Abstract

We develop a new algorithm for the tracking of radioactive particles using Positron Emission Particle Tracking (PEPT). The algorithm relies on the maximization of the likelihood of a simple Gaussian mixture model of the lines of response associated with positron annihilation. The model includes a component that accounts for spurious lines caused by scattering and random coincidence, and it treats the relative activity of particles as well as their positions as parameters to be inferred. Values of these parameters that approximately maximize the likelihood are computed by the application of an expectation-maximization algorithm. A generalization of the model that includes the particle velocities and accelerations as additional parameters takes advantage of the information contained in the exact timing of positron annihilations to reconstruct pieces of trajectories rather than fixed positions, with clear benefits. We test the algorithm on both simulated and experimental data. The results show the algorithm to be highly effective for the simultaneous tracking of many particles (up to 80 in one test). It provides estimates of particle positions that are easily mapped to entire trajectories and handles a variable number of particles in the field of view. The ability to track a large number of particles robustly offers the possibility of a dramatic expansion of the scope of PEPT.

Highlights

  • Positron Emission Particle Tracking (PEPT) is a method of tracking single particles using the back-to-back emission of 511 keV photons from positron annihilation

  • The PEPT technique uses similar principles to Positron Emission Tomography (PET), in which a radioactive tracer undergoing β+ decay emits positrons which subsequently annihilate with surrounding electrons, generating the back-to-back photons

  • We develop a new algorithm to infer the position of multiple PEPT particles from detected Lines of Response (LORs)

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Summary

INTRODUCTION

Positron Emission Particle Tracking (PEPT) is a method of tracking single particles using the back-to-back emission of 511 keV photons from positron annihilation. The PEPT technique uses similar principles to Positron Emission Tomography (PET), in which a radioactive tracer undergoing β+ decay emits positrons which subsequently annihilate with surrounding electrons, generating the back-to-back photons The detection of these gamma ray pairs produces data in the form of lines in R3, known as Lines of Response (LORs). The PET technique consists of inverting the detected LORs to produce a threedimensional image of radioactive scalar density by attributing levels of radioactivity to each voxel in the field of view This requires a relatively long exposure time and is only suitable for visualising dynamic processes occurring on time scales of the order of 1 second.

MIXTURE MODEL
Algorithm
Simple demonstration
Sequential tracking
Higher-order tracking
Ten rotating particles
Pipe-flow experiment: merged trajectories
Pipe-flow experiment: flow-profile reconstruction
Findings
CONCLUSION
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