2019
DOI: 10.1007/s00184-019-00738-1
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Poisson source localization on the plane: the smooth case

Abstract: We consider the problem of localization of Poisson source by the observations of inhomogeneous Poisson processes. We suppose that there are k detectors on the plane and each detector provides the observations of Poisson processes whose intensity functions depend on the position of the emitter. We describe the properties of the maximum likelihood and Bayesian estimators. We show that under regularity conditions these estimators are consistent, asymptotically normal and asymptotically efficient. Then we propose … Show more

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Cited by 9 publications
(11 citation statements)
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References 16 publications
(25 reference statements)
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“…As mentioned in the Introduction there are several other statements related to the problem of Poisson source localization depending on the regularity of the signals. The cases of smooth signals and cusp-type signals are considered in the works [3] and [8] respectively. In particular, in [3] the estimation of the parameter ϑ 0 by k ≥ 3 sensors was made in two steps.…”
Section: Discussionmentioning
confidence: 99%
See 2 more Smart Citations
“…As mentioned in the Introduction there are several other statements related to the problem of Poisson source localization depending on the regularity of the signals. The cases of smooth signals and cusp-type signals are considered in the works [3] and [8] respectively. In particular, in [3] the estimation of the parameter ϑ 0 by k ≥ 3 sensors was made in two steps.…”
Section: Discussionmentioning
confidence: 99%
“…The cases of smooth signals and cusp-type signals are considered in the works [3] and [8] respectively. In particular, in [3] the estimation of the parameter ϑ 0 by k ≥ 3 sensors was made in two steps. First we estimate the moments of the arrival times of the signals, say, τ 1,n , .…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…The intensity function λ j,n (ϑ 0 , t) of the Poisson process received by the j-th detector taken in this work and in [1], [4] is of the form λ j,n (ϑ 0 , t) = nλ j (t − τ j ) 1I {t≥τ j } + nλ 0 , 0 ≤ t ≤ T.…”
Section: Introductionmentioning
confidence: 99%
“…To obtain small errors and have possibility to calculate it we have to consider one or another type of asymptotics. That is why we introduce the large parameter n in the intensity function (1) and study the errors of estimation in the asymptotics n → ∞. This means that the signal and noise are sufficiently large and the estimators θ = θn take values not too far from the true value:…”
Section: Introductionmentioning
confidence: 99%