2005
DOI: 10.1090/s1079-6762-05-00149-6
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Lower bounds for the spectral function and for the remainder in local Weyl’s law on manifolds

Abstract: Abstract. We announce asymptotic lower bounds for the spectral function of the Laplacian and for the remainder in the local Weyl's law on Riemannian manifolds. In the negatively curved case, methods of thermodynamic formalism are applied to improve the estimates. Our results develop and extend the unpublished thesis of A. Karnaukh. We discuss some ideas of the proofs; for complete proofs see our extended paper on the subject.

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Cited by 6 publications
(4 citation statements)
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“…, as λ → +∞, which appears to be an almost impossibly strong condition (cf. [18], [34]). This is because the curve γ opt , which is the boundary of the region in the problem raised in [11] corresponds to ε(λ) = c/λ, 1 Recall that a Zoll manifold is one for which the geodesic flow is periodic with a common minimal period .…”
Section: Introductionmentioning
confidence: 99%
“…, as λ → +∞, which appears to be an almost impossibly strong condition (cf. [18], [34]). This is because the curve γ opt , which is the boundary of the region in the problem raised in [11] corresponds to ε(λ) = c/λ, 1 Recall that a Zoll manifold is one for which the geodesic flow is periodic with a common minimal period .…”
Section: Introductionmentioning
confidence: 99%
“…Ideally, one would want to be able to use a variant of (3.5) where the exponential factor is not present for the second term in the right. Lower bounds of Jakobson and Polterovich [20]- [21] show that this error term cannot be O(λ n−1 2), but their bounds do not rule out some improvement over (3.5), which would lead to more favorable estimates.…”
Section: Discussionmentioning
confidence: 99%
“…In each cyclic subspace, the function is a complete unitary invariant for U restricted to ( ): by this we mean that the function encodes all the spectral data coming from the vectors = U , ∈ Z. For background literature on spectral function and their applications we refer to [1,10,16,[19][20][21]. In summary, the spectral representation theorem is the assertion that commuting unitary operators in Hilbert space may be represented as multiplication operators in an L 2 -Hilbert space.…”
Section: Introductionmentioning
confidence: 99%
“…In each cyclic subspace, the function p ϕ is a complete unitary invariant for U restricted to H(ϕ): by this we mean that the function p ϕ encodes all the spectral data coming from the vectors f k = U k ϕ, k ∈ Z. For background literature on spectral function and their applications we refer to [1,10,16,19,20,21].…”
Section: Introductionmentioning
confidence: 99%