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Noise evaluation of Compton camera imaging for proton therapy

Compton Cameras emerged as an alternative for real-time dose monitoring techniques for Particle Therapy (PT), based on the detection of prompt-gammas. As a consequence of the Compton scattering process, the gamma origin point can be restricted onto the surface of a cone (Compton cone). Through image...

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Detalles Bibliográficos
Autores principales: Ortega, P G, Torres-Espallardo, I, Cerutti, F, Ferrari, A, Gillam, J E, Lacasta, C, Llosá, G, Oliver, J F, Sala, P R, Solevi, P, Rafecas, M
Publicado: 2015
Materias:
XX
Acceso en línea:https://dx.doi.org/10.1088/0031-9155/60/5/1845
http://cds.cern.ch/record/2162923
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author Ortega, P G
Torres-Espallardo, I
Cerutti, F
Ferrari, A
Gillam, J E
Lacasta, C
Llosá, G
Oliver, J F
Sala, P R
Solevi, P
Rafecas, M
author_facet Ortega, P G
Torres-Espallardo, I
Cerutti, F
Ferrari, A
Gillam, J E
Lacasta, C
Llosá, G
Oliver, J F
Sala, P R
Solevi, P
Rafecas, M
author_sort Ortega, P G
collection CERN
description Compton Cameras emerged as an alternative for real-time dose monitoring techniques for Particle Therapy (PT), based on the detection of prompt-gammas. As a consequence of the Compton scattering process, the gamma origin point can be restricted onto the surface of a cone (Compton cone). Through image reconstruction techniques, the distribution of the gamma emitters can be estimated, using cone-surfaces backprojections of the Compton cones through the image space, along with more sophisticated statistical methods to improve the image quality. To calculate the Compton cone required for image reconstruction, either two interactions, the last being photoelectric absorption, or three scatter interactions are needed. Because of the high energy of the photons in PT the first option might not be adequate, as the photon is not absorbed in general. However, the second option is less efficient. That is the reason to resort to spectral reconstructions, where the incoming γ energy is considered as a variable in the reconstruction inverse problem. Jointly with prompt gamma, secondary neutrons and scattered photons, not strongly correlated with the dose map, can also reach the imaging detector and produce false events. These events deteriorate the image quality. Also, high intensity beams can produce particle accumulation in the camera, which lead to an increase of random coincidences, meaning events which gather measurements from different incoming particles. The noise scenario is expected to be different if double or triple events are used, and consequently, the reconstructed images can be affected differently by spurious data. The aim of the present work is to study the effect of false events in the reconstructed image, evaluating their impact in the determination of the beam particle ranges. A simulation study that includes misidentified events (neutrons and random coincidences) in the final image of a Compton Telescope for PT monitoring is presented. The complete chain of detection, from the beam particle entering a phantom to the event classification, is simulated using FLUKA. The range determination is later estimated from the reconstructed image obtained from a two and three-event algorithm based on Maximum Likelihood Expectation Maximization. The neutron background and random coincidences due to a therapeutic-like time structure are analyzed for mono-energetic proton beams. The time structure of the beam is included in the simulations, which will affect the rate of particles entering the detector.
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institution Organización Europea para la Investigación Nuclear
publishDate 2015
record_format invenio
spelling cern-21629232019-09-30T06:29:59Zdoi:10.1088/0031-9155/60/5/1845http://cds.cern.ch/record/2162923Ortega, P GTorres-Espallardo, ICerutti, FFerrari, AGillam, J ELacasta, CLlosá, GOliver, J FSala, P RSolevi, PRafecas, MNoise evaluation of Compton camera imaging for proton therapyXXCompton Cameras emerged as an alternative for real-time dose monitoring techniques for Particle Therapy (PT), based on the detection of prompt-gammas. As a consequence of the Compton scattering process, the gamma origin point can be restricted onto the surface of a cone (Compton cone). Through image reconstruction techniques, the distribution of the gamma emitters can be estimated, using cone-surfaces backprojections of the Compton cones through the image space, along with more sophisticated statistical methods to improve the image quality. To calculate the Compton cone required for image reconstruction, either two interactions, the last being photoelectric absorption, or three scatter interactions are needed. Because of the high energy of the photons in PT the first option might not be adequate, as the photon is not absorbed in general. However, the second option is less efficient. That is the reason to resort to spectral reconstructions, where the incoming γ energy is considered as a variable in the reconstruction inverse problem. Jointly with prompt gamma, secondary neutrons and scattered photons, not strongly correlated with the dose map, can also reach the imaging detector and produce false events. These events deteriorate the image quality. Also, high intensity beams can produce particle accumulation in the camera, which lead to an increase of random coincidences, meaning events which gather measurements from different incoming particles. The noise scenario is expected to be different if double or triple events are used, and consequently, the reconstructed images can be affected differently by spurious data. The aim of the present work is to study the effect of false events in the reconstructed image, evaluating their impact in the determination of the beam particle ranges. A simulation study that includes misidentified events (neutrons and random coincidences) in the final image of a Compton Telescope for PT monitoring is presented. The complete chain of detection, from the beam particle entering a phantom to the event classification, is simulated using FLUKA. The range determination is later estimated from the reconstructed image obtained from a two and three-event algorithm based on Maximum Likelihood Expectation Maximization. The neutron background and random coincidences due to a therapeutic-like time structure are analyzed for mono-energetic proton beams. The time structure of the beam is included in the simulations, which will affect the rate of particles entering the detector.oai:cds.cern.ch:21629232015
spellingShingle XX
Ortega, P G
Torres-Espallardo, I
Cerutti, F
Ferrari, A
Gillam, J E
Lacasta, C
Llosá, G
Oliver, J F
Sala, P R
Solevi, P
Rafecas, M
Noise evaluation of Compton camera imaging for proton therapy
title Noise evaluation of Compton camera imaging for proton therapy
title_full Noise evaluation of Compton camera imaging for proton therapy
title_fullStr Noise evaluation of Compton camera imaging for proton therapy
title_full_unstemmed Noise evaluation of Compton camera imaging for proton therapy
title_short Noise evaluation of Compton camera imaging for proton therapy
title_sort noise evaluation of compton camera imaging for proton therapy
topic XX
url https://dx.doi.org/10.1088/0031-9155/60/5/1845
http://cds.cern.ch/record/2162923
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