Adelic Dirac–Hilbert–Pólya conjecture for the Riemann zeros

Let (Darith,{ηp})(\mathcal{D}_{\mathrm{arith}},\{\eta_p\}) be a chiral adelic Dirac system, where the coefficient functions ηp\eta_p are even, and let ξDirac\xi_{\mathrm{Dirac}} denote its spectral shift function. The nontrivial zeros of ζ(s)\zeta(s) have imaginary parts γk\gamma_k. Adelic Dirac–Hilbert–Pólya conjecture. There exist even coefficient functions ηp\eta_p satisfying

pηp<\sum_p\|\eta_p\|_\infty<\infty

such that ξDirac\xi_{\mathrm{Dirac}}, after affine rescaling, reproduces the signed zero-counting measure

k(δ(λγk)δ(λ+γk))\sum_k\bigl(\delta(\lambda-\gamma_k)-\delta(\lambda+\gamma_k)\bigr)

for the nontrivial zeros of ζ(s)\zeta(s). This is a chiral adelic analogue of the Hilbert–Pólya idea: the zeros are encoded by jump discontinuities of a spectral shift function rather than appearing directly as the spectrum of a self-adjoint Hamiltonian. The supplied text gives no resolution, so the conjecture remains open.

Sources & referencesView supporting material

Primary source

James C. Hateley, “A Chiral Adelic Dirac Operator and the Spectral Realization of the Riemann Zeros”, arXiv:2511.18309 (2025).

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