Entanglement of purification for Werner states: canonical purification and nonadditivity
Abstract
We prove that the von Neumann entanglement of purification is nonadditive. For two-qubit Werner states W(f) with singlet weight 1/64≤ f≤1/4, we show that canonical purification is globally optimal: its entanglement, also known as reflected entropy, gives the exact entanglement of purification. In contrast, the regularized entanglement of purification lies strictly below the reflected entropy for 0<f<f∗, where f∗≈0.017. Together, these results establish nonadditivity throughout 1/64≤ f<f∗. Our canonical-optimality proof generalizes the proof in [1], which established Rényi nonadditivity for 0≤α<1 using classical two-qubit states. We thus resolve the additivity question at α=1. Remarkably, nonadditivity is again witnessed by separable states and no entanglement in the underlying states is required.
Related
BibTeX
@misc{khanian2026entanglement,
title = {{Entanglement of purification for Werner states: canonical purification and nonadditivity}},
author = {Zahra Baghali Khanian and Amir-Reza Negari},
howpublished = {arXiv},
year = {2026},
month = oct,
doi = {10.48550/arxiv.2610.03630},
eprint = {2610.03630},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2610.03630},
}
RIS
TY - UNPB
TI - Entanglement of purification for Werner states: canonical purification and nonadditivity
AU - Zahra Baghali Khanian
AU - Amir-Reza Negari
PY - 2026
DA - 2026/10/02
PB - arXiv
DO - 10.48550/arxiv.2610.03630
UR - https://arxiv.org/abs/2610.03630
AB - We prove that the von Neumann entanglement of purification is nonadditive. For two-qubit Werner states W(f) with singlet weight 1/64≤ f≤1/4, we show that canonical purification is globally optimal: its entanglement, also known as reflected entropy, gives the exact entanglement of purification. In contrast, the regularized entanglement of purification lies strictly below the reflected entropy for 0<f<f_∗, where f_∗≈0.017. Together, these results establish nonadditivity throughout 1/64≤ f<f_∗. Our canonical-optimality proof generalizes the proof in [1], which established Rényi nonadditivity for 0≤α<1 using classical two-qubit states. We thus resolve the additivity question at α=1. Remarkably, nonadditivity is again witnessed by separable states and no entanglement in the underlying states is required.
ER -