2025/12/20 by Yakun Xi, Xi, Yakun
Mathematics · #Mathematical Dynamics and Fractals #Nonlinear Partial Differential Equations #Mathematical Approximation and Integration
paper · doi:10.48550/arxiv.2512.18379
Let (M,g) be a compact, connected Riemannian manifold of dimension n≥ 2, and let \ej\j=0^∞ be an orthonormal basis of Laplace eigenfunctions -Δg ej=λj2 ej. Given a finite Borel measure μ on M, consider the Kuznecov sum Nμ(λ):=∑λj≤ λ|∫M ej dμ|2. Assume that μ admits an averaged s-density constant Aμ with correlation dimension s∈(0,n). We prove that Nμ(λ)= (2π)-(n-s) \rm vol(B n-s) Aμ λn-s+ o(λn-s) (λ→∞). The averaged s-density condition is necessary for such a one-term asymptotic, and in general, the remainder o(λn-s) is sharp in the sense that it cannot be improved uniformly to a power-saving error term. This extends the classical Kuznecov formula of Zelditch for smooth submanifold measures to a broad class of singular and fractal measures.