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arXiv:2312.12956

Restrictions to realize multiport quantum dense coding in a many-body quantum spin system with two- and three-body interactions

P. Kiran, Hemant Shreepad Hegde, Harsha Miriam Reji, R. Prabhu

Published Dec 20, 2023• 0 citations
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Abstract

Quantum information with many-body quantum spin systems has, from time to time, given intriguing and intuitive outcomes to our understanding of multiport quantum communications. We identify that in an anisotropic many-body quantum spin system with two- and three-body interactions, when its two-spin subsystems are all negative under partial transpose, one can restrict this system for realizing only the multiport quantum dense coding protocol which has $(N-1)$ senders and a single receiver. All other single and multi channel dense coding protocols will have quantum dense coding capacities less than that of their respective classical capacities. We characterize the multiport quantum dense coding capacity with $(N-1)$ senders and a single receiver for this system with respect to its system parameters. We also define a magnetic field averaged dense coding capacity for this system, which allows us to comprehensively capture the influence of the entire range of external applied magnetic field and characterize its variation with respect to other system parameters.

DOI
10.48550/arxiv.2312.12956

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Quantum information with many-body quantum spin systems has, from time to time, given intriguing and intuitive outcomes to our understanding of multiport quantum communications. We identify that in an anisotropic many-body quantum spin system with two- and three-body interactions, when its two-spin subsystems are all negative under partial transpose, one can restrict this system for realizing only the multiport quantum dense coding protocol which has (N−1)(N-1)(N−1) senders and a single receiver. All other single and multi channel dense coding protocols will have quantum dense coding capacities less than that of their respective classical capacities. We characterize the multiport quantum dense coding capacity with (N−1)(N-1)(N−1) senders and a single receiver for this system with respect to its system parameters. We also define a magnetic field averaged dense coding capacity for this system, which allows us to comprehensively capture the influence of the entire range of external applied magnetic field and characterize its variation with respect to other system parameters.
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