Dimension\-Open Trace Witnesses Admit Exact Classical Memory Simulations

A common self-consistent channel diagnostic uses a reference contrast matrix R and a processed contrast matrix P. Under a fixed d-dimensional carrier, a common preparation/readout interface, and an invertible reference, one obtains W = Tr(P R^{-1}) = Tr T, where T is the transfer block on the d^2 − 1 traceless operator coordinates. Every entanglement-breaking d-dimensional channel obeys W ≤ d − 1. The inequality is useful only if the dimension and interface assumptions are part of the experimental contract. We construct an exact countermodel when they are not. For every d ≥ 2, set m = d^2 − 1 and let n_1, …, n_{m+1} be the vertices of a regular simplex in R^m. An affine encoding of a local m-dimensional signal ball into the m + 1 = d^2 classical simplex, paired with binary linear readouts, gives an invertible isotropic contrast matrix R = β I_m. The stochastic memory transition K_q = q I_{m+1} + (1 − q) 11^T/(m+1), 0 ≤ q ≤ 1, acts as r ↦ q r on the encoded local chart. Hence for every depth n the observed contrasts satisfy P_n = q^n R, all semigroup identities P_{n+k} = P_n R^{-1} P_k, and the apparent transfer spectrum is exactly that of the d-dimensional depolarizing channel. Yet the physical realization is a measure-and-prepare channel on a d^2-state classical memory and is therefore entanglement breaking for every q. A naive d-dimensional trace witness returns W = (d^2 − 1)q, which exceeds the legitimate entanglement-breaking threshold d − 1 whenever q > 1/(d + 1). At q = 1 the apparent violation factor is d + 1 although the physical memory is classical. Under affine mixture-preserving encodings, d^2 classical states are also minimal for faithfully representing an open (d^2 − 1)-dimensional interface chart. The result does not contradict valid dimension witnesses or trusted-input quantum-memory tests. It identifies a precise failure mode of transferring a dimension-conditioned trace certificate outside its interface contract: repetition consistency, spectral consistency, and arbitrarily deep Markov consistency do not by themselves recover the missing dimension assumption.

Authors

Publication Details

Journal
Zenodo (CERN European Organization for Nuclear Research)
Published
2026-09-29
DOI
https://doi.org/10.5281/zenodo.23044559
Primary Topic
Quantum Information and Cryptography
Type
preprint
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preprint

Dimension\-Open Trace Witnesses Admit Exact Classical Memory Simulations

Oliver Tuma
Zenodo (CERN European Organization for Nuclear Research)
Quantum Information and Cryptography
preprint

Dimension\-Open Trace Witnesses Admit Exact Classical Memory Simulations

Oliver Tuma
preprint en

Abstract

A common self-consistent channel diagnostic uses a reference contrast matrix R and a processed contrast matrix P. Under a fixed d-dimensional carrier, a common preparation/readout interface, and an invertible reference, one obtains W = Tr(P R^{-1}) = Tr T, where T is the transfer block on the d^2 − 1 traceless operator coordinates. Every entanglement-breaking d-dimensional channel obeys W ≤ d − 1. The inequality is useful only if the dimension and interface assumptions are part of the experimental contract. We construct an exact countermodel when they are not. For every d ≥ 2, set m = d^2 − 1 and let n_1, …, n_{m+1} be the vertices of a regular simplex in R^m. An affine encoding of a local m-dimensional signal ball into the m + 1 = d^2 classical simplex, paired with binary linear readouts, gives an invertible isotropic contrast matrix R = β I_m. The stochastic memory transition K_q = q I_{m+1} + (1 − q) 11^T/(m+1), 0 ≤ q ≤ 1, acts as r ↦ q r on the encoded local chart. Hence for every depth n the observed contrasts satisfy P_n = q^n R, all semigroup identities P_{n+k} = P_n R^{-1} P_k, and the apparent transfer spectrum is exactly that of the d-dimensional depolarizing channel. Yet the physical realization is a measure-and-prepare channel on a d^2-state classical memory and is therefore entanglement breaking for every q. A naive d-dimensional trace witness returns W = (d^2 − 1)q, which exceeds the legitimate entanglement-breaking threshold d − 1 whenever q > 1/(d + 1). At q = 1 the apparent violation factor is d + 1 although the physical memory is classical. Under affine mixture-preserving encodings, d^2 classical states are also minimal for faithfully representing an open (d^2 − 1)-dimensional interface chart. The result does not contradict valid dimension witnesses or trusted-input quantum-memory tests. It identifies a precise failure mode of transferring a dimension-conditioned trace certificate outside its interface contract: repetition consistency, spectral consistency, and arbitrarily deep Markov consistency do not by themselves recover the missing dimension assumption.

Zenodo (CERN European Organization for Nuclear Research)
Peace, Justice and strong institutions
Quantum Information and Cryptography
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Dimension\-Open Trace Witnesses Admit Exact Classical Memory Simulations — Oliver Tuma · Zenodo (CERN European Organization for Nuclear Research) (2026) | TGRS Research Map | TGRS