2015
DOI: 10.1103/physreva.92.012312
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Maximal quantum Fisher information for general su(2) parametrization processes

Abstract: Quantum Fisher information is a key concept in the field of quantum metrology, which aims to enhance the accuracy of parameter estimation by using quantum resources. In this paper, utilizing a representation of quantum Fisher information for a general unitary parametrization process, we study unitary parametrization processes governed by su(2) dynamics. We obtain the analytical expression for the Hermitian operator of the parametrization and the maximal quantum Fisher information. We find that the maximal quan… Show more

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Cited by 34 publications
(31 citation statements)
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“…A more general case is that the Hamiltonian is still independent of time but the parameter to estimate is not necessarily multiplicative. This has attracted a lot of attention recently 46 47 48 50 51 52 67 . The Hamiltonian in this case can be represented as H g ( t )= H g in general.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…A more general case is that the Hamiltonian is still independent of time but the parameter to estimate is not necessarily multiplicative. This has attracted a lot of attention recently 46 47 48 50 51 52 67 . The Hamiltonian in this case can be represented as H g ( t )= H g in general.…”
Section: Resultsmentioning
confidence: 99%
“…While most previous research on quantum metrology was focused on multiplicative parameters of Hamiltonians, growing attention has recently been drawn to more general parameters of Hamiltonians 46 or physical dynamics 47 48 , such as those of magnetic fields 46 49 50 51 . Interestingly, in contrast to estimation of multiplicative parameters, estimation of general Hamiltonian parameters exhibits distinct characteristics in some aspects, particularly in the time scaling of the Fisher information 46 , and often requires quantum control to gain the highest sensitivity 52 .…”
mentioning
confidence: 99%
“…In the latter part of this paper, we explicitly calculate this upper bound for two examples: single-qubit states and two-qubit X-states. These states appear in many applications of quantum information theory [4,29,[36][37][38][39]. This paper is organised as follows.…”
Section: Introductionmentioning
confidence: 99%
“…where n θ = (− cos Bt sin θ, − sin Bt, cos Bt cos θ). The maximal QFI is then J θ Q = 4 sin 2 (Bt) [55,57]. Similarly the optimal state can be taken as |ψ(0) = |λmax +|λmin √ 2…”
Section: Precision Under the Unitary Dynamicsmentioning
confidence: 99%