2019
DOI: 10.1109/tit.2018.2854747
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Quantum Channel Capacities per Unit Cost

Abstract: Communication over a noisy channel is often conducted in a setting in which different input symbols to the channel incur a certain cost. For example, for bosonic quantum channels, the cost associated with an input state is the number of photons, which is proportional to the energy consumed. In such a setting, it is often useful to know the maximum amount of information that can be reliably transmitted per cost incurred. This is known as the capacity per unit cost. In this paper, we generalize the capacity per … Show more

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Cited by 13 publications
(14 citation statements)
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“…on S(H ACD ) under the energy constraint on ρ A which essentially refines the continuity bound for this function obtained in [40] by using the method from [39]. 12 Assume that H A is the Hamiltonian of a quantum system A with the minimal energy E 0 satisfying condition (14) andF H A is any function on R + satisfying conditions (17) and (18). Denote by CB t (Ē, ε | C, D) the expression in the r.h.s.…”
Section: Tight Continuity Bound For the Qcmi At The Output Of A Localsupporting
confidence: 60%
“…on S(H ACD ) under the energy constraint on ρ A which essentially refines the continuity bound for this function obtained in [40] by using the method from [39]. 12 Assume that H A is the Hamiltonian of a quantum system A with the minimal energy E 0 satisfying condition (14) andF H A is any function on R + satisfying conditions (17) and (18). Denote by CB t (Ē, ε | C, D) the expression in the r.h.s.…”
Section: Tight Continuity Bound For the Qcmi At The Output Of A Localsupporting
confidence: 60%
“…The product B • n s = τ P/(hf c ) is the number of signal photons received in unit time. As a side note, PIE is closely related to the information theoretic concept of the capacity per unit cost which has been analyzed within the classical [72] as well as the quantum mechanical [73], [74] framework.…”
Section: Photon-starved Communicationmentioning
confidence: 99%
“…which is the Poisson distribution one would obtain for a discrete ensemble of coherent states with amplitudes satisfying η 0 |α k | 2 = c k in (9). Note that the average number of photons at the output for this scenario is still equal to η 0n0 .…”
Section: Poisson Channelmentioning
confidence: 76%
“…The ultimate information rates for such channels, known as classical channel capacities, have been studied extensively in the literature [4]- [6]. However, even though the optimal ensembles of quantum states saturating the classical capacity bound for Gaussian channels have been discovered, the necessary measurement schemes remain largely unknown, with the exception of a few particular scenarios [7]- [9]. These involve regimes of very weak and very strong signal strengths, quantified by the average number of photons per channel use received at the output, in which respectively a photon number resolving (PNR) or a heterodyne detection become almost optimal [4], [7], [8].…”
Section: Introductionmentioning
confidence: 99%