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A Differential-Geometric Approach to Quantum Ignorance Consistent with Entropic Properties of Statistical Mechanics

In this paper, we construct the metric tensor and volume for the manifold of purifications associated with an arbitrary reduced density operator [Formula: see text]. We also define a quantum coarse-graining (CG) to study the volume where macrostates are the manifolds of purifications, which we call...

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Detalles Bibliográficos
Autores principales: Ray, Shannon, Alsing, Paul M., Cafaro, Carlo, Jacinto, H S.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2023
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10217130/
https://www.ncbi.nlm.nih.gov/pubmed/37238543
http://dx.doi.org/10.3390/e25050788
Descripción
Sumario:In this paper, we construct the metric tensor and volume for the manifold of purifications associated with an arbitrary reduced density operator [Formula: see text]. We also define a quantum coarse-graining (CG) to study the volume where macrostates are the manifolds of purifications, which we call surfaces of ignorance (SOI), and microstates are the purifications of [Formula: see text]. In this context, the volume functions as a multiplicity of the macrostates that quantifies the amount of information missing from [Formula: see text]. Using examples where the SOI are generated using representations of [Formula: see text] , [Formula: see text] , and [Formula: see text] , we show two features of the CG: (1) A system beginning in an atypical macrostate of smaller volume evolves to macrostates of greater volume until it reaches the equilibrium macrostate in a process in which the system and environment become strictly more entangled, and (2) the equilibrium macrostate takes up the vast majority of the coarse-grained space especially as the dimension of the total system becomes large. Here, the equilibrium macrostate corresponds to a maximum entanglement between the system and the environment. To demonstrate feature (1) for the examples considered, we show that the volume behaves like the von Neumann entropy in that it is zero for pure states, maximal for maximally mixed states, and is a concave function with respect to the purity of [Formula: see text]. These two features are essential to typicality arguments regarding thermalization and Boltzmann’s original CG.