and, in general
where is the parallel propagator of along , defined by
(See  for more details.) These are the loop observables, introduced in Yang Mills theories in [95, 96], and in gravity in [183, 184].
The loop observables coordinatize the phase space and have a closed Poisson algebra, denoted by the loop algebra. This algebra has a remarkable geometrical flavor. For instance, the Poisson bracket between and is non vanishing only if lies over ; if it does, the result is proportional to the holonomy of the Wilson loops obtained by joining and at their intersection (by rerouting the 4 legs at the intersection). More precisely
is a vector distribution with support on and is the loop obtained starting at the intersection between and , and following first and then . is with reversed orientation.
A (non-SU(2) gauge invariant) quantity that plays a role in certain aspects of the theory, particularly in the regularization of certain operators, is obtained by integrating the E field over a two dimensional surface S
where f is a function on the surface S, taking values in the Lie algebra of SU (2). As an alternative to the full loop observables (5, 6, 7), one can also take the holonomies and E [S, f] as elementary variables [15, 17]; this is more natural to do, for instance, in the C*-algebric approach .
|Loop Quantum Gravity
© Max-Planck-Gesellschaft. ISSN 1433-8351
Problems/Comments to email@example.com