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Research PaperResearchia:202605.23055

Self-testing of exact entanglement embezzlement

Samuel J. Harris

Abstract

We consider bipartite exact entanglement embezzlement with a catalyst state vector $ψ$ in a Hilbert space $\mathcal{H}$ using unitaries (or more generally, contractions). If $\mathcal{M} \subseteq \mathcal{B}(\mathcal{H})$ is a von Neumann algebra and $U \in M_d \otimes \mathcal{M}$ and $V \in \mathcal{M}' \otimes M_d$ are unitaries (or more generally contractions), then such a protocol is of the form $(U \otimes I_d)(I_d \otimes V)(e_0 \otimes ψ\otimes e_0)=\sum_{i=0}^{d-1} α_i e_i \otimes ψ\ot...

Submitted: May 23, 2026Subjects: Quantum Physics; Quantum Computing

Description / Details

We consider bipartite exact entanglement embezzlement with a catalyst state vector ψψ in a Hilbert space H\mathcal{H} using unitaries (or more generally, contractions). If MβŠ†B(H)\mathcal{M} \subseteq \mathcal{B}(\mathcal{H}) is a von Neumann algebra and U∈MdβŠ—MU \in M_d \otimes \mathcal{M} and V∈Mβ€²βŠ—MdV \in \mathcal{M}' \otimes M_d are unitaries (or more generally contractions), then such a protocol is of the form (UβŠ—Id)(IdβŠ—V)(e0βŠ—ΟˆβŠ—e0)=βˆ‘i=0dβˆ’1Ξ±ieiβŠ—ΟˆβŠ—ei(U \otimes I_d)(I_d \otimes V)(e_0 \otimes ψ\otimes e_0)=\sum_{i=0}^{d-1} Ξ±_i e_i \otimes ψ\otimes e_i, where each Ξ±i>0Ξ±_i>0 and βˆ‘i=0dβˆ’1Ξ±i2=1\sum_{i=0}^{d-1} Ξ±_i^2=1. We show that any such protocol must arise from a unique state on the tensor product OdβŠ—Od\mathcal{O}_d \otimes \mathcal{O}_d of the Cuntz algebra with itself. As a result, we prove that exact entanglement embezzlement is a self-test for a collection of dd Cuntz isometries for each party and a unique quasi-free state on the Cuntz algebra Od\mathcal{O}_d in the sense of \cite{Iz93}. Moreover, we use modular theory to show that the von Neumann algebra generated by the copy of Od\mathcal{O}_d is the unique separable approximately finite-dimensional Type IIIΞ»\text{III}_Ξ» factor for some 0<λ≀10<Ξ»\leq 1, where λλ can be determined by an algebraic condition on the Schmidt coefficients of the state Ο†=βˆ‘i=0dβˆ’1Ξ±ieiβŠ—ei\varphi=\sum_{i=0}^{d-1} Ξ±_i e_i \otimes e_i.


Source: arXiv:2605.22713v1 - http://arxiv.org/abs/2605.22713v1 PDF: https://arxiv.org/pdf/2605.22713v1 Original Link: http://arxiv.org/abs/2605.22713v1

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Date:
May 23, 2026
Topic:
Quantum Computing
Area:
Quantum Physics
Comments:
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