Adelic Dirac–Hilbert–Pólya conjecture for the Riemann zeros

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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

∑p∥ηp∥∞<∞\sum_p\|\eta_p\|_\infty<\infty

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

∑k(δ(λ−γk)−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.

References

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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