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Characterization of scintillating fibers for use as positron detector in positron emission tomography. | LitMetric

Characterization of scintillating fibers for use as positron detector in positron emission tomography.

Phys Med

Medical Physics Unit, McGill University, Montreal, Quebec, Canada; Department of Oncology, McGill University, Montreal, Quebec, Canada; Research Institute of the McGill University Health Centre, Montreal, Quebec, Canada.

Published: September 2019

AI Article Synopsis

  • * The detector design involves scintillating fibers connected to fiber-optic cables and photo multiplier tubes, allowing it to be worn on a patient's wrist while evaluating its response to gamma radiation and positron-emitting radio-tracers like F and C.
  • * Results indicate that the scintillating fibers have promising attenuation length properties and signal purity, suggesting they could provide a viable non-invasive alternative for measuring AIF in PET imaging.

Article Abstract

Purpose: Manual and automatic blood sampling at different time intervals is considered the gold standard to determine the arterial input function (AIF) in dynamic positron emission tomography (PET). However, blood sampling is characterized by poor time resolution and is an invasive procedure. The aim of this study was to characterize the scintillating fibers used to develop a non-invasive positron detector.

Methods: The detector consists of a scintillating fiber coupled at each end to transmission fiber-optic cables that are connected to photo multiplier tubes in a dual readout setup. The detector is designed to be wrapped around the wrist of the patient undergoing dynamic PET. The attenuation length and bending losses were measured with excitation from gamma radiation (Cs) and ultraviolet (UV) light. The response to positron-emitting radio-tracers was evaluated with F and C.

Results: The attenuation length for a 3.0 m and 1.5 m long scintillating fiber both coincides with the attenuation length given by the manufacturer when excited with the Cs source, but not with the UV source due to the differences in scintillation mechanisms. The bending losses are smaller than the measurement uncertainty for the Cs source irradiation, and increase when the bending radius decrease for the UV source irradiation. The signal-to-noise ratio for F and C solutions are 1.98 and 22.54 respectively. The measured decay constant of C agrees with its characteristic value.

Conclusion: The performed measurements in the dual readout configuration suggest that scintillating fibers may be suitable to determine the AIF non-invasively.

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Source
http://dx.doi.org/10.1016/j.ejmp.2019.08.009DOI Listing

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