2016
DOI: 10.1002/oca.2287
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Quantum state transfer control based on the optimal measurement

Abstract: Summary This paper explores the optimal control of quantum state transfer in a two‐dimensional quantum system by a sequence of non‐selective projection measurements. We show that for a given initial state, one can always find the corresponding projection operator that can effectively drive the given initial state to any arbitrary target pure state. An external control field is proposed to compensate the effect of the free evolution of system. Numerical simulations and characteristics analysis are given in thre… Show more

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Cited by 12 publications
(7 citation statements)
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“…In classical definition, fisher information is measuring the amount of information that an observable random variable carries about an unknown parameter σ. The quantum fisher information is formally generalized from classical fisher information definition as [32,33]:…”
Section: Average Total Qfimentioning
confidence: 99%
“…In classical definition, fisher information is measuring the amount of information that an observable random variable carries about an unknown parameter σ. The quantum fisher information is formally generalized from classical fisher information definition as [32,33]:…”
Section: Average Total Qfimentioning
confidence: 99%
“…On the other hand, finding the best measurements is one of the significant challenges in quantum computing. Optimal measurements have been used in many context, such as quantum discrimination [2], quantum entanglement [3][4][5], quantum teleportation [6], and superdense coding [7], also in the calculation of quantum correlation [1,[8][9][10][11][12]. We know that quantum correlations play a very critical role in quantum information and computation.…”
Section: Introductionmentioning
confidence: 99%
“…For example, continuous weak measurement [8,9,10,11] and sequential unsharp measurement [12] with estimation methods such as maximum likelihood and Baysian method [13,14,15] have been widely used in experiments [16,17]. When the projective or strong measurements are acted, the state of the system will collapse to its eigenstates, thus one needs to reprepare the ensemble and measurement apparatus at each step [18]. The weak measurements offer a trade-off between information gain and the disturbance of the system [19].…”
Section: Introductionmentioning
confidence: 99%