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Quantum Orlicz Spaces in Information Geometry

机译:信息几何中的量子Orlicz空间

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Let Ho be a selfadjoint operator such that Tre~(-βH_0) is of trace class for some β < 1, and let X_ε denote the set of ε-bounded forms, i.e., ‖(H_0+C)~(-1/2-ε)X(H_0+C)~(-1/2+ε)‖ < C for some C > 0. Let X := Span ∪_(ε∈(0,1/2]) Χ_ε. Let M denote the underlying set of the quantum information manifold of states of the form ρ_x = e~(-H_0-X-ΨX), X ∈ X. We show that if Tr e~(H_0) = 1, 1. the map Φ, Φ(X) = 1/2Tr (e~(-H_0+X) +e~(-H_0-X) - 1 is a quantum Young function defined on X 2. The Orlicz space defined by Φ is the tangent space of M at ρ_0; its affine structure is defined by the (+1)-connection of Amari 3. The subset of a 'hood of ρ_0, consisting of p-nearby states (those σ ∈ M obeying C~(-1)ρ~(1+p) ≤ σ ≤ Cρ~(1-p) for some C > 1) admits a flat affine connection known as the (-1) connection, and the span of this set is part of the cotangent space of M 4. These dual structures extend to the completions in the Luxemburg norms.
机译:令Ho为自伴算子,使得Tre〜(-βH_0)对于某些1的跟踪类,令X_ε表示ε界形式的集合,即‖(H_0 + C)〜(-1/2 -ε)X(H_0 + C)〜(-1 / 2 +ε)” 0。令X:=跨度∪_(εε(0,1 / 2])Χ_ε。令M表示形式为ρ_x= e〜(-H_0-X-ΨX),X∈X的状态的量子信息流的底层集合。我们证明,如果Tr e〜(H_0)= 1,1.则映射Φ,Φ (X)= 1 / 2Tr(e〜(-H_0 + X)+ e〜(-H_0-X)-1是在X 2上定义的量子Young函数。由Φ定义的Orlicz空间是M的切线空间ρ_0;其仿射结构由Amari 3的(+1)连接定义。ρ_0罩的子集由p附近状态(其中σ∈M服从C〜(-1)ρ〜(1)组成) + p)≤σ≤Cρ〜(1-p)对于某些C> 1)允许一个平直的仿射连接,称为(-1)连接,并且该集合的跨度是M 4的余切空间的一部分。这些双重结构扩展到卢森堡规范中的完成。

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