Von Neumann entropy and majorization
arXiv:1304.7442 · doi:10.1016/j.jmaa.2013.06.019
Abstract
We consider the properties of the Shannon entropy for two probability distributions which stand in the relationship of majorization. Then we give a generalization of a theorem due to Uhlmann, extending it to infinite dimensional Hilbert spaces. Finally we show that for any quantum channel $Φ$, one has $S(Φ(Ï))=S(Ï)$ for all quantum states $Ï$ if and only if there exists an isometric operator $V$ such that $Φ(Ï)=VÏV^*$.
Version 2 contains some corrections and linguistic improvements