2017
DOI: 10.1103/physreva.95.012136
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Quantum estimation of unknown parameters

Abstract: We discuss the problem of finding the best measurement strategy for estimating the value of a quantum system parameter. In general the optimum quantum measurement, in the sense that it maximizes the quantum Fisher information and hence allows one to minimize the estimation error, can only be determined if the value of the parameter is already known. A modification of the quantum Van Trees inequality, which gives a lower bound on the error in the estimation of a random parameter, is proposed. The suggested ineq… Show more

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Cited by 22 publications
(18 citation statements)
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“…And while this does not guarantee that our solution will be optimal for a few observations (an adaptive scheme may be better than repeating the same measurement in that case), we will see that having an error that is a function of the number of repetitions where the first point is already tight, and that also tends towards the asymptotically optimal solution as the number of shots grows, is enough to draw conclusions to important questions such as the role of photon number correlations or the performance of experimentally feasible measurements in the regime of limited data. For instance, we have found an example where the correlations between the paths of the Mach-Zehnder interferometer appear to be particularly useful in this regime, and we have demonstrated that while measuring quadratures and counting photons after the action of a beam splitter are asymptotically equivalent in an ideal scenario, the former measurement scheme is better for a low number of repeated experiments.It is interesting to note that a related approach was recently discussed in [35], where the authors presented a modification of the quantum Van Trees inequality and used it to construct an adaptive strategy based on an optimal parameter-independent single-shot measurement scheme. Therefore, our work and [35] are complementary, since we will mainly focus on repeated measurements to connect the optimal single-shot and asymptotic regimes and to 2 If the probability model belongs to the exponential family and the estimator is unbiased, then it is possible to saturate the Cramér-Rao bound exactly even for a single shot [4,23,24].…”
mentioning
confidence: 99%
“…And while this does not guarantee that our solution will be optimal for a few observations (an adaptive scheme may be better than repeating the same measurement in that case), we will see that having an error that is a function of the number of repetitions where the first point is already tight, and that also tends towards the asymptotically optimal solution as the number of shots grows, is enough to draw conclusions to important questions such as the role of photon number correlations or the performance of experimentally feasible measurements in the regime of limited data. For instance, we have found an example where the correlations between the paths of the Mach-Zehnder interferometer appear to be particularly useful in this regime, and we have demonstrated that while measuring quadratures and counting photons after the action of a beam splitter are asymptotically equivalent in an ideal scenario, the former measurement scheme is better for a low number of repeated experiments.It is interesting to note that a related approach was recently discussed in [35], where the authors presented a modification of the quantum Van Trees inequality and used it to construct an adaptive strategy based on an optimal parameter-independent single-shot measurement scheme. Therefore, our work and [35] are complementary, since we will mainly focus on repeated measurements to connect the optimal single-shot and asymptotic regimes and to 2 If the probability model belongs to the exponential family and the estimator is unbiased, then it is possible to saturate the Cramér-Rao bound exactly even for a single shot [4,23,24].…”
mentioning
confidence: 99%
“…We assume a coherent probe state |α⟩, and, without loss of generality, that the displacement is positive and real, i.e., α = |α| > 0. This probe state is acted upon by the rotation operator R(θ) given by (5). The action of the rotation operator R(θ) on the probe state |α⟩ gives the encoded state e −iθ α .…”
Section: Phase Estimationmentioning
confidence: 99%
“…Bayesian approach they are treated as random variables with an associated prior distribution function. The application of the Bayesian estimation scheme for various quantum parameter estimation problems has previously been studied in [5], [8], [17], [18]. The Bayesian estimation approach utilizes knowledge of the prior distribution of the unknown parameter θ and the likelihood of the observed data to find the posterior distribution of θ.…”
Section: Introductionmentioning
confidence: 99%
“…Optimality of a quantum sensing protocol is defined via a cost function C which must be identified in context of a specific measurement task. In our study of variational N -atom Ramsey interferometry, we wish to optimize for phase estimation accuracy, defined as the mean square error (φ) relative to the actual phase φ averaged with respect to a certain prior distribution P δφ (φ) over a finite dynamic range δφ of the interferometer [20,22,[63][64][65][66][67]. We contrast this to approaches optimizing accuracy for a specific value of the phase, corresponding to δφ → 0, as is done in a Fisher information approach [68,69], and underlies the discussion of Ramsey interferometry with squeezed spin states (SSS) [70,71] or GHZ states [72].…”
Section: Introductionmentioning
confidence: 99%