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(37d) The single-parameter two-qubit EJM is defined as Jκ = {|Φκ j ⟩ ⟨Φκ j | : j = 0, 1, 2, 3}

Define four orthonormal states [ 54]: |Φκ 0⟩ = 1 2 e− iπ 4 |00⟩ − rκ +|01⟩ − rκ −|10⟩ + e− 3iπ 4 |11⟩ , (37a) |Φκ 1⟩ = 1 2 e iπ 4 |00⟩ + rκ −|01⟩ + rκ +|10⟩ + e 3iπ 4 |11⟩ , (37b) |Φκ 2⟩ = 1 2 e− 3iπ 4 |00⟩ + rκ −|01⟩ + rκ +|10⟩ + e− iπ 4 | · 2025

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Efficient Verification of Entangled Measurements with Local States

quant-ph · 2026-06-19 · unverdicted · novelty 7.0

A symmetry reduction for locally transitive projective measurements turns entangled measurement verification into single-state verification, yielding explicit local protocols and fidelity estimators for Bell, stabilizer, and other measurements.

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  • Efficient Verification of Entangled Measurements with Local States quant-ph · 2026-06-19 · unverdicted · none · ref 4

    A symmetry reduction for locally transitive projective measurements turns entangled measurement verification into single-state verification, yielding explicit local protocols and fidelity estimators for Bell, stabilizer, and other measurements.