Abstract
In this chapter we discuss entanglement in a general setting and we review some quantitative measures of entanglement and their properties.
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Notes
- 1.
The general case is unclear to us, but one could modify the definition to make the set of separable states norm-closed.
- 2.
Here the tensor product \(M_N(\mathbb {C}) \otimes \mathfrak {A}_2\) is algebraic, with no completion required. To obtain the (unique) \(C^*\)-norm, one may use the fact that there exists a universal representation \(\pi _u:\mathfrak {A}_2\rightarrow \mathfrak {B}(\mathcal {H}_u)\), which is faithful and hence isometric. One may then represent \(M_N(\mathbb {C}) \otimes \mathfrak {A}_2\) on \(\mathbb {C}^N\otimes \mathcal {H}_u\) and use the operator norm.
- 3.
We thank Marc M. Wilde for pointing out this reference to us.
- 4.
Actually, this is all that is needed in order to define \(E_M\).
- 5.
- 6.
- 7.
A function \(f: \mathbb {R}\rightarrow \mathbb {R}\) is called operator monotone if \(f(A) \le f(B)\) whenever two self-adjoint operators A, B on a Hilbert space \(\mathcal {H}\) satisfy \(A \le B\) on the form domain of B. If \(A=B\) on the form domain of B we obtain \(f(A)\le f(B)\). Notice especially the asymmetry in the assumption on the form domain.
- 8.
We may always pass to a new protocol whose rate is arbitrarily close, so that the \(\limsup \) is actually a \(\lim \).
- 9.
We even get the statement for the “asymptotic” relative entropy of entanglement defined by \(E_R^\infty (\omega ) = \lim _{n \rightarrow \infty } \frac{1}{n} E_R(\omega ^{\otimes n})\). Note that the limit exists: Use (e5) and Lemma 12 of [25].
- 10.
Property (e4) for \(E_M\) has been proven only in a restricted sense, and instead of (e3) we have the opposite: concavity \(\overline{\mathrm{(e3)}}\).
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Hollands, S., Sanders, K. (2018). Entanglement Measures in QFT. In: Entanglement Measures and Their Properties in Quantum Field Theory. SpringerBriefs in Mathematical Physics, vol 34. Springer, Cham. https://doi.org/10.1007/978-3-319-94902-4_3
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