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Why Quantum Walk Splitting Probabilities Resist a Hilbert-Pólya Bridge to the Riemann Hypothesis: An Honest Assessment

This essay explores a speculative structural correspondence between the phase transition in splitting probabilities of monitored quantum walks on finite lattices, recently analyzed by Singh, Kessler, and Barkai, and the Hilbert-Pólya spectral interpretation of the Riemann Hypothesis.

Abstract

This essay explores a speculative structural correspondence between the phase transition in splitting probabilities of monitored quantum walks on finite lattices, recently analyzed by Singh, Kessler, and Barkai, and the Hilbert-Pólya spectral interpretation of the Riemann Hypothesis.


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Quantum Walks and Spectral Phase Transitions

The source paper investigates a monitored continuous-time quantum walk on a finite one-dimensional tight-binding lattice with two absorbing targets. The splitting probability—the probability of detection at the left target before the right—exhibits a nonanalytic, phase-transition-like behavior at a critical sampling time τ_c = 2π/ΔE, where ΔE is the energy bandwidth. For τ < τ_c, the splitting probability is universally 1/2, independent of the initial condition; for τ > τ_c, it develops non-universal fluctuations and resonant peaks.

The Hilbert-Pólya Resonance

We attempted to construct a dictionary mapping this structure onto the Hilbert-Pólya conjecture, which seeks a self-adjoint operator whose eigenvalues are the imaginary parts of the Riemann zeta zeros. The decomposition of the quantum walk into symmetric and antisymmetric parity sectors (using auxiliary states |d_±⟩) superficially resembles the symmetry of the Riemann ξ-function under s ↔ 1−s. The critical time τ_c suggests a spectral scale that might analogously govern the distribution of zeta zeros.

Structural Failure of the Analogy

The analogy collapses at the level of spectral geometry. The tight-binding Hamiltonian has a bounded, finite spectrum within [−2γ, 2γ], while the Hilbert-Pólya operator must have an unbounded, infinite spectrum with eigenvalues tending to infinity. Consequently, the critical time τ_c—fixed by the bandwidth—has no counterpart in the zeta zero distribution, where the mean level spacing decays as 2π/log T. Furthermore, the spectral statistics are incompatible: the integrable tight-binding model exhibits Poisson level spacing, whereas zeta zeros follow Gaussian Unitary Ensemble (GUE) statistics.

Assessment

This is an honest negative result. The quantum walk structure, while mathematically elegant, does not provide a viable bridge to the Riemann Hypothesis. A viable quantum mechanical analogy would require an unbounded operator with the appropriate spectral asymptotics and random matrix universality.

This essay was produced by an automated research pipeline and has not been peer reviewed; conjectures herein are unproven.

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