2009
DOI: 10.1109/tns.2009.2015308
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Maximum-Likelihood Methods for Processing Signals From Gamma-Ray Detectors

Abstract: In any gamma-ray detector, each event produces electrical signals on one or more circuit elements. From these signals, we may wish to determine the presence of an interaction; whether multiple interactions occurred; the spatial coordinates in two or three dimensions of at least the primary interaction; or the total energy deposited in that interaction. We may also want to compute listmode probabilities for tomographic reconstruction. Maximum-likelihood methods provide a rigorous and in some senses optimal appr… Show more

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Cited by 147 publications
(148 citation statements)
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“…For an event at position r producing N photons the probability of the i-th PMT detecting n i photons is well approximated by the Poisson distribution [14]:…”
Section: Event Reconstruction Methodsmentioning
confidence: 99%
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“…For an event at position r producing N photons the probability of the i-th PMT detecting n i photons is well approximated by the Poisson distribution [14]:…”
Section: Event Reconstruction Methodsmentioning
confidence: 99%
“…There are several methods for obtaining the LRFs described in the literature. The most straightforward of these is the direct measurement, by scanning the detector with a moving well-collimated γ-ray source [14,20]. Unfortunately, a combination of several factors made this method impractical for the ZEPLIN-III detector.…”
Section: Reconstruction Of Light Response Functionsmentioning
confidence: 99%
“…For a review of ML estimation as applied to photon-processing detectors, see Barrett et al 16 To summarize what we know about how to implement optimum estimation of photon attributes, an ideal photon-processing detector must:…”
Section: Photon-processing Detectorsmentioning
confidence: 99%
“…The Fano factor of the photoelectrons on the j th detector element (F nj ) is given by [26] ( 16) Here, α j is the fraction of emitted optical photons detected at the j th detector element. In the photon transport model described in Section III-B, α j is the product of the quantum and geometrical efficiencies of the j th detector element.…”
Section: A Assumptions For Maximizing the Impact Of The Fano Factormentioning
confidence: 99%