Resolvent intertwining and spectral duality in Markov chains with geometric resetting
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[2608.15140] Resolvent intertwining and spectral duality in Markov chains with geometric resetting Skip to main content Search Submit Donate Log in Search arXiv Press Enter to search · Advanced search Mathematics > Probability arXiv:2608.15140 (math) [Submitted on 15 Aug 2026] Title: Resolvent intertwining and spectral duality in Markov chains with geometric resetting Authors: Juan Antonio Vega Coso View a PDF of the paper titled Resolvent intertwining and spectral duality in Markov chains with geometric resetting, by Juan Antonio Vega Coso View PDF HTML (experimental) Abstract: We uncover the resolvent origin of the spectral duality governing reset-neutral distributions in Markov chains with geometric resetting. Starting from the abstract conditions of Paper~III, we show that the spectral duality $B_\nu(z)=\kappa(z)\,A_\nu(\sigma(z))$ is equivalent to a single symmetry of the resolvent $R(\gamma)=(I-(1-\gamma)P)^{-1}$: the intertwining relation $[\Delta^2\mathcal{R},R(\gamma)]=0$, where $\mathcal{R}$ is the reflection operator of an involution $\sigma$ and $\Delta=\operatorname{diag}(\sqrt{\kappa(z)})$; equivalently, $\widetilde{\mathcal{T}}=K^{-1/2}\Delta^2\mathcal{R}$ is an involution. This symmetry determines the universal critical value $C^*=1/(1+\sqrt{K})$, with $K=\kappa(z)\kappa(\sigma(z))$, which depends only on the scalar $K$ --- not on the resetting rate $\gamma$, the reset distribution, or the particular chain. We characterize the class of $(\sigma,\kappa)$-reversible chains, encompassing both the biased random walk and genuinely non-homogeneous dynamics sharing the same $C^*$; a Doob $h$-transform realizes the duality $K\mapsto1/K$, hence $C^*\mapsto1-C^*$, with fixed point $C^*=1/2$. The orientation field admits the explicit resolvent representation $\psi(\gamma)=R(\gamma)(b^{(0)}-C^*b)$: its gauge-normalized form $\Delta^{-1}\psi(\gamma)$ is antisymmetric under $\sigma$, it has an exact node at the fixed point of $\sigma$, and it governs the exact sign law $\operatorname{sgn}(C(\pi,\gamma)-C^*) =\operatorname{sgn}\langle\pi,\psi(\gamma)\rangle$. Numerical experiments confirm the theory to machine precision. These results establish the operator-theoretic foundation of the spectral duality of Paper~III and provide the bridge to the information-geometric framework of Paper~V. Comments: 17 pages, 3 figures, 5 tables Subjects: Probability (math.PR) MSC classes: 60J10 (Primary), 60J35, 47A10 (Secondary) Cite as: arXiv:2608.15140 [math.PR] (or arXiv:2608.15140v1 [math.PR] for this version) https://doi.org/10.48550/arXiv.2608.15140 Focus to learn more arXiv-issued DOI via DataCite Submission history From: Juan Antonio Vega Coso [ view email ] [v1] Sat, 15 Aug 2026 09:31:30 UTC (30 KB) Full-text links: Access Paper: View a PDF of the paper titled Resolvent intertwining and spectral duality in Markov chains with geometric resetting, by Juan Antonio Vega Coso View PDF HTML (experimental) TeX Source view license Current browse context: math.PR < prev | next > new | recent | 2026-08 Change to browse by: math References & Citations NASA ADS Google Scholar Semantic Scholar export BibTeX citation Loading... BibTeX formatted citation × loading... 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