1997
DOI: 10.1016/s0550-3213(97)00017-5
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Diffeomorphism invariant measure for finite-dimensional geometries

Abstract: We consider families of geometries of D-dimensional space, described by a finite number of parameters. Starting from the De Witt metric we extract a unique integration measure which turns out to be a geometric invariant, i.e. independent of the gauge fixed metric used for describing the geometries. The measure is also invariant in form under an arbitrary change of parameters describing the geometries. We prove the existence of geometries for which there are no related gauge fixing surfaces orthogonal to the ga… Show more

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Cited by 28 publications
(24 citation statements)
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“…There has been considerable debate in the literature on the measure for quantum Regge calculus [75][76][77][78]. One difficulty that makes any analytical calculations hard are the triangle inequalities that make determining the integration range very complicated.…”
Section: Quantum Regge Calculus: the Path Integral Measurementioning
confidence: 99%
“…There has been considerable debate in the literature on the measure for quantum Regge calculus [75][76][77][78]. One difficulty that makes any analytical calculations hard are the triangle inequalities that make determining the integration range very complicated.…”
Section: Quantum Regge Calculus: the Path Integral Measurementioning
confidence: 99%
“…One may hope that in the non-perturbative Regge regime no gauge-fixing is necessary, since the contributions from zero-modes cancel out in the path-integral representation for operator averages [124,122]. Menotti and Peirano [162,164,163,161], following a strategy suggested by Jevicki and Ninomiya [134], have argued vigorously that the functional integral should contain a non-trivial Faddeev-Popov determinant. Their starting point is somewhat different from that adopted in the path-integral simulations (see also [199]).…”
Section: Gauge Invariance In Regge Calculus?mentioning
confidence: 99%
“…where = 2(1 − g) is the Euler characteristic of the manifold M expressed by the number of handles g in M. For a simplicial complex K the Euler characteristic can be computed as 12) where N 0 , N 1 , and N 2 denote the number of sites, links, and triangles, respectively. In higher than two dimensions an R 2 interaction term is sometimes added to guarantee the boundedness of the gravitational action from below.…”
Section: Model and Simulationmentioning
confidence: 99%