Given a symmetry group acting on a principal fibre bundle, symmetric states of the quantum theory of a diffeomorphism invariant theory of connections on this fibre bundle are defined. These symmetric states, equipped with a scalar product derived from the Ashtekar-Lewandowski measure for loop quantum gravity, form a Hilbert space of their own. Restriction to this Hilbert space yields a quantum symmetry reduction procedure in the framework of spin network states the structure of which is analyzed in detail. Three illustrating examples are discussed: Reduction of 3+1 to 2+1 dimensional quantum gravity, spherically symmetric electromagnetism and spherically symmetric gravity
Loop quantum gravity is an approach to quantum gravity that starts from the Hamiltonian formulation ...
I discuss the role played by the spin-network basis and recoupling theory (in its graphical tangle-t...
AbstractGiven a real-analytic manifoldM, a compact connected Lie groupGand a principalG-bundleP→M, t...
In the canonical quantization of gravity in terms of the Ashtekar variables one uses paths in the 3-...
Abstract. In the canonical quantization of gravity in terms of the Ashtekar variables one uses paths...
Based on a recent purely geometric construction of observables for the spatial diffeomorphism constr...
Quantization of diffeomorphism invariant theories of connections is studied. A complete solution of ...
We introduce a new basis on the state space of non-perturbative quantum gravity. The states of this ...
We investigate up to which extend the kinematic setting of loop quantum gravity can be fit into a di...
The kinematical setting of spherically symmetric quantum geometry, derived from the full theory of l...
19 pages, 1 figure; v2: corrected typos, section 4 expanded;The state space of Loop Quantum Gravity ...
As a toy model for the implementation of the diffeomorphism constraint, the interpretation of the re...
Much of the work in loop quantum gravity and quantum geometry rests on a mathematically rigorous int...
A simple diffeomorphism invariant theory of connections with the non-compact structure group R of re...
We investigate the action of diffeomorphisms in the context of Hamiltonian Gravity. By considering h...
Loop quantum gravity is an approach to quantum gravity that starts from the Hamiltonian formulation ...
I discuss the role played by the spin-network basis and recoupling theory (in its graphical tangle-t...
AbstractGiven a real-analytic manifoldM, a compact connected Lie groupGand a principalG-bundleP→M, t...
In the canonical quantization of gravity in terms of the Ashtekar variables one uses paths in the 3-...
Abstract. In the canonical quantization of gravity in terms of the Ashtekar variables one uses paths...
Based on a recent purely geometric construction of observables for the spatial diffeomorphism constr...
Quantization of diffeomorphism invariant theories of connections is studied. A complete solution of ...
We introduce a new basis on the state space of non-perturbative quantum gravity. The states of this ...
We investigate up to which extend the kinematic setting of loop quantum gravity can be fit into a di...
The kinematical setting of spherically symmetric quantum geometry, derived from the full theory of l...
19 pages, 1 figure; v2: corrected typos, section 4 expanded;The state space of Loop Quantum Gravity ...
As a toy model for the implementation of the diffeomorphism constraint, the interpretation of the re...
Much of the work in loop quantum gravity and quantum geometry rests on a mathematically rigorous int...
A simple diffeomorphism invariant theory of connections with the non-compact structure group R of re...
We investigate the action of diffeomorphisms in the context of Hamiltonian Gravity. By considering h...
Loop quantum gravity is an approach to quantum gravity that starts from the Hamiltonian formulation ...
I discuss the role played by the spin-network basis and recoupling theory (in its graphical tangle-t...
AbstractGiven a real-analytic manifoldM, a compact connected Lie groupGand a principalG-bundleP→M, t...