Abstract

Let (X,μ)({\cal X},μ) be a measure space. For any measurable set Y⊂XY\subset{\cal X} let 1Y:X→R1_Y : {\cal X}\to{\mathbb R} be the indicator of YY and let πYπ_Y be the orthogonal projector L2(X)∋f↦πYf=1YfL^2({\cal X})\ni f\mapstoπ_Y f = 1_Y f. For any bounded operator WW on L2(X,μ)L^2({\cal X},μ) we define its μμ-norm ∥W∥μ=inf⁡χ∑μ(Yj)∥WπY∥2\|W\|_μ= \inf_χ\sqrt{\sum μ(Y_j) \|Wπ_Y\|^2}, where the infinum is taken over all measurable partitions χ={Y1,…,YJ}χ= \{Y_1,\ldots,Y_J\} of X{\cal X}. We present some properties of the μμ-norm and some computations. Our main motivation is the problem of the construction of a quantum entropy.

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