(30) The overlap between the states is given by c = |⟨φ|ψ ⟩|= |⟨φ 1|ψ 1⟩ ⟨φ 2|ψ 2⟩|=r1r2, (31) where we denote |⟨φj|ψj⟩|=rj and demand that r1r2 = c

Separable case Here we derive the two-state operator norm ∥B∥TS, c,s with the constraint that both pre-, post-selected states are separable, namely |φ⟩ = |φ 1⟩ ⊗ |φ 2⟩, |ψ ⟩ = |

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Quantum nonlocal correlations of anomalous weak values

quant-ph · 2026-07-01 · unverdicted · novelty 7.0

Post-selection enhances CHSH correlations in PPS ensembles but entanglement is required to exceed separable PPS bounds, enabling constructive post-selected entanglement witnesses for pure two-qubit states.

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Quantum nonlocal correlations of anomalous weak values quant-ph · 2026-07-01 · unverdicted · none · ref 5
Post-selection enhances CHSH correlations in PPS ensembles but entanglement is required to exceed separable PPS bounds, enabling constructive post-selected entanglement witnesses for pure two-qubit states.

(30) The overlap between the states is given by c = |⟨φ|ψ ⟩|= |⟨φ 1|ψ 1⟩ ⟨φ 2|ψ 2⟩|=r1r2, (31) where we denote |⟨φj|ψj⟩|=rj and demand that r1r2 = c

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