1
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Zhang J, Xiao X, Chen Y, Zhang B, Ma X, Ai X, Li J. A Portable Three-Layer Compton Camera for Wide-Energy-Range Gamma-ray Imaging: Design, Simulation and Preliminary Testing. SENSORS (BASEL, SWITZERLAND) 2023; 23:8951. [PMID: 37960650 PMCID: PMC10647430 DOI: 10.3390/s23218951] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 10/06/2023] [Revised: 10/30/2023] [Accepted: 11/01/2023] [Indexed: 11/15/2023]
Abstract
(1) Background: The imaging energy range of a typical Compton camera is limited due to the fact that scattered gamma photons are seldom fully absorbed when the incident energies are above 3 MeV. Further improving the upper energy limit of gamma-ray imaging has important application significance in the active interrogation of special nuclear materials and chemical warfare agents, as well as range verification of proton therapy. (2) Methods: To realize gamma-ray imaging in a wide energy range of 0.3~7 MeV, a principle prototype, named a portable three-layer Compton camera, is developed using the scintillation detector that consists of an silicon photomultiplier array coupled with a Gd3Al2Ga3O12:Ce pixelated scintillator array. Implemented in a list-mode maximum likelihood expectation maximization algorithm, a far-field energy-domain imaging method based on the two interaction events is applied to estimate the initial energy and spatial distribution of gamma-ray sources. The simulation model of the detectors is established based on the Monte Carlo simulation toolkit Geant4. The reconstructed images of a 133Ba, a 137Cs and a 60Co point-like sources have been successfully obtained with our prototype in laboratory tests and compared with simulation studies. (3) Results: The proportion of effective imaging events accounts for about 2%, which allows our prototype to realize the reconstruction of the distribution of a 0.05 μSv/h 137Cs source in 10 s. The angular resolution for resolving two 137Cs point-like sources is 15°. Additional simulated imaging of the 6.13 MeV gamma-rays from 14.1 MeV neutron scattering with water preliminarily demonstrates the imaging capability for high incident energy. (4) Conclusions: We conclude that the prototype has a good imaging performance in a wide energy range (0.3~7 MeV), which shows potential in several MeV gamma-ray imaging applications.
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Affiliation(s)
| | | | | | | | | | | | - Jinglun Li
- State Key Laboratory of NBC Protection for Civilian, Beijing 102205, China; (J.Z.); (X.X.); (Y.C.); (B.Z.); (X.M.); (X.A.)
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2
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Borja-Lloret M, Barrientos L, Bernabéu J, Lacasta C, Muñoz E, Ros A, Roser J, Viegas R, Llosá G. Influence of the background in Compton camera images for proton therapy treatment monitoring. Phys Med Biol 2023; 68:144001. [PMID: 37339665 DOI: 10.1088/1361-6560/ace024] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [MESH Headings] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 02/03/2023] [Accepted: 06/20/2023] [Indexed: 06/22/2023]
Abstract
Objective. Background events are one of the most relevant contributions to image degradation in Compton camera imaging for hadron therapy treatment monitoring. A study of the background and its contribution to image degradation is important to define future strategies to reduce the background in the system.Approach. In this simulation study, the percentage of different kinds of events and their contribution to the reconstructed image in a two-layer Compton camera have been evaluated. To this end, GATE v8.2 simulations of a proton beam impinging on a PMMA phantom have been carried out, for different proton beam energies and at different beam intensities.Main results. For a simulated Compton camera made of Lanthanum (III) Bromide monolithic crystals, coincidences caused by neutrons arriving from the phantom are the most common type of background produced by secondary radiations in the Compton camera, causing between 13% and 33% of the detected coincidences, depending on the beam energy. Results also show that random coincidences are a significant cause of image degradation at high beam intensities, and their influence in the reconstructed images is studied for values of the time coincidence windows from 500 ps to 100 ns.Significance. Results indicate the timing capabilities required to retrieve the fall-off position with good precision. Still, the noise observed in the image when no randoms are considered make us consider further background rejection methods.
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Affiliation(s)
- M Borja-Lloret
- Institut de Física Corpuscular (IFIC), CSIC-UV, València, Spain
| | - L Barrientos
- Institut de Física Corpuscular (IFIC), CSIC-UV, València, Spain
| | - J Bernabéu
- Institut de Física Corpuscular (IFIC), CSIC-UV, València, Spain
| | - C Lacasta
- Institut de Física Corpuscular (IFIC), CSIC-UV, València, Spain
| | - E Muñoz
- Institut de Física Corpuscular (IFIC), CSIC-UV, València, Spain
| | - A Ros
- Institut de Física Corpuscular (IFIC), CSIC-UV, València, Spain
| | - J Roser
- Institut de Física Corpuscular (IFIC), CSIC-UV, València, Spain
| | - R Viegas
- Institut de Física Corpuscular (IFIC), CSIC-UV, València, Spain
| | - G Llosá
- Institut de Física Corpuscular (IFIC), CSIC-UV, València, Spain
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3
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Missaglia A, Bourkadi-Idrissi A, Casamichiela F, Mazzucconi D, Carminati M, Agosteo S, Fiorini C. Prompt-gamma fall-off estimation with C-ion irradiation at clinical energies, using a knife-edge slit camera: A Monte Carlo study. Phys Med 2023; 107:102554. [PMID: 36907030 DOI: 10.1016/j.ejmp.2023.102554] [Citation(s) in RCA: 3] [Impact Index Per Article: 3.0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Journal Information] [Submit a Manuscript] [Subscribe] [Scholar Register] [Received: 07/03/2022] [Revised: 02/09/2023] [Accepted: 02/18/2023] [Indexed: 03/12/2023] Open
Abstract
PURPOSE In-vivo range verification has been a hot topic in particle therapy since two decades. Many efforts have been done for proton therapy, while fewer studies were conducted considering a beam of carbon ions. In the present work, a simulation study was performed to show whether it is possible to measure the prompt-gamma fall-off inside the high neutron background typical of carbon-ion irradiation, using a knife-edge slit camera. In addition to this, we wanted to estimate the uncertainty in retrieving the particle range in the case of a pencil beam of C-ions at clinically relevant energy of 150 MeVu. METHODS For these purposes, the Monte Carlo code FLUKA was adopted for simulations and three different analytical methods were implemented to get the accuracy in the range retrieval of the simulated set-up. RESULTS The analysis of simulation data has brought to the promising and desired precision of about 4 mm in the determination of the dose profile fall-off in case of a spill irradiation, for which all the three cited methods were coherent in their predictions. CONCLUSIONS The Prompt Gamma Imaging technique should be further studied as a tool to reduce range uncertainties affecting carbon ion radiation therapy.
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Affiliation(s)
- Andrea Missaglia
- Dipartimento di Elettronica, Informazione e Bioingegneria - Politecnico di Milano, Via Ponzio, 34/5, 20133, Milan, Italy.
| | - Aicha Bourkadi-Idrissi
- Dipartimento di Elettronica, Informazione e Bioingegneria - Politecnico di Milano, Via Ponzio, 34/5, 20133, Milan, Italy; INFN - sezione di Milano, Via Giovanni Celoria, 16, 20133, Milan, Italy.
| | - Francesco Casamichiela
- Dipartimento di Energia - Politecnico di Milano, Via Lambruschini, 4, 20156, Milan, Italy.
| | - Davide Mazzucconi
- INFN - sezione di Milano, Via Giovanni Celoria, 16, 20133, Milan, Italy; Dipartimento di Energia - Politecnico di Milano, Via Lambruschini, 4, 20156, Milan, Italy.
| | - Marco Carminati
- Dipartimento di Elettronica, Informazione e Bioingegneria - Politecnico di Milano, Via Ponzio, 34/5, 20133, Milan, Italy; INFN - sezione di Milano, Via Giovanni Celoria, 16, 20133, Milan, Italy.
| | - Stefano Agosteo
- INFN - sezione di Milano, Via Giovanni Celoria, 16, 20133, Milan, Italy; Dipartimento di Energia - Politecnico di Milano, Via Lambruschini, 4, 20156, Milan, Italy.
| | - Carlo Fiorini
- Dipartimento di Elettronica, Informazione e Bioingegneria - Politecnico di Milano, Via Ponzio, 34/5, 20133, Milan, Italy; INFN - sezione di Milano, Via Giovanni Celoria, 16, 20133, Milan, Italy.
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4
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Parajuli RK, Sakai M, Parajuli R, Tashiro M. Development and Applications of Compton Camera-A Review. SENSORS (BASEL, SWITZERLAND) 2022; 22:7374. [PMID: 36236474 PMCID: PMC9573429 DOI: 10.3390/s22197374] [Citation(s) in RCA: 7] [Impact Index Per Article: 3.5] [Reference Citation Analysis] [Abstract] [Key Words] [MESH Headings] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Received: 08/11/2022] [Revised: 09/08/2022] [Accepted: 09/20/2022] [Indexed: 06/16/2023]
Abstract
The history of Compton cameras began with the detection of radiation sources originally for applications in astronomy. A Compton camera is a promising γ-ray detector that operates in the wide energy range of a few tens of keV to MeV. The γ-ray detection method of a Compton camera is based on Compton scattering kinematics, which is used to determine the direction and energy of the γ-rays without using a mechanical collimator. Although the Compton camera was originally designed for astrophysical applications, it was later applied in medical imaging as well. Moreover, its application in environmental radiation measurements is also under study. Although a few review papers regarding Compton cameras have been published, they either focus very specifically on the detectors used in such cameras or the particular applications of Compton cameras. Thus, the aim of this paper is to review the features and types of Compton cameras and introduce their applications, associated imaging algorithms, improvement scopes, and their future aspects.
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Affiliation(s)
- Raj Kumar Parajuli
- Department of Molecular Imaging and Theranostics, National Institutes for Quantum Science and Technology, 4-9-1 Anagawa, Inage, Chiba 263-8555, Japan
- Gunma University Heavy Ion Medical Center, Gunma University, 3-39-22 Showa-machi, Maebashi 371-8511, Japan
| | - Makoto Sakai
- Gunma University Heavy Ion Medical Center, Gunma University, 3-39-22 Showa-machi, Maebashi 371-8511, Japan
| | | | - Mutsumi Tashiro
- Gunma University Heavy Ion Medical Center, Gunma University, 3-39-22 Showa-machi, Maebashi 371-8511, Japan
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5
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Giacomo SD, Utica G, Carminati M, Borghi G, Picciotto A, Fiorini C. Timing Performances of SDD as Photodetector Candidate for Proton Therapy Application. IEEE TRANSACTIONS ON RADIATION AND PLASMA MEDICAL SCIENCES 2022. [DOI: 10.1109/trpms.2021.3137668] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/05/2022]
Affiliation(s)
- S. Di Giacomo
- Dipartimento di Elettronica, Informazione e Bioingegneria, Politecnico di Milano, Milan, Italy
| | - G. Utica
- Dipartimento di Elettronica, Informazione e Bioingegneria, Politecnico di Milano, Milan, Italy
| | - M. Carminati
- Dipartimento di Elettronica, Informazione e Bioingegneria, Politecnico di Milano, Milan, Italy
| | - G. Borghi
- Integrated Radiation and Image Sensors, Fondazione Bruno Kessler, Trento, Italy
| | - A. Picciotto
- Integrated Radiation and Image Sensors, Fondazione Bruno Kessler, Trento, Italy
| | - C. Fiorini
- Dipartimento di Elettronica, Informazione e Bioingegneria, Politecnico di Milano, Milan, Italy
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6
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Mohammadi A, Tashima H, Takyu S, Iwao Y, Akamatsu G, Kang HG, Obata F, Nishikido F, Parodi K, Yamaya T. Feasibility of triple gamma ray imaging of 10C for range verification in ion therapy. Phys Med Biol 2022; 67. [DOI: 10.1088/1361-6560/ac826a] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 04/27/2022] [Accepted: 07/19/2022] [Indexed: 11/12/2022]
Abstract
Abstract
Objective. In carbon ion therapy, the visualization of the range of incident particles in a patient body is important for treatment verification. In-beam positron emission tomography (PET) imaging is one of the methods to verify the treatment in ion therapy due to the high quality of PET images. We have shown the feasibility of in-beam PET imaging of radioactive 15O and 11C ion beams for range verification using our OpenPET system. Recently, we developed a whole gamma imager (WGI) that can simultaneously work as PET, single gamma ray and triple gamma ray imaging. The WGI has high potential to detect the location of 10C, which emits positrons with a simultaneous gamma ray of 718 keV, within the patient’s body during ion therapy. Approach. In this work, we focus on investigating the performance of WGI for 10C imaging and its feasibility for range verification in carbon ion therapy. First, the performance of the WGI was studied to image a 10C point source using the Geant4 toolkit. Then, the feasibility of WGI was investigated for an irradiated polymethyl methacrylate (PMMA) phantom with a 10C ion beam at the carbon therapy facility of the Heavy Ion Medical Accelerator in Chiba. Main results. The average spatial resolution and sensitivity for the simulated 10C point source at the centre of the field of view were 5.5 mm FWHM and 0.010%, respectively. The depth dose of the 10C ion beam was measured, and the triple gamma image of 10C nuclides for an irradiated PMMA phantom was obtained by applying a simple back projection to the detected triple gammas. Significance. The shift between Bragg peak position and position of the peak of the triple gamma image in an irradiated PMMA phantom was 2.8 ± 0.8 mm, which demonstrates the capability of triple gamma imaging using WGI for range verification of 10C ion beams.
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7
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Compton imaging for medical applications. Radiol Phys Technol 2022; 15:187-205. [PMID: 35867197 DOI: 10.1007/s12194-022-00666-2] [Citation(s) in RCA: 10] [Impact Index Per Article: 5.0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 04/04/2022] [Revised: 07/04/2022] [Accepted: 07/04/2022] [Indexed: 12/18/2022]
Abstract
Compton imaging exploits inelastic scattering, known as Compton scattering, using a Compton camera consisting of a scatterer detector in the front layer and an absorber detector in the back layer. This method was developed for astronomy, and in recent years, research and development for environmental and medical applications has been actively conducted. Compton imaging can discriminate gamma rays over a wide energy range from several hundred keV to several MeV. Therefore, it is expected to be applied to the simultaneous imaging of multiple nuclides in nuclear medicine and prompt gamma ray imaging for range verification in particle therapy. In addition, multiple gamma coincidence imaging is expected to be realized, which allows the source position to be determined from a single coincidence event using nuclides that emit multiple gamma rays simultaneously, such as nuclides that emit a single gamma ray simultaneously with positron decay. This review introduces various efforts toward the practical application of Compton imaging in the medical field, including in vivo studies, and discusses its prospects.
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8
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Cramér–Rao Bound Evaluations of Compton Imager Designs for Proton Beam Range Verification. IEEE TRANSACTIONS ON RADIATION AND PLASMA MEDICAL SCIENCES 2022. [DOI: 10.1109/trpms.2021.3116118] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/06/2022]
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9
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Backer H, Bayerlein R, Binder T, Denker S, Fleck I, Peterson TE. Gamma-Ray Imaging Using Coincident Detection of Cherenkov Photons for Medical Applications. IEEE TRANSACTIONS ON RADIATION AND PLASMA MEDICAL SCIENCES 2022. [DOI: 10.1109/trpms.2021.3101481] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/08/2022]
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10
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Lerendegui-Marco J, Balibrea-Correa J, Babiano-Suárez V, Ladarescu I, Domingo-Pardo C. Towards machine learning aided real-time range imaging in proton therapy. Sci Rep 2022; 12:2735. [PMID: 35177663 PMCID: PMC8854574 DOI: 10.1038/s41598-022-06126-6] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [MESH Headings] [Grants] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 06/02/2021] [Accepted: 01/20/2022] [Indexed: 11/08/2022] Open
Abstract
Compton imaging represents a promising technique for range verification in proton therapy treatments. In this work, we report on the advantageous aspects of the i-TED detector for proton-range monitoring, based on the results of the first Monte Carlo study of its applicability to this field. i-TED is an array of Compton cameras, that have been specifically designed for neutron-capture nuclear physics experiments, which are characterized by [Formula: see text]-ray energies spanning up to 5-6 MeV, rather low [Formula: see text]-ray emission yields and very intense neutron induced [Formula: see text]-ray backgrounds. Our developments to cope with these three aspects are concomitant with those required in the field of hadron therapy, especially in terms of high efficiency for real-time monitoring, low sensitivity to neutron backgrounds and reliable performance at the high [Formula: see text]-ray energies. We find that signal-to-background ratios can be appreciably improved with i-TED thanks to its light-weight design and the low neutron-capture cross sections of its LaCl[Formula: see text] crystals, when compared to other similar systems based on LYSO, CdZnTe or LaBr[Formula: see text]. Its high time-resolution (CRT [Formula: see text] 500 ps) represents an additional advantage for background suppression when operated in pulsed HT mode. Each i-TED Compton module features two detection planes of very large LaCl[Formula: see text] monolithic crystals, thereby achieving a high efficiency in coincidence of 0.2% for a point-like 1 MeV [Formula: see text]-ray source at 5 cm distance. This leads to sufficient statistics for reliable image reconstruction with an array of four i-TED detectors assuming clinical intensities of 10[Formula: see text] protons per treatment point. The use of a two-plane design instead of three-planes has been preferred owing to the higher attainable efficiency for double time-coincidences than for threefold events. The loss of full-energy events for high energy [Formula: see text]-rays is compensated by means of machine-learning based algorithms, which allow one to enhance the signal-to-total ratio up to a factor of 2.
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Affiliation(s)
| | | | | | - Ion Ladarescu
- Instituto de Física Corpuscular, CSIC-University of Valencia, Valencia, Spain
| | - César Domingo-Pardo
- Instituto de Física Corpuscular, CSIC-University of Valencia, Valencia, Spain
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11
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Tashima H, Yoshida E, Iwao Y, Wakizaka H, Mohammadi A, Nitta M, Kitagawa A, Inaniwa T, Nishikido F, Tsuji AB, Nagai Y, Seki C, Minamimoto T, Fujibayashi Y, Yamaya T. Development of a Multiuse Human-Scale Single-Ring OpenPET System. IEEE TRANSACTIONS ON RADIATION AND PLASMA MEDICAL SCIENCES 2021. [DOI: 10.1109/trpms.2020.3037055] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/09/2022]
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12
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Livingstone J, Dauvergne D, Etxebeste A, Fontana M, Gallin-Martel ML, Huisman B, Létang JM, Marcatili S, Sarrut D, Testa É. Influence of sub-nanosecond time of flight resolution for online range verification in proton therapy using the line-cone reconstruction in Compton imaging. Phys Med Biol 2021; 66. [PMID: 34020434 DOI: 10.1088/1361-6560/ac03cb] [Citation(s) in RCA: 4] [Impact Index Per Article: 1.3] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 12/14/2020] [Accepted: 05/21/2021] [Indexed: 11/11/2022]
Abstract
Online ion range monitoring in hadron therapy can be performed via detection of secondary radiation, such as promptγ-rays, emitted during treatment. The promptγemission profile is correlated with the ion depth-dose profile and can be reconstructed via Compton imaging. The line-cone reconstruction, using the intersection between the primary beam trajectory and the cone reconstructed via a Compton camera, requires negligible computation time compared to iterative algorithms. A recent report hypothesised that time of flight (TOF) based discrimination could improve the precision of theγfall-off position (FOP) measured via line-cone reconstruction, where TOF comprises both the proton transit time from the phantom entrance untilγemission, and the flight time of theγ-ray to the detector. The aim of this study was to implement such a method and investigate the influence of temporal resolution on the precision of the FOP. Monte Carlo simulations of a 160 MeV proton beam incident on a homogeneous PMMA phantom were performed using GATE. The Compton camera consisted of a silicon-based scatterer and CeBr3scintillator absorber. The temporal resolution of the detection system (absorber + beam trigger) was varied between 0.1 and 1.3 ns rms and a TOF-based discrimination method applied to eliminate unlikely solution(s) from the line-cone reconstruction. The FOP was obtained for varying temporal resolutions and its precision obtained from its shift across 100 independentγemission profiles compared to a high statistics reference profile. The optimal temporal resolution for the given camera geometry and 108primary protons was 0.2 ns where a precision of 2.30 ± 0.15 mm (1σ) on the FOP was found. This precision is comparable to current state-of-the-art Compton imaging using iterative reconstruction methods or 1D imaging with mechanically collimated devices, and satisfies the requirement of being smaller than the clinical safety margins.
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Affiliation(s)
- Jayde Livingstone
- Univ Lyon, Université Claude Bernard Lyon 1, CNRS/IN2P3, Institut de Physique des 2 Infinis, F-69622 Villeurbanne, France.,Université Grenoble Alpes, CNRS/IN2P3, Laboratoire de Physique Subatomique et de Cosmologie, F-38026 Grenoble, France
| | - Denis Dauvergne
- Université Grenoble Alpes, CNRS/IN2P3, Laboratoire de Physique Subatomique et de Cosmologie, F-38026 Grenoble, France
| | - Ane Etxebeste
- University of Lyon, INSA-Lyon, Université Claude Bernard Lyon 1, UJM-Saint Etienne, CNRS, Inserm, CREATIS UMR 5220, U1206, F-69373 Lyon, France
| | - Mattia Fontana
- Univ Lyon, Université Claude Bernard Lyon 1, CNRS/IN2P3, Institut de Physique des 2 Infinis, F-69622 Villeurbanne, France
| | - Marie-Laure Gallin-Martel
- Université Grenoble Alpes, CNRS/IN2P3, Laboratoire de Physique Subatomique et de Cosmologie, F-38026 Grenoble, France
| | - Brent Huisman
- University of Lyon, INSA-Lyon, Université Claude Bernard Lyon 1, UJM-Saint Etienne, CNRS, Inserm, CREATIS UMR 5220, U1206, F-69373 Lyon, France
| | - Jean Michel Létang
- University of Lyon, INSA-Lyon, Université Claude Bernard Lyon 1, UJM-Saint Etienne, CNRS, Inserm, CREATIS UMR 5220, U1206, F-69373 Lyon, France
| | - Sara Marcatili
- Université Grenoble Alpes, CNRS/IN2P3, Laboratoire de Physique Subatomique et de Cosmologie, F-38026 Grenoble, France
| | - David Sarrut
- University of Lyon, INSA-Lyon, Université Claude Bernard Lyon 1, UJM-Saint Etienne, CNRS, Inserm, CREATIS UMR 5220, U1206, F-69373 Lyon, France
| | - Étienne Testa
- Université Grenoble Alpes, CNRS/IN2P3, Laboratoire de Physique Subatomique et de Cosmologie, F-38026 Grenoble, France
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13
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Ros García A, Barrio J, Etxebeste A, García López J, Jiménez-Ramos MC, Lacasta C, Muñoz E, Oliver JF, Roser J, Llosá G. MACACO II test-beam with high energy photons. ACTA ACUST UNITED AC 2020; 65:245027. [DOI: 10.1088/1361-6560/abc5cd] [Citation(s) in RCA: 9] [Impact Index Per Article: 2.3] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/12/2022]
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14
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Fischetti M, Baroni G, Battistoni G, Bisogni G, Cerello P, Ciocca M, De Maria P, De Simoni M, Di Lullo B, Donetti M, Dong Y, Embriaco A, Ferrero V, Fiorina E, Franciosini G, Galante F, Kraan A, Luongo C, Magi M, Mancini-Terracciano C, Marafini M, Malekzadeh E, Mattei I, Mazzoni E, Mirabelli R, Mirandola A, Morrocchi M, Muraro S, Patera V, Pennazio F, Schiavi A, Sciubba A, Solfaroli Camillocci E, Sportelli G, Tampellini S, Toppi M, Traini G, Valle SM, Vischioni B, Vitolo V, Sarti A. Inter-fractional monitoring of [Formula: see text]C ions treatments: results from a clinical trial at the CNAO facility. Sci Rep 2020; 10:20735. [PMID: 33244102 PMCID: PMC7693236 DOI: 10.1038/s41598-020-77843-z] [Citation(s) in RCA: 9] [Impact Index Per Article: 2.3] [Reference Citation Analysis] [Abstract] [Key Words] [MESH Headings] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 04/14/2020] [Accepted: 11/13/2020] [Indexed: 12/26/2022] Open
Abstract
The high dose conformity and healthy tissue sparing achievable in Particle Therapy when using C ions calls for safety factors in treatment planning, to prevent the tumor under-dosage related to the possible occurrence of inter-fractional morphological changes during a treatment. This limitation could be overcome by a range monitor, still missing in clinical routine, capable of providing on-line feedback. The Dose Profiler (DP) is a detector developed within the INnovative Solution for In-beam Dosimetry in hadronthErapy (INSIDE) collaboration for the monitoring of carbon ion treatments at the CNAO facility (Centro Nazionale di Adroterapia Oncologica) exploiting the detection of charged secondary fragments that escape from the patient. The DP capability to detect inter-fractional changes is demonstrated by comparing the obtained fragment emission maps in different fractions of the treatments enrolled in the first ever clinical trial of such a monitoring system, performed at CNAO. The case of a CNAO patient that underwent a significant morphological change is presented in detail, focusing on the implications that can be drawn for the achievable inter-fractional monitoring DP sensitivity in real clinical conditions. The results have been cross-checked against a simulation study.
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Affiliation(s)
- M. Fischetti
- Dipartimento di Scienze di Base e Applicate per l’Ingegneria, Sapienza Università di Roma, Rome, Italy
- INFN Sezione di Roma I, Rome, Italy
| | - G. Baroni
- Dipartimento di Elettronica Informazione e Bioingegneria, Politecnico di Milano, Milan, Italy
| | | | - G. Bisogni
- INFN Sezione di Pisa, Pisa, Italy
- Dipartimento di Fisica “E. Fermi”, Università di Pisa, Pisa, Italy
| | | | - M. Ciocca
- CNAO Centro Nazionale di Adroterapia Oncologica, Pavia, Italy
| | - P. De Maria
- Scuola di Specializzazione di Fisica Medica, Sapienza Università di Roma, Rome, Italy
| | - M. De Simoni
- Dipartimento di Fisica, Sapienza Università di Roma, Rome, Italy
- INFN Sezione di Roma I, Rome, Italy
| | - B. Di Lullo
- Dipartimento di Scienze di Base e Applicate per l’Ingegneria, Sapienza Università di Roma, Rome, Italy
| | - M. Donetti
- CNAO Centro Nazionale di Adroterapia Oncologica, Pavia, Italy
| | - Y. Dong
- INFN Sezione di Milano, Milan, Italy
- Dipartimento di Fisica, Università degli Studi di Milano, Milan, Italy
| | | | | | - E. Fiorina
- INFN Sezione di Torino, Turin, Italy
- CNAO Centro Nazionale di Adroterapia Oncologica, Pavia, Italy
| | - G. Franciosini
- Dipartimento di Fisica, Sapienza Università di Roma, Rome, Italy
- INFN Sezione di Roma I, Rome, Italy
| | - F. Galante
- Dipartimento di Scienze di Base e Applicate per l’Ingegneria, Sapienza Università di Roma, Rome, Italy
| | - A. Kraan
- INFN Sezione di Pisa, Pisa, Italy
| | - C. Luongo
- INFN Sezione di Pisa, Pisa, Italy
- Dipartimento di Chimica e Chimica Industriale, Università di Pisa, Pisa, Italy
| | - M. Magi
- Dipartimento di Scienze di Base e Applicate per l’Ingegneria, Sapienza Università di Roma, Rome, Italy
| | - C. Mancini-Terracciano
- Dipartimento di Fisica, Sapienza Università di Roma, Rome, Italy
- INFN Sezione di Roma I, Rome, Italy
| | - M. Marafini
- INFN Sezione di Roma I, Rome, Italy
- Museo Storico della Fisica e Centro Studi e Ricerche “E. Fermi”, Rome, Italy
| | - E. Malekzadeh
- CNAO Centro Nazionale di Adroterapia Oncologica, Pavia, Italy
| | - I. Mattei
- INFN Sezione di Milano, Milan, Italy
| | | | - R. Mirabelli
- Dipartimento di Fisica, Sapienza Università di Roma, Rome, Italy
- INFN Sezione di Roma I, Rome, Italy
- Museo Storico della Fisica e Centro Studi e Ricerche “E. Fermi”, Rome, Italy
| | - A. Mirandola
- CNAO Centro Nazionale di Adroterapia Oncologica, Pavia, Italy
| | - M. Morrocchi
- INFN Sezione di Pisa, Pisa, Italy
- Dipartimento di Fisica “E. Fermi”, Università di Pisa, Pisa, Italy
| | - S. Muraro
- INFN Sezione di Milano, Milan, Italy
| | - V. Patera
- Dipartimento di Scienze di Base e Applicate per l’Ingegneria, Sapienza Università di Roma, Rome, Italy
- INFN Sezione di Roma I, Rome, Italy
- Museo Storico della Fisica e Centro Studi e Ricerche “E. Fermi”, Rome, Italy
| | | | - A. Schiavi
- Dipartimento di Scienze di Base e Applicate per l’Ingegneria, Sapienza Università di Roma, Rome, Italy
- INFN Sezione di Roma I, Rome, Italy
| | - A. Sciubba
- Dipartimento di Scienze di Base e Applicate per l’Ingegneria, Sapienza Università di Roma, Rome, Italy
- INFN Sezione dei Laboratori di Frascati, Rome, Italy
- Museo Storico della Fisica e Centro Studi e Ricerche “E. Fermi”, Rome, Italy
| | - E. Solfaroli Camillocci
- Dipartimento di Fisica, Sapienza Università di Roma, Rome, Italy
- INFN Sezione di Roma I, Rome, Italy
- Scuola di Specializzazione in Fisica Medica, Sapienza Università di Roma, Rome, Italy
| | - G. Sportelli
- INFN Sezione di Pisa, Pisa, Italy
- Dipartimento di Fisica “E. Fermi”, Università di Pisa, Pisa, Italy
| | - S. Tampellini
- CNAO Centro Nazionale di Adroterapia Oncologica, Pavia, Italy
| | - M. Toppi
- Dipartimento di Scienze di Base e Applicate per l’Ingegneria, Sapienza Università di Roma, Rome, Italy
- INFN Sezione dei Laboratori di Frascati, Rome, Italy
| | - G. Traini
- INFN Sezione di Roma I, Rome, Italy
- Museo Storico della Fisica e Centro Studi e Ricerche “E. Fermi”, Rome, Italy
| | | | - B. Vischioni
- CNAO Centro Nazionale di Adroterapia Oncologica, Pavia, Italy
| | - V. Vitolo
- CNAO Centro Nazionale di Adroterapia Oncologica, Pavia, Italy
| | - A. Sarti
- Dipartimento di Scienze di Base e Applicate per l’Ingegneria, Sapienza Università di Roma, Rome, Italy
- INFN Sezione di Roma I, Rome, Italy
- Museo Storico della Fisica e Centro Studi e Ricerche “E. Fermi”, Rome, Italy
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Panthi R, Maggi P, Peterson S, Mackin D, Polf J, Beddar S. Secondary Particle Interactions in a Compton Camera Designed for in vivo Range Verification of Proton Therapy. IEEE TRANSACTIONS ON RADIATION AND PLASMA MEDICAL SCIENCES 2020; 5:383-391. [PMID: 34056151 DOI: 10.1109/trpms.2020.3030166] [Citation(s) in RCA: 3] [Impact Index Per Article: 0.8] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/07/2022]
Abstract
The purpose of this study was to determine the types, proportions, and energies of secondary particle interactions in a Compton camera (CC) during the delivery of clinical proton beams. The delivery of clinical proton pencil beams ranging from 70 to 200 MeV incident on a water phantom was simulated using Geant4 software (version 10.4). The simulation included a CC similar to the configuration of a Polaris J3 CC designed to image prompt gammas (PGs) emitted during proton beam irradiation for the purpose of in vivo range verification. The interaction positions and energies of secondary particles in each CC detector module were scored. For a 150-MeV proton beam, a total of 156,688(575) secondary particles per 108 protons, primarily composed of gamma rays (46.31%), neutrons (41.37%), and electrons (8.88%), were found to reach the camera modules, and 79.37% of these particles interacted with the modules. Strategies for using CCs for proton range verification should include methods of reducing the large neutron backgrounds and low-energy non-PG radiation. The proportions of interaction types by module from this study may provide information useful for background suppression.
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Affiliation(s)
- Rajesh Panthi
- The University of Texas M. D. Anderson Cancer Center, Houston, Texas 77030, USA
| | - Paul Maggi
- University of Maryland School of Medicine, Baltimore, Maryland 21201, USA
| | | | - Dennis Mackin
- The University of Texas M. D. Anderson Cancer Center, Houston, Texas 77030
| | - Jerimy Polf
- University of Maryland School of Medicine, Baltimore, Maryland 21201
| | - Sam Beddar
- University of Texas M. D. Anderson Cancer Center, Houston, TX 77030
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The SiFi-CC project – Feasibility study of a scintillation-fiber-based Compton camera for proton therapy monitoring. Phys Med 2020; 76:317-325. [DOI: 10.1016/j.ejmp.2020.07.013] [Citation(s) in RCA: 8] [Impact Index Per Article: 2.0] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Submit a Manuscript] [Subscribe] [Scholar Register] [Received: 01/31/2020] [Revised: 06/19/2020] [Accepted: 07/09/2020] [Indexed: 11/15/2022] Open
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Feng Y, Etxebeste A, Sarrut D, Letang JM, Maxim V. 3-D Reconstruction Benchmark of a Compton Camera Against a Parallel-Hole Gamma Camera on Ideal Data. IEEE TRANSACTIONS ON RADIATION AND PLASMA MEDICAL SCIENCES 2020. [DOI: 10.1109/trpms.2019.2955745] [Citation(s) in RCA: 6] [Impact Index Per Article: 1.5] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/07/2022]
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18
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Zhang H, Fan P, Wang S, Xia Y, Xu T, Wei Q, Lu W, Wu Z, Liu Y, Ma T. Design and Performance Evaluation of a BGO + SiPM Detector for High-Energy Prompt Gamma Imaging in Proton Therapy Monitoring. IEEE TRANSACTIONS ON RADIATION AND PLASMA MEDICAL SCIENCES 2020. [DOI: 10.1109/trpms.2020.2972594] [Citation(s) in RCA: 4] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/07/2022]
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