HEAT KERNELS ON COVERING SPACES AND TOPOLOGICAL INVARIANTS
HEAT KERNELS ON COVERING SPACES AND TOPOLOGICAL INVARIANTS
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DOI:
10.4310/jdg/1214448084
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发表时间:
1992
影响因子:
2.5
通讯作者:
J. Lott
中科院分区:
文献类型:
--
作者:
J. Lott
It is well known that there are relationships between the heat flow, acting on differential forms on a closed oriented manifold M, and the topology of M. From Hodge theory, one can recover the Betti numbers of M from the heat flow. Furthermore, Ray and Singer [42] defined an analytic torsion, a smooth invariant of acyclic flat bundles on M, and conjectured that it equals the classical Reidemeister torsion. This conjecture was proved to be true independently by Cheeger [7] and Muller [40]. The analytic torsion is nonzero only on odd-dimensional manifolds, and behaves in some ways as an odd-dimensional counterpart of the Euler characteristic [20]. If M is not simply-connected, then there is a covering space analog of the Betti numbers. Using the heat flow on the universal cover M, one can define the L2-Betti numbers of M [1] by taking the trace of the heat kernel not in the ordinary sense, but as an element of a certain type II von Neumann algebra. More concretely, this amounts to integrating the local trace of the heat kernel over a fundamental domain in M. In §11, we summarize this theory. We consider the covering space analog of the analytic torsion. This iΛanalytic torsion has the same relation to the iΛcohomology as the ordinary analytic torsion bears to de Rham cohomology. In §111 we define the iΛanalytic torsion <9^(M), under a technical assumption which we discuss later, and prove its basic properties. We show that &^(M) is a smooth invariant of manifolds whose L2-Betti numbers vanish. The proof is similar to that of the analogous statement for the ordinary analytic torsion, but requires some care because of the possible slow decay of the heat kernels for large time. In order to know if there are interesting examples of &^(M), we compute it in the case where M admits a hyperbolic metric. It is clear that is proportionate to the volume of the hyperbolic metric, which is