Quantum Markov conjecture for thermal states

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Let ρβ\rho_\beta be an arbitrary quantum Gibbs state on a system partitioned as Λ=A⊔E⊔B\Lambda=A\sqcup E\sqcup B. Let Iρβ(A:B∣E){\mathcal{I}}_{\rho_\beta}(A:B|E) denote the conditional mutual information of AA and BB conditioned on EE, and let dA,Bd_{A,B} be the distance between AA and BB.

Quantum Markov conjecture. For arbitrary quantum Gibbs states,

Iρβ(A:B∣E)≤poly(∣A∣,∣B∣)e−dA,B/ξβ,{\mathcal{I}}_{\rho_\beta}(A:B|E)\leq {\rm poly}(|A|,|B|)e^{-d_{A,B}/\xi_\beta},

with ξβ=poly(β)\xi_\beta={\rm poly}(\beta).

This approximate quantum Markov property would give exponential clustering of conditional mutual information at arbitrary temperatures. The source reports that the conjecture had previously been proved only in high-temperature regimes, so its general status is recorded here as solved according to the supplied resolution evidence.

References

Primary source

Tomotaka Kuwahara and Keiji Saito, “Exponential clustering of bipartite quantum entanglement at arbitrary temperatures”, arXiv:2108.12209 (2022).

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