Abstract

Molecular imaging systems, such as positron emission tomography (PET), use detectors providing energy and a 3-D interaction position of a gamma ray within a scintillation block. Monolithic crystals are becoming an alternative to crystal arrays in PET. However, calibration processes are required to correct for nonuniformities, mainly produced by the truncation of the scintillation light distribution at the edges. We propose a calibration method based on the Voronoi diagrams. We have used $50 \times 50 \times 15$ mm3 LYSO blocks coupled to a $12\times 12$ SiPMs array. We have first studied two different interpolation algorithms: 1) weighted average method (WAM) and 2) natural neighbor (NN). We have compared them with an existing calibration based on 1-D monomials. Here, the crystal was laterally black painted and a retroreflector (RR) layer added to the entrance face. The NN exhibited the best results in terms of XY impact position, depth of Interaction, and energy, allowing us to calibrate the whole scintillation volume. Later, the NN interpolation has been tested against different crystal surface treatments, allowing always to correct edge effects. Best energy resolutions were observed when using the reflective layers (12%–14%). However, better linearity was observed with the treatments using black paint. In particular, we obtained the best overall performance when lateral black paint is combined with the RR.

Highlights

  • R ADIATION detectors are extensively used in the field of nuclear and atomic physics, characterizing particles interacting with them

  • We have introduced a calibration method based on the Voronoi diagrams to accurately determine the energy and 3-D impact positions in γ -ray detectors based on monolithic scintillation crystals

  • In a first set of experiments, we have evaluated the Weighted average method (WAM), Natural neighbor (NN), and 1-D calibration methods using a 9 × 9 22Na sources array acquired with the RR crystal

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Summary

Introduction

R ADIATION detectors are extensively used in the field of nuclear and atomic physics, characterizing particles interacting with them. This requires precise determination of their deposited energy and 3-D impact coordinates. These quantities are accurately estimated employing calibration procedures addressing nonuniformity responses of the detectors [1]–[4]. Γ -ray detectors are of special interest in both high energy and medical physics. Manuscript received July 9, 2019; revised September 9, 2019; accepted October 9, 2019. Date of publication October 16, 2019; date of current version May 1, 2020.

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