2016
DOI: 10.1016/s0034-4877(16)30032-5
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Irreducible Decompositions and Stationary States of Quantum Channels

Abstract: Abstract. For a quantum channel (completely positive, trace-preserving map), we prove a generalization to the infinite dimensional case of a result by Baumgartner and Narnhofer ([3]). This result is, in a probabilistic language, a decomposition of a general quantum channel into its irreducible positive recurrent components. This decomposition is related with a communication relation on the reference Hilbert space. This allows us to describe the full structure of invariant states of a quantum channel, and of th… Show more

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Cited by 24 publications
(36 citation statements)
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“…Specifically, using a generalized notion of quantum sufficient statistic [24][25][26][27], we show that a local operation on part of a system is efficient if and only if it unitarily preserves the minimal sufficient statistic of the part for arXiv:2001.02258v3 [quant-ph] 1 Feb 2020 the whole. Our geometric interpretation of this also draws on recent progress on fixed points of quantum channels [28][29][30][31].…”
Section: Introductionmentioning
confidence: 99%
“…Specifically, using a generalized notion of quantum sufficient statistic [24][25][26][27], we show that a local operation on part of a system is efficient if and only if it unitarily preserves the minimal sufficient statistic of the part for arXiv:2001.02258v3 [quant-ph] 1 Feb 2020 the whole. Our geometric interpretation of this also draws on recent progress on fixed points of quantum channels [28][29][30][31].…”
Section: Introductionmentioning
confidence: 99%
“…A necessary and sufficient algebraic condition for uniqueness of this invariant state is (see e.g. [7,20,5])…”
Section: Introductionmentioning
confidence: 99%
“…Each spin is L-dimensional and indexed by the physical index . Let us consider a faithful channel E = {E } L =1 (with E N × N matrices for some bond dimension N ) and write its corresponding MPS |Φ (47) where the N × N boundary matrix B provides the ability to pin the boundary of the chain to various states [98]. Physically meaningful boundaries are either B = I (the identity) for translationally invariant MPS's or B = |r l| for some states |r , |l quantifying the effect of the boundary on the right and left ends of the chain.…”
Section: Mps From Faithful Channelsmentioning
confidence: 99%