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It should be mentioned that the quantification of entanglement for infinite-dimensional quantum systems is a subtle issue [22-24]. The minimization necessary to evaluate most measures of entanglement is typically not feasible, and without further assumptions they are not even trace-norm continuous [22]. For those two-mode Gaussian states the sequence of states converges to in the weak sense, the entanglement of formation in the infinite setting [22] is available in principle: it has been shown in [231 that for the symmetric Gaussians that we encounter here, the entanglement of formation is identical to the Gaussian entanglement of formation. For the intermediate steps this clearly does not hold, however. In this paper, we take a pragmatic approach and choose the computable logarithmic negativity as the appropriate functional that quantifies the degree of entanglement
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It should be mentioned that the quantification of entanglement for infinite-dimensional quantum systems is a subtle issue [22-24]. The minimization necessary to evaluate most measures of entanglement is typically not feasible, and without further assumptions they are not even trace-norm continuous [22]. For those two-mode Gaussian states the sequence of states converges to in the weak sense, the entanglement of formation in the infinite setting [22] is available in principle: it has been shown in [231 that for the symmetric Gaussians that we encounter here, the entanglement of formation is identical to the Gaussian entanglement of formation. For the intermediate steps this clearly does not hold, however. In this paper, we take a pragmatic approach and choose the computable logarithmic negativity as the appropriate functional that quantifies the degree of entanglement.
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i,j,k,l = 0 if i + j + k + l is an odd number, as can again be shown by induction
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i,j,k,l = 0 if i + j + k + l is an odd number, as can again be shown by induction.
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