Destroying and Preserving Measurement Incompatibility over a Quantum Channel
quant-ph
Submitted: 2026-10-05
Updated: 2026-10-05
License: http://creativecommons.org/licenses/by/4.0/
The gist: A quantum channel is called incompatibility-breaking if it always destroys the incompatibility of quantum measurements.
Abstract
A quantum channel is called incompatibility-breaking if it always destroys the incompatibility of quantum measurements. On the other extreme are incompatibility-preserving channels, which never destroy incompatibility. This work studies both types of channels through the mathematical framework of zonotopes and zonoids, an approach that provides a complete characterization of compatibility for dichotomic measurements and is particularly powerful in the qubit setting. Using the language of zonoids, we present necessary and sufficient conditions for when a qubit unital channel is incompatibility-breaking, which are also sufficient for nonunital channels. As one of our main results, we demonstrate the superactivation phenomenon of two incompatibility-breaking qubit channels that are no longer incompatibility-breaking when used in parallel. Translating this result into the task of quantum steering, it says that two copies of a two-qubit Werner state can be steered at noise threshold 1/2, even though this is impossible using just one copy. For the problem of incompatibility preservation, we prove that a quantum channel with matching input and output dimensions will preserve general incompatibility if and only if it is a unitary transformation. When the output dimension is larger, this result no longer holds, and we offer a conjectured form of a general incompatibility-preserving channel.
Sources
- Network nonlocality breaking channels
- Compatibility of quantum instruments
- Quantum ensembles as waves on state space
- One pure steered state implies Einstein-Podolsky-Rosen steering
- Quantum contextuality and joint measurement of three observables of a qubit
- A universal set of qubit quantum channels
- Continuous coexistency preservers on effect algebras
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