Definition

For a (A,H,D)(\mathcal A,H,D), its metric dimension is the critical summability exponent

dimmet(D)=inf{p>0:Tr ⁣((1+D2)p/2)<},\dim_{\mathrm{met}}(D)= \inf\left\{p>0: \operatorname{Tr}\!\left((1+D^2)^{-p/2}\right)<\infty \right\},

with value ++\infty if the set is empty. Equivalently, it is the infimum of exponents for which the regularized inverse (1+D2)1/2(1+D^2)^{-1/2} belongs to the corresponding . The infimum need not be attained and need not be an integer. It depends on the spectral growth of DD, including eigenvalue multiplicities, rather than on the algebra alone.

Counting-function interpretation

Let ND(Λ)N_D(\Lambda) count eigenvalues of D|D| not exceeding Λ\Lambda, with multiplicity. Polynomial growth ND(Λ)=O(Λd)N_D(\Lambda)=O(\Lambda^d) implies summability for every p>dp>d. Under a matching two-sided Weyl asymptotic ND(Λ)CΛdN_D(\Lambda)\sim C\Lambda^d, the critical exponent equals dd, and (1+D2)1/2(1+D^2)^{-1/2} has singular values of order n1/dn^{-1/d}. It then lies at the endpoint in the Ld,\mathcal L^{d,\infty}, although generally not in Ld\mathcal L^d.

Without regular variation or comparable estimates, a critical exponent alone does not imply weak-ideal membership at the endpoint.

Canonical manifold case

For the canonical spin spectral triple of a closed dd-dimensional Riemannian spin manifold, Weyl's law gives metric dimension dd. The triple is strictly pp-summable for every p>dp>d, while d|\not D|^{-d}, with the kernel removed, is of weak trace class. This analytic dimension agrees with manifold dimension and supports the noncommutative integral Connes, Chapter VI, §1.

Rescaling DD by a nonzero constant changes metric lengths but not the critical exponent. Taking direct sums can change the dimension to the larger of the component dimensions when both have polynomial spectral growth.

Distinction from dimension spectrum

Some authors reserve “spectral dimension” for a heat-kernel scaling exponent or for the abscissa of convergence of Tr(Ds)\operatorname{Tr}(|D|^{-s}). These agree with the core under standard compact-resolvent conventions, after removing the kernel, but borderline and infinite-dimensional cases require care.

References
  1. A. Connes, Noncommutative Geometry, Academic Press, 1994. Author-hosted text. Relevant: Chapters IV and VI on infinitesimal order, summability, and the dimension of a canonical manifold triple.
  2. J. M. Gracia-Bondía, J. C. Várilly, and H. Figueroa, Elements of Noncommutative Geometry, Birkhäuser, 2001. DOI record. Relevant: §§10.1 and 10.5 on summability, spectral dimension, and zeta functions.