bibkey: chen2020mpdoparent authors: Chi-Fang Chen, Kohtaro Kato and Fernando G. S. L. Brandão year: 2020 title: “Matrix Product Density Operators: when do they have a local parent Hamiltonian?” doi: null url: https://arxiv.org/abs/2010.14682v3 claim: “Conjecture III.1 asserts a uniform completely contractive data-processing bound for conditional mutual information under every channel with scalar whole-space correctable algebra. Conjecture III.2 asserts the analogous uniform bound for the trace-norm CMI of Definition 2 under every channel with local trace-norm contraction ratio below one.” strata_touched:
- D5/S3/Quantum/Information/ChenKatoBrandaoCMIRefutation
- D5/S3/Quantum/Information/ChenKatoBrandaoTraceNormCMIRefutation license: citation-only triage: anchor
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Source: https://arxiv.org/abs/2010.14682v3
The arXiv abstract page lists the arXiv-issued DOI https://doi.org/10.48550/arXiv.2010.14682 and no published journal DOI. Version 3 is the source version. Section II.D, PDF p. 11, equation (22) defines the correctable algebra. Section III.C, PDF p. 16, contains Proposition III.3 and Conjecture III.1; Proposition III.4 follows on p. 17.
The correctable-algebra definition reads:
For a given channel , we define the correctable algebra as .
Conjecture III.1 reads:
For any channel with trivial correctable algebra , there exists a constant such that for any tripartite system and any state , it holds that .
Proposition III.3 reads:
Let be a CPTP map which has trivial correctable algebra. Consider a tripartite system . Then, for any state with , we have .
Section I, PDF p. 3, equation (1) reads:
The CMI is a function defined for a tripartite state as , where is the von Neumann entropy of the reduced state on .
Definition 2 (Section III.A.1, PDF p. 14) reads:
Conjecture III.2 (Section III.C, PDF p. 17) reads:
For any channel with local contraction ratio There exists a global constant such that for any tripartite system and any state , it holds that .
It is followed by: “We do not know if extra constants or factor of dimension should be present between and like the crude bound in Theorem III.2.”
The source’s Proposition III.4 is conditional on Conjecture III.1. A refutation of that conjecture removes this route to unconditional decay; it does not refute exponential decay for every Y-shaped MPDO.
Bény, Kempf and Kribs, Quantum Error Correction of Observables, https://arxiv.org/abs/0705.1574, DOI https://doi.org/10.1103/PhysRevA.76.042303, Theorem 9, supplies the support-sensitive criterion for correctability on a projected support. The support projection is part of that criterion; a correctable observable on a chosen support need not be correctable on the whole input space. This distinguishes recovery of selected preparations from the whole-space algebra in equation (22).