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This research establishes a holographic duality linking steady states of quantum channels to boundary mixed-state orders in higher-dimensional topological systems. By utilizing isometric tensor network states, the study maps spontaneous symmetry breaking phenomena to anyon condensation, offering new theoretical tools for analyzing mixed-state phases. The work advances fundamental understanding of quantum information geometry and topological order without immediate product applications.
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Holographic duality between bulk topological order and boundary mixed-state order

arXiv2 min read

arXiv:2511.19597v2 Announce Type: replace Abstract: We introduce a holographic framework for analyzing the steady states of repeated quantum channels with strong symmetries. Using channel-state duality, we show that the steady state of a $d$-dimensional quantum channel is holographically mapped to the boundary reduced density matrix of a $(d+1)$-dimensional wavefunction generated by a sequential unitary circuit. From this perspective, strong-to-weak spontaneous symmetry breaking (SWSSB) in the steady state arises from the anyon condensation on the boundary of a topological order in one higher dimension. The conditional mutual information (CMI) associated with SWSSB is then inherited from the bulk topological entanglement entropy. We make this duality explicit using isometric tensor network states (isoTNS) by identifying the channel's time evolution with the transfer matrix of a higher-dimensional isoTNS. Built on isoTNS, we further construct continuously tunable quantum channels that exhibit distinct mixed-state phases and transitions in the steady states.

Abstract:We introduce a holographic framework for analyzing the steady states of repeated quantum channels with strong symmetries. Using channel-state duality, we show that the steady state of a $d$-dimensional quantum channel is holographically mapped to the boundary reduced density matrix of a $(d+1)$-dimensional wavefunction generated by a sequential unitary circuit. From this perspective, strong-to-weak spontaneous symmetry breaking (SWSSB) in the steady state arises from the anyon condensation on the boundary of a topological order in one higher dimension. The conditional mutual information (CMI) associated with SWSSB is then inherited from the bulk topological entanglement entropy. We make this duality explicit using isometric tensor network states (isoTNS) by identifying the channel's time evolution with the transfer matrix of a higher-dimensional isoTNS. Built on isoTNS, we further construct continuously tunable quantum channels that exhibit distinct mixed-state phases and transitions in the steady states.

Quantum Physics (quant-ph); Statistical Mechanics (cond-mat.stat-mech); Strongly Correlated Electrons (cond-mat.str-el)

arXiv:2511.19597 [quant-ph]

(or arXiv:2511.19597v2 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2511.19597 Focus to learn more arXiv-issued DOI via DataCite

https://doi.org/10.1103/lrqp-pnl1 Focus to learn more DOI(s) linking to related resources

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