Definition

Let (A,H,D)(\mathcal A,H,D) be a . Write Ds|D|^{-s} for the complex power that is zero on kerD\ker D and equals λs\lambda^{-s} on the positive spectral value λ\lambda. The spectral zeta function is

ζD(s)=Tr(Ds)\zeta_D(s)=\operatorname{Tr}(|D|^{-s})

at those sCs\in\mathbb C for which Ds|D|^{-s} is trace class, using the . More generally, for a bounded operator bb, the weighted spectral zeta function is ζb(s)=Tr(bDs)\zeta_b(s)=\operatorname{Tr}(b|D|^{-s}) wherever the product is trace class. Meromorphic continuations, when they exist, are continuations of these initially convergent functions.

Convergence and spectral growth

If the nonzero eigenvalues of D|D|, repeated with multiplicity, are λ1λ2\lambda_1\leq\lambda_2\leq\cdots, then

ζD(s)=nλns\zeta_D(s)=\sum_{n}\lambda_n^{-s}

in its half-plane of absolute convergence. Thus the convergence abscissa measures eigenvalue growth. Finite-dimensional kernels do not affect that growth, but the convention on kerD\ker D must be fixed before negative powers are written.

Heat-kernel relation

For Res\operatorname{Re}s sufficiently large, Mellin transformation gives

Γ(s/2)ζD(s)=0ts/21Tr ⁣(etD2PkerD)dt.\Gamma(s/2)\zeta_D(s) =\int_0^\infty t^{s/2-1} \operatorname{Tr}\!\left(e^{-tD^2}-P_{\ker D}\right)\,dt.

This relation connects small-time heat asymptotics with poles and residues of the zeta function. Under regularity and suitable asymptotic hypotheses, weighted zeta functions are the analytic input for the dimension spectrum and local index formula Connes–Moscovici, §II.

Conventions and scope
References
  1. A. Connes and H. Moscovici, “The Local Index Formula in Noncommutative Geometry,” Geometric and Functional Analysis 5 (1995), 174–243. DOI record. Relevant: §II on zeta functions, residues, and dimension spectrum.
  2. J. M. Gracia-Bondía, J. C. Várilly, and H. Figueroa, Elements of Noncommutative Geometry, Birkhäuser, 2001. Publisher record. Relevant: §10.5 on spectral dimension and zeta functions.