2006
DOI: 10.2977/prims/1166642153
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$L^2$-Betti Numbers of Infinite Configuration Spaces

Abstract: The space Γ X of all locally finite configurations in a infinite covering X of a compact Riemannian manifold is considered. The de Rham complex of square-integrable differential forms over Γ X , equipped with the Poisson measure, and the corresponding de Rham cohomology and the spaces of harmonic forms are studied. A natural von Neumann algebra containing the projection onto the space of harmonic forms is constructed. Explicit formulae for the corresponding trace are obtained. A regularized index of the Dirac … Show more

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Cited by 3 publications
(9 citation statements)
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“…and STR P = e −χ(K) . The latter expression coincides with the formula derived in [1] for the case the de Rham complex over the configuration space equipped with the Poisson measure. Remark 6.1.…”
Section: Fock Space Of Braid-invariant Harmonic Forms: L 2 -Dimensionsupporting
confidence: 85%
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“…and STR P = e −χ(K) . The latter expression coincides with the formula derived in [1] for the case the de Rham complex over the configuration space equipped with the Poisson measure. Remark 6.1.…”
Section: Fock Space Of Braid-invariant Harmonic Forms: L 2 -Dimensionsupporting
confidence: 85%
“…The right-hand side of formula (45) can be understood as a regularized index of the Dirac operator D + D * , where D := m N d m N , see [11] and e.g. [30] for the discussion of von Neumann supertraces in geometry and topology of Riemannian manifolds and their relation to L 2 -index theorems, and [1], [2], [3] for the extension of these notions to the framework of infinite configuration spaces.…”
Section: Fock Space Of Braid-invariant Harmonic Forms: L 2 -Dimensionmentioning
confidence: 99%
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“…Laplace operators with potentials q given by homogeneous random fields (see [10,21,29]). That is, q is supposed to be G-invariant in the sense that q(gx, ω) = q(x, U g ω), (2) where G g → U g is a representation of G by measure preserving transformations of the probability space. For such operators, the -function is defined by the formula…”
Section: Introductionmentioning
confidence: 99%
“…Let us remark that the interest in the analysis on infinite configuration spaces has risen in recent years, because of new approaches and rich applications in statistical mechanics and quantum field theory (see [3,4] and the review [30]). L 2 -Betti numbers of configuration spaces with Poisson and Lebesgue-Poisson measures, were computed in [2,15], respectively (see also [1,14,16]). …”
Section: Introductionmentioning
confidence: 99%