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Let the ancillary state beβ= diag(p,1−p) and the two–qubit dilation UAD(γ) =   1 0 0 0 0 √1−γ √γ0 0− √γ √1−γ0 0 0 0 1   ,E 0(ρ) = TrB UAD(γ) (ρ⊗β)U AD(γ)†

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