Approximate transformations of bipartite pure-state entanglement from the majorization lattice

TL;DR

This paper introduces a new method for approximate entanglement transformations of bipartite pure states using the majorization lattice, providing a potentially optimal target state that surpasses previous fidelity-based approaches.

Contribution

The paper proposes a novel strategy for approximate entanglement transformation based on the majorization lattice, specifically using the supremum of initial and target states' Schmidt coefficients.

Findings

The proposed method often coincides with previous fidelity-based approaches in specific cases.

The strategy is effective for two-qubit pure states and entanglement concentration.

It provides a new perspective on approximate transformations beyond fidelity measures.

Abstract

We study the problem of deterministic transformations of an \textit{initial} pure entangled quantum state, $|\psi\rangle$, into a \textit{target} pure entangled quantum state, $|\phi\rangle$, by using \textit{local operations and classical communication} (LOCC). A celebrated result of Nielsen [Phys. Rev. Lett. \textbf{83}, 436 (1999)] gives the necessary and sufficient condition that makes this entanglement transformation process possible. Indeed, this process can be achieved if and only if the majorization relation $\psi \prec \phi$ holds, where $\psi$ and $\phi$ are probability vectors obtained by taking the squares of the Schmidt coefficients of the initial and target states, respectively. In general, this condition is not fulfilled. However, one can look for an \textit{approximate} entanglement transformation. Vidal \textit{et. al} [Phys. Rev. A \textbf{62}, 012304 (2000)] have proposed a deterministic transformation using LOCC in order to obtain a target state $|\chi^\mathrm{opt}\rangle$ most approximate to $|\phi\rangle$ in terms of maximal fidelity between them. Here, we show a strategy to deal with approximate entanglement transformations based on the properties of the \textit{majorization lattice}. More precisely, we propose as approximate target state one whose Schmidt coefficients are given by the supremum between $\psi$ and $\phi$. Our proposal is inspired on the observation that fidelity does not respect the majorization relation in general. Remarkably enough, we find that for some particular interesting cases, like two-qubit pure states or the entanglement concentration protocol, both proposals are coincident.