The Geometry of Time in Topological Quantum Gravity of the Ricci Flow

We continue the study of topological nonrelativistic quantum gravity associated with a family of Ricci flow equations on Riemannian manifolds. This topological gravity is of the cohomological type, and it exhibits an {cal N}=2 extended BRST symmetry. In our previous work, we constructed this theory in a two-step procedure in the appropriate nonrelativistic {cal N}=2 superspace, first presenting a topological theory of the spatial metric g_ij, and then adding the superspace versions of the lapse and shift variables n and nⁱ while gauging the symmetries of foliation-preserving spacetime diffeomorphisms. In the relation to Perelman's theory of the Ricci flow, the role of Perelman's dilaton is played by our nonprojectable lapse. Here we demonstrate that this construction is equivalent to a standard one-step BRST gauge-fixing of a theory whose fields are g_ij, nⁱ and n, and whose gauge symmetries consist of (i) the topological deformations of g_ij, and (ii) the ultralocal nonrelativistic limit of spacetime diffeomorphisms. The supercharge Q of our superspace construction plays the role of the BRST charge. The spacetime diffeomorphism symmetries appear in an interestingly "shifted" form, which may be of broader interest for nonrelativistic quantum gravity outside of the present topological context. In contrast to the foliation-preserving spacetime diffeomorphisms, the gauge symmetries identified in this paper act nonprojectably on time, making it clear that this theory has no local propagating degrees of freedom. We point out an intriguing dual interpretation of the same theory, as a gauge fixing of a dual copy of ultralocal spacetime diffeomorphisms, with the role of ghosts and antighosts interchanged and the second supercharge bar Q of the {cal N}=2 superalgebra playing the role of the BRST charge in the dual picture.