Furthermore, this is an assumption that
fails
in conventional quantum field theory, because in that context
well defined operators and finite norm states need to be smeared
in at least three dimensions, and one-dimensional objects are too
singular.
The fact that at the basis of loop gravity there is a
mathematical assumption that fails for conventional Yang-Mills
quantum field theory is probably at the origin of some of the
resistance that loop quantum gravity encounters among some high
energy theorists. What distinguishes gravity from Yang-Mills
theories, however, and makes this assumption viable in gravity,
even if it fails for Yang-Mills theory, is diffeomorphism
invariance. The loop states are singular states that span a
``huge'' non-separable state space. (Non-perturbative)
diffeomorphism invariance plays two roles. First, it wipes away
the infinite redundancy. Second, it ``smears'' a loop state into
a knot state, so that the physical states are not really
concentrated in one dimension, but are, in a sense, smeared all
over the entire manifold by the nonperturbative diffeomorphisms.
This will be more clear in the next section.
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Loop Quantum Gravity
Carlo Rovelli http://www.livingreviews.org/lrr-1998-1 © Max-Planck-Gesellschaft. ISSN 1433-8351 Problems/Comments to livrev@aei-potsdam.mpg.de |