
doi: 10.1007/bf01212339
For \({\mathcal A}\) any subset of \({\mathcal B}({\mathcal H})\) (the bounded operators on a Hilbert space) containing the unit, and \(\sigma\) and \(\rho\) restrictions of states on \({\mathcal B}({\mathcal H})\) to \({\mathcal A}\), \(ent_{{\mathcal A}}(\sigma | \rho)\)- the entropy of \(\sigma\) relative to \(\rho\) given the information in \({\mathcal A}\)- is defined and given an axiomatic characterisation. It is compared with \(ent^ S_{{\mathcal A}}(\sigma | \rho)\)- the relative entropy introduced by Umegaki and generalised by various authors - which is defined only for \({\mathcal A}\) an algebra. It is proved that ent and \(ent^ S\) agree on pairs of normal states on an injective von Neumann algebra. It is also proved that ent always has all the most important properties known for \(ent^ S:\) monotonicity, concavity, \(w^*\) upper semicontinuity, etc. It is shown, as an extension of the property of semi-discreteness, that a von Neumann algebra (\({\mathcal A},{\mathcal H})\) is injective if and only if there exists a net \((\lambda_{\alpha})_{\alpha \in I}\) of normal completely positive finite rank maps \(\lambda_{\alpha}:{\mathcal B}({\mathcal H})\to {\mathcal A}\) such that \(\lambda_{\alpha}(1)=1\) and such that \(\lambda_{\alpha | {\mathcal A}}\) tends to the identity map on \({\mathcal A}\) in the topology of simple \(w^*\) convergence.
normal states on an injective von Neumann algebra, Applications of selfadjoint operator algebras to physics, relative entropy, 46L50, 82A15, 46L30, Classical equilibrium statistical mechanics (general), Noncommutative dynamical systems
normal states on an injective von Neumann algebra, Applications of selfadjoint operator algebras to physics, relative entropy, 46L50, 82A15, 46L30, Classical equilibrium statistical mechanics (general), Noncommutative dynamical systems
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