2016
DOI: 10.1109/tit.2016.2516006
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Smooth Entropy Bounds on One-Shot Quantum State Redistribution

Abstract: In quantum state redistribution as introduced in [Luo and Devetak (2009)] and [Devetak and Yard (2008)], there are four systems of interest: the A system held by Alice, the B system held by Bob, the C system that is to be transmitted from Alice to Bob, and the R system that holds a purification of the state in the ABC registers. We give upper and lower bounds on the amount of quantum communication and entanglement required to perform the task of quantum state redistribution in a one-shot setting. Our bounds ar… Show more

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Cited by 36 publications
(92 citation statements)
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References 30 publications
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“…We use a new achievability bound for a communication cost in terms of one-shot entropies. The proof of this result appears in a joint work with Berta and Christandl [11]. Independently of our work, similar upper bounds on one-shot state redistribution have been obtained by Datta, Hsieh and Oppenheim [21].…”
Section: Protocol Compression and Direct Sumsupporting
confidence: 82%
See 1 more Smart Citation
“…We use a new achievability bound for a communication cost in terms of one-shot entropies. The proof of this result appears in a joint work with Berta and Christandl [11]. Independently of our work, similar upper bounds on one-shot state redistribution have been obtained by Datta, Hsieh and Oppenheim [21].…”
Section: Protocol Compression and Direct Sumsupporting
confidence: 82%
“…Entanglement is deemed free for the compression. We make use of a one-shot state redistribution achievability bound that we derived in joint work with Berta and Christandl [11]. The bound in that work is stated in terms of one-shot entropies.…”
Section: Protocol Compression At Information Costmentioning
confidence: 99%
“…Regarding the existing algorithms, the achievability bounds of E(ψ) of the corresponding entanglementassisted LOCC algorithms can be calculated from the analyses in Refs. [38], [40]- [44], [47]. Given > 0, these achievability bounds are in the form E(ψ) = · · · + O log 1 as → 0, which diverges to infinity as higher fidelity is pursued.…”
Section: Proof Of Theoremmentioning
confidence: 99%
“…In this section, we consider state redistribution with feedback [8], where the state redistribution protocol consists of M rounds of forward and backward quantum communication between Alice and Bob. The initial state of the protocol is again the pure state ψ ABCR ⊗ Φ k T A T B , where systems A and C are with Alice, B is with Bob, R is an inaccessible reference system, and Φ k…”
Section: State Redistribution With Feedbackmentioning
confidence: 99%