Universal recovery maps and approximate sufficiency of quantum relative entropy
Marius Junge, Renato Renner, David Sutter, Mark M. Wilde, Andreas Winter
TL;DR
This work proves the existence of an explicit universal recovery map $\mathcal{R}_{\sigma,\mathcal{N}}$ that depends only on a reference state $\sigma$ and a quantum channel $\mathcal{N}$, providing a tight, information-theoretic remainder to the data processing inequality: $D(\rho||\sigma) \ge D(\mathcal{N}(\rho)||\mathcal{N}(\sigma)) - 2 \log F\bigl(\rho,(\mathcal{R}_{\sigma,\mathcal{N}}\circ\mathcal{N})(\rho)\bigr)$ for all $\rho$ with $\mathrm{supp}(\rho) \subseteq \mathrm{supp}(\sigma)$. The recovery map is constructed via a universal mixture of rotated Petz maps and satisfies $(\mathcal{R}_{\sigma,\mathcal{N}}\circ\mathcal{N})(\sigma)=\sigma$, establishing a robust criterion for approximate quantum error correction that is not state-dependent. The authors extend the result to infinite dimensions, derive universal refinements for strong subadditivity, concavity of conditional entropy, and joint convexity of relative entropy, and apply the framework to approximate quantum error correction, connecting information-theoretic distinguishability to recoverability with explicit fidelity-based bounds. Overall, the paper provides a powerful, universal tool for evaluating recoverability and robustness of quantum information against noise, with potential practical impact on quantum coding and fault-tolerant protocols.
Abstract
The data processing inequality states that the quantum relative entropy between two states $ρ$ and $σ$ can never increase by applying the same quantum channel $\mathcal{N}$ to both states. This inequality can be strengthened with a remainder term in the form of a distance between $ρ$ and the closest recovered state $(\mathcal{R} \circ \mathcal{N})(ρ)$, where $\mathcal{R}$ is a recovery map with the property that $σ= (\mathcal{R} \circ \mathcal{N})(σ)$. We show the existence of an explicit recovery map that is universal in the sense that it depends only on $σ$ and the quantum channel $\mathcal{N}$ to be reversed. This result gives an alternate, information-theoretic characterization of the conditions for approximate quantum error correction.
