aiqbench analysis
This paper resolves an open problem in quantum resource theory by characterizing Flatness-Preserving Operations (FPOs) as either constant maps or specific orthogonality-preserving operations involving flat states. The work provides a rigorous mathematical framework for understanding antiflatness, distinguishing between trivial unitary evolutions and more complex isometric embeddings that maintain quantum state flatness. These findings advance the theoretical foundations necessary for manipulating non-classical resources in quantum information processing.
Flatness-Preserving Operations
arXiv:2608.30697v1 Announce Type: new Abstract: A quantum state is called flat if it is proportional to a projector. There has been recent interest in studying antiflatness, the property of diverging from flat states, and establishing a resource theory for it. Identifying the free operations (the Flatness-Preserving Operations (FPOs)) remained an open problem. For this purpose, we first discuss Orthogonality-Preserving Operations (OPOs), of which trivial examples are unitary operations in an isolated system. More generally, we give a simple proof that all OPOs are isometric embeddings consisting of combinations of unitaries/isometries and appending a fixed state. We then show that all FPOs are either constant maps to some fixed flat state or a special case of an OPO, where the appended fixed state must be a flat state. We also show that the only possible flat convex combinations of flat states are those of orthogonal flat states with weights given by their purities.
Abstract:A quantum state is called flat if it is proportional to a projector. There has been recent interest in studying antiflatness, the property of diverging from flat states, and establishing a resource theory for it. Identifying the free operations (the Flatness-Preserving Operations (FPOs)) remained an open problem. For this purpose, we first discuss Orthogonality-Preserving Operations (OPOs), of which trivial examples are unitary operations in an isolated system. More generally, we give a simple proof that all OPOs are isometric embeddings consisting of combinations of unitaries/isometries and appending a fixed state. We then show that all FPOs are either constant maps to some fixed flat state or a special case of an OPO, where the appended fixed state must be a flat state. We also show that the only possible flat convex combinations of flat states are those of orthogonal flat states with weights given by their purities.
arXiv:2608.30697 [quant-ph]
(or arXiv:2608.30697v1 [quant-ph] for this version)
https://doi.org/10.48550/arXiv.2608.30697 Focus to learn more arXiv-issued DOI via DataCite (pending registration)
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