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This research introduces a quantitative witness to distinguish genuine tripartite entanglement from biseparable states using measurable Pauli correlations, offering a rigorous tool for characterizing GHZ-type quantum resources. By establishing strict bounds that separate the GHZ state from W states and separable mixtures, the work provides a concrete metric for verifying high-fidelity multipartite entanglement in experimental setups. This advancement is critical for scaling quantum networks and fault-tolerant architectures where distinguishing true global correlations from local noise is essential.
A measure for genuine tripartite entanglement
arXiv:2605.02876v3 Announce Type: replace Abstract: We introduce a real-valued functional $I(\vec{n}_1,\vec{n}_2)$ of four three-qubit correlation expectation values that turns the Greenberger--Horne--Zeilinger (GHZ) algebraic paradox into a quantitative witness of genuine tripartite entanglement. We prove that $|I(\vec{n}_1,\vec{n}_2;\rho)|\le 2$ for all three-qubit states $\rho$ and all direction pairs, with equality if and only if $\vec{n}_1\perp \vec{n}_2$ and $\rho$ is locally unitarily (LU) equivalent to the GHZ state. We obtain a closed-form $I(\hat{x},\hat{y})$ on the five-parameter Ac\'in canonical family of three-qubit pure states; it depends only on $\lambda_0\lambda_4$ and is maximised at $\lambda_0=\lambda_4 =1/\sqrt{2}$. For the W state, $I(\hat{x},\hat{y})=0$ and $\max_{\vec{n}_1,\vec{n}_2}|I_{\mathrm{W}}|=35/27\approx 1.296$, strictly below the GHZ value. Maximising the underlying correlation structure over independent local orthonormal frames yields a manifestly LU-invariant quantity $\mathcal{E}_{\mathrm{GHZ}}(\rho)\in[0,1]$ that equals one if and only if $\rho$ is LU equivalent to the GHZ state, equals $35/54\approx0.648$ on the W state, and is bounded by $1/2$ on all biseparable and fully separable states; it is therefore a local-frame-independent indicator of GHZ-type genuine tripartite correlation, obtainable from four Pauli correlators. We relate $\mathcal{E}_{\mathrm{GHZ}}$ to GHZ fidelity witnesses, analyse its behaviour under local operations and classical communication, and delimit what it does and does not certify about genuine tripartite nonlocality, stating which properties are proven and which (notably global convexity and the resulting genuine-multipartite-entanglement witness threshold) are established numerically and remain open analytically. We also outline a generalisation of $I$ to three-qudit systems built from Heisenberg--Weyl operators, recovering the standard qubit construction at $d=2$.
Abstract:We introduce a real-valued functional $I(\vec{n}_1,\vec{n}_2)$ of four three-qubit correlation expectation values that turns the Greenberger--Horne--Zeilinger (GHZ) algebraic paradox into a quantitative witness of genuine tripartite entanglement. We prove that $|I(\vec{n}_1,\vec{n}_2;\rho)|\le 2$ for all three-qubit states $\rho$ and all direction pairs, with equality if and only if $\vec{n}_1\perp \vec{n}_2$ and $\rho$ is locally unitarily (LU) equivalent to the GHZ state. We obtain a closed-form $I(\hat{x},\hat{y})$ on the five-parameter Acín canonical family of three-qubit pure states; it depends only on $\lambda_0\lambda_4$ and is maximised at $\lambda_0=\lambda_4 =1/\sqrt{2}$. For the W state, $I(\hat{x},\hat{y})=0$ and $\max_{\vec{n}_1,\vec{n}_2}|I_{\mathrm{W}}|=35/27\approx 1.296$, strictly below the GHZ value. Maximising the underlying correlation structure over independent local orthonormal frames yields a manifestly LU-invariant quantity $\mathcal{E}_{\mathrm{GHZ}}(\rho)\in[0,1]$ that equals one if and only if $\rho$ is LU equivalent to the GHZ state, equals $35/54\approx0.648$ on the W state, and is bounded by $1/2$ on all biseparable and fully separable states; it is therefore a local-frame-independent indicator of GHZ-type genuine tripartite correlation, obtainable from four Pauli correlators. We relate $\mathcal{E}_{\mathrm{GHZ}}$ to GHZ fidelity witnesses, analyse its behaviour under local operations and classical communication, and delimit what it does and does not certify about genuine tripartite nonlocality, stating which properties are proven and which (notably global convexity and the resulting genuine-multipartite-entanglement witness threshold) are established numerically and remain open analytically. We also outline a generalisation of $I$ to three-qudit systems built from Heisenberg--Weyl operators, recovering the standard qubit construction at $d=2$.
arXiv:2605.02876 [quant-ph]
(or arXiv:2605.02876v3 [quant-ph] for this version)
https://doi.org/10.48550/arXiv.2605.02876 Focus to learn more arXiv-issued DOI via DataCite
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