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Eigenvalues of the volume operator in loop quantum gravity
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Eigenvalues of the volume operator
in loop quantum gravity
Krzysztof A. Meissner1
Institute of Theoretical Physics, Warsaw University
Hoz?a 69, 00-681 Warsaw, Poland
and
CERN, Theoretical Division
Abstract
We present a simple method to calculate certain sums of the eigen-
values of the volume operator in loop quantum gravity. We derive the
asymptotic distribution of the eigenvalues in the classical limit of very
large spins which turns out to be of a very simple form. The results can
be useful for example in the statistical approach to quantum gravity.
1 Introduction
Volume operators were introduced by Rovelli and Smolin [1] and by Ashtekar
and Lewandowski [2] (the latter will be used in the current paper). The
volume operator is much less understood than the area operator, one of the
reasons being that it is not diagonal in any reasonable basis and there are
ambiguities in defining its action on a given graph (see [3] and references
therein; clarification of the issue is given in [4]). The matrix elements of the
volume operator were obtained in [5], [6] (in the context of cosmology [7]);
however, the formulae are very complicated and it is extremely difficult to
get analytic expressions for the eigenvalues of the volume operator, except
for very small values of the momenta (for some bounds on the eigenvalues
see [8]). Therefore it seems worthwhile to try to find some alternative way
of describing the eigenvalues. In this paper we show that relatively simple
formulae can be obtained for the sums of squares (or higher even powers) of
the eigenvalues, with the most important “quantum numbers” in the vertex
1E-mail address: Krzysztof.Meissner@fuw.edu.pl
1
fixed: j, j1, j2, j3, where j is the total spin and j1, j2, j3 are spins of the
incoming legs. We also calculate the sums of higher powers (4, 6 and 8) of
the eigenvalues with fixed j1, j2, j3. At the end of the paper we derive (in the
form of an integra
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