is provided.
13 pages. v2: Journal version. Minor clarifications
References in corpus (3)
Cited by in corpus (16)
- The Spin Foam Approach to Quantum Gravity
- Loop Quantum Gravity
- Black hole entropy from loop quantum gravity in higher dimensions
- BF Theory Explanation of the Entropy for Non-rotating Isolated Horizons
- Higher-dimensional quantum Oppenheimer-Snyder model
- Higher dimensional Loop Quantum Cosmology
- The Wald entropy formula and loop quantum gravity
- The thermodynamics of isolated horizons in loop quantum gravity
- Fermions in Loop Quantum Gravity and Resolution of Doubling Problem
- Some notes on the Kodama state, maximal symmetry, and the isolated horizon boundary condition
- Reformulation of Boundary BF Theory Approach to Statistical Explanation of the Entropy of Isolated Horizons
- Alternative Self-dual Gravity in Eight Dimensions
- Loop quantum cosmology in 2+1 dimension
- Fix Immirzi parameter by quasinormal modes in four and higher spacetime dimensions
- Fermions coupled to the Palatini action in dimensions
- Hamiltonian Theory: generalizations to higher dimensions, supersymmetry and modified gravity