Non-separable Hilbert space in LQG Most of Hilbert spaces appearing in real life are separable ones: even such large for the first spaces as Fock space, spaces of functions in infinite number of variables and so on. However I heard that when dealing with quantum loop gravity one encounter non-separable Hilbert space. 

Could somebody explain how this space is constructed? What are natural operators, relevant for LQG, acting in such space? 

I would like also to understand some conceptual reason for the apperance of nonseparable Hilbert spaces in this context: since the main idea of LQG is that the geometry is ,,quantized'' I would suspect that Hilbert spaces which occure in LQG would be finite dimensional. 
 A: The lack of separability in the kinematical Hilbert space in LQG is a mathematical artifact; it doesn't affect the physics, and it disappears when tweaking the mathematical setting. 
In more detail, according to the abstract of this paper by Fairbairn & Rovelli in 2004:

In the standard construction, the kinematical Hilbert space of the diffeomorphism invariant states is non-separable. This is a consequence of the fact that the knot-space of the equivalence class of graphs under diffeomorphisms is non-countable.

They add: 

However, the continuous moduli labelling these classes do not appear to affect the physics.

And then:

We investigate the possibility that these moduli could be only a consequence of a poor choice in in the fine-tuning of the mathematical setting.

To which they affirm:

We show that by simply choosing a minor extension of the functional class of the classical fields and coordinates, the moduli disappears, the knot classes become countable, and the kinematical Hilbert space becomes countable.

