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Positivity and Nonadditivity of Quantum Capacities Using Generalized Erasure Channels - MaRDI portal

Positivity and Nonadditivity of Quantum Capacities Using Generalized Erasure Channels

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Publication:5001809

DOI10.1109/TIT.2021.3080819zbMATH Open1475.81009arXiv2003.00583MaRDI QIDQ5001809

Vikesh Siddhu, Robert B. Griffiths

Publication date: 23 July 2021

Published in: IEEE Transactions on Information Theory (Search for Journal in Brave)

Abstract: We consider various forms of a process, which we call {em gluing}, for combining two or more complementary quantum channel pairs (mathcalB,mathcalC) to form a composite. One type of gluing combines a perfect channel with a second channel to produce a emph{generalized erasure channel} pair (mathcalBg,mathcalCg). We consider two cases in which the second channel is (i) an amplitude-damping, or (ii) a phase-damping qubit channel; (ii) is the emph{dephrasure channel} of Leditzky et al. For both (i) and (ii), (mathcalBg,mathcalCg) depends on the damping parameter 0leqpleq1 and a parameter 0leqlambdaleq1 that characterizes the gluing process. In both cases we study Q(1)(mathcalBg) and Q(1)(mathcalCg), where Q(1) is the channel coherent information, and determine the regions in the (p,lambda) plane where each is zero or positive, confirming previous results for (ii). A somewhat surprising result for which we lack any intuitive explanation is that Q(1)(mathcalCg) is zero for lambdaleq1/2 when p=0, but is strictly positive (though perhaps extremely small) for all values of lambda>0 when p is positive by even the smallest amount. In addition we study the nonadditivity of Q(1)(mathcalBg) for two identical channels in parallel. It occurs in a well-defined region of the (p,lambda) plane in case (i). In case (ii) we have extended previous results for the dephrasure channel without, however, identifying the full range of (p,lambda) values where nonadditivity occurs. Again, an intuitive explanation is lacking.


Full work available at URL: https://arxiv.org/abs/2003.00583






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