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Why Random-Matching Markov Chains Resist a Spectral Bridge to the Riemann Hypothesis: An Exploratory Assessment

This essay examines the reversible Markov chain governing Pauli-weight diffusion in the shallow random Clifford circuits of Anand et al. (2026).

Abstract

This essay examines the reversible Markov chain governing Pauli-weight diffusion in the shallow random Clifford circuits of Anand et al. (2026).


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The Source Structure

Anand, Gorokhovsky, Hritz, and Sun study random Clifford circuits built from random perfect matchings on n qubits. Their key technical tool is a reduction of the second-moment dynamics of these circuits to a reversible Markov chain on binary support strings (the “Pauli weight chain”). The chain has a stationary distribution π(w) ∝ 3w (n choose w) and exhibits logarithmic hitting-time bounds. The transition operator is self-adjoint with respect to the inner product weighted by π.

The Proposed Analogy

The Hilbert–Pólya conjecture posits that the non-trivial zeros of the Riemann zeta function correspond to the eigenvalues of a self-adjoint operator on an infinite-dimensional Hilbert space. Because the Pauli-weight chain is defined by a self-adjoint (reversible) transition matrix, it superficially invites comparison: both involve spectra of self-adjoint operators, and both are studied via their spectral gaps and level statistics.

Assessment of the Bridge

We rate this correspondence a suggestive metaphor. While the property of self-adjointness provides a formal similarity, the disanalogies are severe: the Markov chain acts on a finite state space, lacks any functional equation or Euler product, and possesses a spectral gap incompatible with the unbounded accumulation of zeta zeros. We propose testing whether the finite-chain eigenvalue spacing nevertheless mimics the GUE statistics observed in the zeta zeros; a negative result would definitively refute the bridge.

This essay was produced by an automated research pipeline and has not been peer reviewed; conjectures herein are unproven.

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