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Purushothaman S, Kostyleva D, Dendooven P, Haettner E, Geissel H, Schuy C, Weber U, Boscolo D, Dickel T, Graeff C, Hornung C, Kazantseva E, Kuzminchuk-Feuerstein N, Mukha I, Pietri S, Roesch H, Tanaka YK, Zhao J, Durante M, Parodi K, Scheidenberger C. Quasi-real-time range monitoring by in-beam PET: a case for 15O. Sci Rep 2023; 13:18788. [PMID: 37914762 PMCID: PMC10620432 DOI: 10.1038/s41598-023-45122-2] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 06/03/2023] [Accepted: 10/16/2023] [Indexed: 11/03/2023] Open
Abstract
A fast and reliable range monitoring method is required to take full advantage of the high linear energy transfer provided by therapeutic ion beams like carbon and oxygen while minimizing damage to healthy tissue due to range uncertainties. Quasi-real-time range monitoring using in-beam positron emission tomography (PET) with therapeutic beams of positron-emitters of carbon and oxygen is a promising approach. The number of implanted ions and the time required for an unambiguous range verification are decisive factors for choosing a candidate isotope. An experimental study was performed at the FRS fragment-separator of GSI Helmholtzzentrum für Schwerionenforschung GmbH, Germany, to investigate the evolution of positron annihilation activity profiles during the implantation of [Formula: see text]O and [Formula: see text]O ion beams in a PMMA phantom. The positron activity profile was imaged by a dual-panel version of a Siemens Biograph mCT PET scanner. Results from a similar experiment using ion beams of carbon positron-emitters [Formula: see text]C and [Formula: see text]C performed at the same experimental setup were used for comparison. Owing to their shorter half-lives, the number of implanted ions required for a precise positron annihilation activity peak determination is lower for [Formula: see text]C compared to [Formula: see text]C and likewise for [Formula: see text]O compared to [Formula: see text]O, but their lower production cross-sections make it difficult to produce them at therapeutically relevant intensities. With a similar production cross-section and a 10 times shorter half-life than [Formula: see text]C, [Formula: see text]O provides a faster conclusive positron annihilation activity peak position determination for a lower number of implanted ions compared to [Formula: see text]C. A figure of merit formulation was developed for the quantitative comparison of therapy-relevant positron-emitting beams in the context of quasi-real-time beam monitoring. In conclusion, this study demonstrates that among the positron emitters of carbon and oxygen, [Formula: see text]O is the most feasible candidate for quasi-real-time range monitoring by in-beam PET that can be produced at therapeutically relevant intensities. Additionally, this study demonstrated that the in-flight production and separation method can produce beams of therapeutic quality, in terms of purity, energy, and energy spread.
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Affiliation(s)
- S Purushothaman
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany.
| | - D Kostyleva
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
| | - P Dendooven
- Department of Radiation Oncology, Particle Therapy Research Center (PARTREC), University Medical Center Groningen, University of Groningen, Groningen, The Netherlands
| | - E Haettner
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
| | - H Geissel
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
- II. Physikalisches Institut, Justus-Liebig-Universität, Gießen, Germany
| | - C Schuy
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
| | - U Weber
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
| | - D Boscolo
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
| | - T Dickel
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
- II. Physikalisches Institut, Justus-Liebig-Universität, Gießen, Germany
| | - C Graeff
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
- Department of Electrical Engineering and Information Technology, Technische Universität Darmstadt, Darmstadt, Germany
| | - C Hornung
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
| | - E Kazantseva
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
| | | | - I Mukha
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
| | - S Pietri
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
| | - H Roesch
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
- Institute for Nuclear Physics, Technische Universität Darmstadt, Darmstadt, Germany
| | - Y K Tanaka
- RIKEN Cluster for Pioneering Research, RIKEN, Wako, Japan
| | - J Zhao
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
- School of Physics, Beihang University, Beijing, China
| | - M Durante
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany.
- Department of Condensed Matter Physics, Technische Universität Darmstadt, Darmstadt, Germany.
| | - K Parodi
- Department of Medical Physics, Faculty of Physics, Ludwig-Maximilians Universität München, Munich, Germany
| | - C Scheidenberger
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
- II. Physikalisches Institut, Justus-Liebig-Universität, Gießen, Germany
- Helmholtz Forschungsakademie Hessen für FAIR (HFHF), Campus Gießen, Gießen, Germany
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Haettner E, Geissel H, Franczak B, Kostyleva D, Purushothaman S, Tanaka Y, Amjad F, Boscolo D, Dickel T, Graeff C, Hessler C, Hornung C, Kazantseva E, Kuzminchuk N, Morrissey D, Mukha I, Pietri S, Rocco E, Roy P, Roesch H, Schuy C, Schütt P, Weber U, Weick H, Zhao J, Durante M, Parodi K, Scheidenberger C. Production and separation of positron emitters for hadron therapy at FRS-Cave M. Nucl Instrum Methods Phys Res B 2023; 541:114-116. [PMID: 37265512 PMCID: PMC7614599 DOI: 10.1016/j.nimb.2023.04.026] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/03/2023]
Abstract
The FRagment Separator FRS at GSI is a versatile spectrometer and separator for experiments with relativistic in-flight separated short-lived exotic beams. One branch of the FRS is connected to the target hall where the bio-medical cave (Cave M) is located. Recently a joint activity between the experimental groups of the FRS and the biophysics at the GSI and Department of physics at LMU was started to perform biomedical experiments relevant for hadron therapy with positron emitting carbon and oxygen beams. This paper presents the new ion-optical mode and commissioning results of the FRS-Cave M branch where positron emitting 15O-ions were provided to the medical cave for the first time. An overall conversion efficiency of 2.9±0.2×10-4 15O fragments per primary 16O ion accelerated in the synchrotron SIS18 was reached.
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Affiliation(s)
- E. Haettner
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291, Darmstadt, Germany
| | - H. Geissel
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291, Darmstadt, Germany
- II. Physikalisches Institut, Justus-Liebig-Universität, 35392, Gieβen, Germany
| | - B. Franczak
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291, Darmstadt, Germany
| | - D. Kostyleva
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291, Darmstadt, Germany
| | - S. Purushothaman
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291, Darmstadt, Germany
| | - Y.K. Tanaka
- RIKEN Cluster for Pioneering Research, RIKEN, 351-0198, Saitama, Japan
| | - F. Amjad
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291, Darmstadt, Germany
| | - D. Boscolo
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291, Darmstadt, Germany
| | - T. Dickel
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291, Darmstadt, Germany
- II. Physikalisches Institut, Justus-Liebig-Universität, 35392, Gieβen, Germany
| | - C. Graeff
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291, Darmstadt, Germany
| | - C. Hessler
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291, Darmstadt, Germany
| | - C. Hornung
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291, Darmstadt, Germany
| | - E. Kazantseva
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291, Darmstadt, Germany
| | - N. Kuzminchuk
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291, Darmstadt, Germany
| | - D. Morrissey
- Department of Chemistry and NSCL, Michigan State University, 48824, East Lansing, USA
| | - I. Mukha
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291, Darmstadt, Germany
| | - S. Pietri
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291, Darmstadt, Germany
| | - E. Rocco
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291, Darmstadt, Germany
| | - P. Roy
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291, Darmstadt, Germany
| | - H. Roesch
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291, Darmstadt, Germany
| | - C. Schuy
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291, Darmstadt, Germany
| | - P. Schütt
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291, Darmstadt, Germany
| | - U. Weber
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291, Darmstadt, Germany
| | - H. Weick
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291, Darmstadt, Germany
| | - J. Zhao
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291, Darmstadt, Germany
| | - M. Durante
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291, Darmstadt, Germany
- Institut für Physik Kondensierter Materie, Technische Universität Darmstadt, 64289, Darmstadt, Germany
| | - K. Parodi
- Faculty of Physics, Department of Medical Physics, Ludwig-Maximilians-Universität München, 85748, München, Germany
| | - C. Scheidenberger
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64291, Darmstadt, Germany
- II. Physikalisches Institut, Justus-Liebig-Universität, 35392, Gieβen, Germany
- Helmholtz Research Academy Hesse for FAIR (HFHF), GSI Helmholtz Center for Heavy Ion Research, Campus Gieβen, 35392, Gieβen, Germany
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Kostyleva D, Purushothaman S, Dendooven P, Haettner E, Geissel H, Ozoemelam I, Schuy C, Weber U, Boscolo D, Dickel T, Drozd V, Graeff C, Franczak B, Hornung C, Horst F, Kazantseva E, Kuzminchuk-Feuerstein N, Mukha I, Nociforo C, Pietri S, Reidel CA, Roesch H, Tanaka YK, Weick H, Zhao J, Durante M, Parodi K, Scheidenberger C. Precision of the PET activity range during irradiation with 10C, 11C, and 12C beams. Phys Med Biol 2022; 68. [PMID: 36533621 DOI: 10.1088/1361-6560/aca5e8] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 10/02/2022] [Accepted: 11/24/2022] [Indexed: 11/25/2022]
Abstract
Objective. Beams of stable ions have been a well-established tool for radiotherapy for many decades. In the case of ion beam therapy with stable12C ions, the positron emitters10,11C are produced via projectile and target fragmentation, and their decays enable visualization of the beam via positron emission tomography (PET). However, the PET activity peak matches the Bragg peak only roughly and PET counting statistics is low. These issues can be mitigated by using a short-lived positron emitter as a therapeutic beam.Approach.An experiment studying the precision of the measurement of ranges of positron-emitting carbon isotopes by means of PET has been performed at the FRS fragment-separator facility of GSI Helmholtzzentrum für Schwerionenforschung GmbH, Germany. The PET scanner used in the experiment is a dual-panel version of a Siemens Biograph mCT PET scanner.Main results.High-quality in-beam PET images and activity distributions have been measured from the in-flight produced positron emitting isotopes11C and10C implanted into homogeneous PMMA phantoms. Taking advantage of the high statistics obtained in this experiment, we investigated the time evolution of the uncertainty of the range determined by means of PET during the course of irradiation, and show that the uncertainty improves with the inverse square root of the number of PET counts. The uncertainty is thus fully determined by the PET counting statistics. During the delivery of 1.6 × 107ions in 4 spills for a total duration of 19.2 s, the PET activity range uncertainty for10C,11C and12C is 0.04 mm, 0.7 mm and 1.3 mm, respectively. The gain in precision related to the PET counting statistics is thus much larger when going from11C to10C than when going from12C to11C. The much better precision for10C is due to its much shorter half-life, which, contrary to the case of11C, also enables to include the in-spill data in the image formation.Significance. Our results can be used to estimate the contribution from PET counting statistics to the precision of range determination in a particular carbon therapy situation, taking into account the irradiation scenario, the required dose and the PET scanner characteristics.
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Affiliation(s)
- D Kostyleva
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
| | - S Purushothaman
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
| | - P Dendooven
- Particle Therapy Research Center (PARTREC), Department of Radiation Oncology, University Medical Center Groningen, University of Groningen, Groningen, The Netherlands
| | - E Haettner
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
| | - H Geissel
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany.,II. Physikalisches Institut, Justus-Liebig-Universität, Gießen, Germany
| | - I Ozoemelam
- Fontys University of Applied Sciences, Eindhoven, The Netherlands
| | - C Schuy
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
| | - U Weber
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
| | - D Boscolo
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
| | - T Dickel
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany.,II. Physikalisches Institut, Justus-Liebig-Universität, Gießen, Germany
| | - V Drozd
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany.,Faculty of Science and Engineering, University of Groningen, Groningen, The Netherlands
| | - C Graeff
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
| | - B Franczak
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
| | - C Hornung
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
| | - F Horst
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
| | - E Kazantseva
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
| | | | - I Mukha
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
| | - C Nociforo
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
| | - S Pietri
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
| | - C A Reidel
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
| | - H Roesch
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany.,Institute for Nuclear Physics, Technische Universität Darmstadt, Darmstadt, Germany
| | - Y K Tanaka
- RIKEN Cluster for Pioneering Research, Wako, Japan
| | - H Weick
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
| | - J Zhao
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany.,School of Physics, Beihang University, Beijing, People's Republic of China
| | - M Durante
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany.,Department of Condensed Matter Physics, Technische Universität Darmstadt, Darmstadt, Germany
| | - K Parodi
- Department of Physics, Ludwig-Maximilians Universität München, Munich, Germany
| | - C Scheidenberger
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany.,II. Physikalisches Institut, Justus-Liebig-Universität, Gießen, Germany.,Helmholtz Forschungsakademie Hessen für FAIR (HFHF), Campus Gießen, Gießen, Germany
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Rädler M, Buizza G, Palaniappan P, Gianoli C, Baroni G, Paganelli C, Parodi K, Riboldi M. PD-0899 Magnetic field of a proton pencil beam as range verification method: The impact of secondaries. Radiother Oncol 2022. [DOI: 10.1016/s0167-8140(22)02978-4] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/30/2022]
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Dedes G, Drosten H, Götz S, Dickmann J, Sarosiek C, Pankuch M, Krah N, Rit S, Bashkirov V, Schulte RW, Johnson RP, Parodi K, DeJongh E, Landry G. Comparative accuracy and resolution assessment of two prototype proton computed tomography scanners. Med Phys 2022; 49:4671-4681. [PMID: 35396739 DOI: 10.1002/mp.15657] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 11/25/2021] [Revised: 02/14/2022] [Accepted: 03/07/2022] [Indexed: 11/10/2022] Open
Abstract
BACKGROUND Improving the accuracy of relative stopping power (RSP) in proton therapy may allow reducing range margins. Proton computed tomography (pCT) has been shown to provide state-of-the-art RSP accuracy estimation, and various scanner prototypes have recently been built. The different approaches used in scanner design are expected to impact spatial resolution and RSP accuracy. PURPOSE The goal of this study was to perform the first direct comparison, in terms of spatial resolution and RSP accuracy, of two pCT prototype scanners installed at the same facility and by using the same image reconstruction algorithm. METHODS A phantom containing cylindrical inserts of known RSP was scanned at the phase-II pCT prototype of the U.S. pCT collaboration and at the commercially oriented ProtonVDA scanner. Following distance-driven binning filtered backprojection reconstruction, the radial edge spread function of high-density inserts was used to estimate the spatial resolution. RSP accuracy was evaluated by the mean absolute percent error (MAPE) over the inserts. No direct imaging dose estimation was possible, which prevented a comparison of the two scanners in terms of RSP noise. RESULTS In terms of RSP accuracy, both scanners achieved the same MAPE of 0.72% when excluding the porous sinus insert from the evaluation. The ProtonVDA scanner reached a better overall MAPE when all inserts and the body of the phantom were accounted for (0.81%), compared to the phase-II scanner (1.14%). The spatial resolution with the phase-II scanner was found to be 0.61 lp/mm, while for the ProtonVDA scanner somewhat lower at 0.46 lp/mm. CONCLUSIONS The comparison between two prototype pCT scanners operated in the same clinical facility showed that they both fulfill the requirement of an RSP accuracy of about 1%. Their spatial resolution performance reflects the different design choices of either a scanner with full tracking capabilities (phase-II) or of a more compact tracker system which only provides the positions of protons but not their directions (ProtonVDA). This article is protected by copyright. All rights reserved.
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Affiliation(s)
- G Dedes
- Department of Medical Physics, Faculty of Physics, Ludwig-Maximilians-Universität München, Am Coulombwall 1, Garching b. München, 85748, Germany
| | - H Drosten
- Department of Medical Physics, Faculty of Physics, Ludwig-Maximilians-Universität München, Am Coulombwall 1, Garching b. München, 85748, Germany
| | - S Götz
- Department of Medical Physics, Faculty of Physics, Ludwig-Maximilians-Universität München, Am Coulombwall 1, Garching b. München, 85748, Germany
| | - J Dickmann
- Department of Medical Physics, Faculty of Physics, Ludwig-Maximilians-Universität München, Am Coulombwall 1, Garching b. München, 85748, Germany
| | - C Sarosiek
- Department of Physics, Northern Illinois University, 1425 W. Lincoln Highway DeKalb, Illinois, IL, 60115, United States of America
| | - M Pankuch
- Northwestern Medicine Chicago Proton Center, 4455 Weaver Parkway, Warrenville, Illinois, IL, 60555, United States of America
| | - N Krah
- University of Lyon, INSA-Lyon, Université Claude Bernard Lyon 1, UJM-Saint Etienne, CNRS, Inserm, CREATIS UMR 5220, U1294, LYON, F-69373, France
| | - S Rit
- University of Lyon, INSA-Lyon, Université Claude Bernard Lyon 1, UJM-Saint Etienne, CNRS, Inserm, CREATIS UMR 5220, U1294, LYON, F-69373, France
| | - V Bashkirov
- Division of Biomedical Engineering Sciences, Loma Linda University, Loma Linda, California, CA 92354, United States of America
| | - R W Schulte
- Division of Biomedical Engineering Sciences, Loma Linda University, Loma Linda, California, CA 92354, United States of America
| | - R P Johnson
- Department of Physics, U.C. Santa Cruz, 1156 High Street Santa Cruz, California, CA, 95064, United States of America
| | - K Parodi
- Department of Medical Physics, Faculty of Physics, Ludwig-Maximilians-Universität München, Am Coulombwall 1, Garching b. München, 85748, Germany
| | - E DeJongh
- ProtonVDA LLC, 1700 Park Street STE 208, Naperville, Illinois, IL, 60563, United States of America
| | - G Landry
- Department of Medical Physics, Faculty of Physics, Ludwig-Maximilians-Universität München, Am Coulombwall 1, Garching b. München, 85748, Germany.,Department of Radiation Oncology, University Hospital, LMU Munich, Munich, 81377, Germany.,German Cancer Consortium (DKTK), Munich, 81377, Germany
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Götz S, Dickmann J, Rit S, Krah N, Khellaf F, Schulte RW, Parodi K, Dedes G, Landry G. Evaluation of the impact of a scanner prototype on proton CT and helium CT image quality and dose efficiency with Monte Carlo simulation. Phys Med Biol 2022; 67. [PMID: 35086073 DOI: 10.1088/1361-6560/ac4fa4] [Citation(s) in RCA: 2] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 11/08/2021] [Accepted: 01/27/2022] [Indexed: 11/12/2022]
Abstract
Objective.The use of ion computed tomography (CT) promises to yield improved relative stopping power (RSP) estimation as input to particle therapy treatment planning. Recently, proton CT (pCT) has been shown to yield RSP accuracy on par with state-of-the-art x-ray dual energy CT. There are however concerns that the lower spatial resolution of pCT compared to x-ray CT may limit its potential, which has spurred interest in the use of helium ion CT (HeCT). The goal of this study was to investigate image quality of pCT and HeCT in terms of noise, spatial resolution, RSP accuracy and imaging dose using a detailed Monte Carlo (MC) model of an existing ion CT prototype.Approach.Three phantoms were used in simulated pCT and HeCT scans allowing estimation of noise, spatial resolution and the scoring of dose. An additional phantom was used to evaluate RSP accuracy. The imaging dose required to achieve the same image noise in a water and a head phantom was estimated at both native spatial resolution, and in a scenario where the HeCT spatial resolution was reduced and matched to that of pCT using Hann windowing of the reconstruction filter. A variance reconstruction formalism was adapted to account for Hann windowing.Main results.We confirmed that the scanner prototype would produce higher spatial resolution for HeCT than pCT by a factor 1.8 (0.86 lp mm-1versus 0.48 lp mm-1at the center of a 20 cm water phantom). At native resolution, HeCT required a factor 2.9 more dose than pCT to achieve the same noise, while at matched resolution, HeCT required only 38% of the pCT dose. Finally, RSP mean absolute percent error (MAPE) was found to be 0.59% for pCT and 0.67% for HeCT.Significance.This work compared the imaging performance of pCT and HeCT when using an existing scanner prototype, with the spatial resolution advantage of HeCT coming at the cost of increased dose. When matching spatial resolution via Hann windowing, HeCT had a substantial dose advantage. Both modalities provided state-of-the-art RSP MAPE. HeCT might therefore help reduce the dose exposure of patients with comparable image noise to pCT, enhanced spatial resolution and acceptable RSP accuracy at the same time.
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Affiliation(s)
- S Götz
- Department of Medical Physics, Fakultät für Physik, Ludwig-Maximilians-Universität München (LMU Munich), D-85748 Garching bei München, Germany
| | - J Dickmann
- Department of Medical Physics, Fakultät für Physik, Ludwig-Maximilians-Universität München (LMU Munich), D-85748 Garching bei München, Germany
| | - S Rit
- University of Lyon, INSA-Lyon, Unversité Claude Bernard Lyon 1, UJM-Saint Etienne, CNRS, Inserm, CREATIS, UMR 5220, U1294 F-69373, Lyon, France
| | - N Krah
- University of Lyon, INSA-Lyon, Unversité Claude Bernard Lyon 1, UJM-Saint Etienne, CNRS, Inserm, CREATIS, UMR 5220, U1294 F-69373, Lyon, France.,IP2I, UMR 5822 F-69622, Villeurbanne, France
| | - F Khellaf
- University of Lyon, INSA-Lyon, Unversité Claude Bernard Lyon 1, UJM-Saint Etienne, CNRS, Inserm, CREATIS, UMR 5220, U1294 F-69373, Lyon, France
| | - R W Schulte
- Division of Biomedical Engineering Sciences, Loma Linda University, Loma Linda, CA 92354, United States of America
| | - K Parodi
- Department of Medical Physics, Fakultät für Physik, Ludwig-Maximilians-Universität München (LMU Munich), D-85748 Garching bei München, Germany
| | - G Dedes
- Department of Medical Physics, Fakultät für Physik, Ludwig-Maximilians-Universität München (LMU Munich), D-85748 Garching bei München, Germany
| | - G Landry
- Department of Medical Physics, Fakultät für Physik, Ludwig-Maximilians-Universität München (LMU Munich), D-85748 Garching bei München, Germany.,Department of Radiation Oncology, University Hospital, LMU Munich, D-81377 Munich, Germany.,German Cancer Consortium (DKTK), D-81377 Munich, Germany
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7
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Flacco A, Bayart E, Cavallone M, De Marzi L, Patriarca A, Lamarre-Jouenne I, Schreiber J, Rösch T, Parodi K, Grangeon T. FLASH Modalities Track (Oral Presentations) LASER-DRIVEN PROTON SOURCE FOR IN-VITRO AND IN-VIVO HIGH DOSE, ULTRA-HIGH DOSE-RATE EXPERIMENTS. Phys Med 2022. [DOI: 10.1016/s1120-1797(22)01542-3] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Submit a Manuscript] [Subscribe] [Scholar Register] [Indexed: 11/16/2022] Open
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8
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Schauer J, Lascaud J, Huang Y, Vidal M, Hérault J, Dollinger G, Parodi K, Wieser HP. FEASABILITY STUDY OF IONOACOUSTIC SIGNAL DETECTION UNDER FLASH CONDITIONS AT A CLINICAL SYNCHROCYLOTRON FACILITY. Phys Med 2022. [DOI: 10.1016/s1120-1797(22)01696-9] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Submit a Manuscript] [Subscribe] [Scholar Register] [Indexed: 10/19/2022] Open
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9
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Balling F, Hartmann J, Rösch T, Tischendorf L, Doyle L, Berndl M, Gerlach S, Parodi K, Schreiber J. LASER-DRIVEN ION ACCELERATION BEAMLINE AT THE CENTRE FOR ADVANCED LASER APPLICATIONS. Phys Med 2022. [DOI: 10.1016/s1120-1797(22)01581-2] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Submit a Manuscript] [Subscribe] [Scholar Register] [Indexed: 11/16/2022] Open
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10
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Gerlach S, Kirsch L, Trautmann C, Assmann W, Parodi K, Schreiber J. BEAM MONITORING OF ULTRA-HIGH DOSE RATES: THE TI-BEAT DETECTOR. Phys Med 2022. [DOI: 10.1016/s1120-1797(22)01576-9] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Submit a Manuscript] [Subscribe] [Scholar Register] [Indexed: 11/17/2022] Open
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11
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Gerlach S, Balling F, Anna-Katharina S, Brack FE, Kirsch L, Kroll F, Schramm U, Zeil K, Assmann W, Parodi K, Schreiber J. PARTICLE DOSIMETRY FOR PULSED ULTRA-HIGH PEAK DOSE RATES: THE I-BEAT DETECTOR. Phys Med 2022. [DOI: 10.1016/s1120-1797(22)01580-0] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Submit a Manuscript] [Subscribe] [Scholar Register] [Indexed: 11/28/2022] Open
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12
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Lascaud J, Pinto M, Dash P, Wieser HP, Rouffaud R, Certon D, Sitarz M, Poulsen P, Parodi K. FLASH Modalities Track (Oral Presentations) FEASIBILITY STUDY OF TRANSIENT IONOACOUSTICS-BASED PROTON BEAM MONITORING FOR SMALL ANIMAL IRRADIATION AT CYCLOTRON-BASED CLINICAL FACILITIES UNDER FLASH CONDITIONS. Phys Med 2022. [DOI: 10.1016/s1120-1797(22)01475-2] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Submit a Manuscript] [Subscribe] [Scholar Register] [Indexed: 10/19/2022] Open
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13
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Wieser HP, Huang Y, Schauer J, Lascaud J, Würl M, Lehrack S, Radonic D, Vidal M, Hérault J, Chmyrov A, Ntziachristos V, Assmann W, Parodi K, Dollinger G. Experimental demonstration of accurate Bragg peak localization with ionoacoustic tandem phase detection (iTPD). Phys Med Biol 2021; 66. [PMID: 34847532 DOI: 10.1088/1361-6560/ac3ead] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.7] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 09/21/2021] [Accepted: 11/30/2021] [Indexed: 11/12/2022]
Abstract
Accurate knowledge of the exact stopping location of ions inside the patient would allow full exploitation of their ballistic properties for patient treatment. The localized energy deposition of a pulsed particle beam induces a rapid temperature increase of the irradiated volume and leads to the emission of ionoacoustic (IA) waves. Detecting the time-of-flight (ToF) of the IA wave allows inferring information on the Bragg peak location and can henceforth be used forin-vivorange verification. A challenge for IA is the poor signal-to-noise ratio at clinically relevant doses and viable machines. We present a frequency-based measurement technique, labeled as ionoacoustic tandem phase detection (iTPD) utilizing lock-in amplifiers. The phase shift of the IA signal to a reference signal is measured to derive theToF. Experimental IA measurements with a 3.5 MHz lead zirconate titanate (PZT) transducer and lock-in amplifiers were performed in water using 22 MeV proton bursts. A digital iTPD was performedin-silicoat clinical dose levels on experimental data obtained from a clinical facility and secondly, on simulations emulating a heterogeneous geometry. For the experimental setup using 22 MeV protons, a localization accuracy and precision obtained through iTPD deviates from a time-based reference analysis by less than 15μm. Several methodological aspects were investigated experimentally in systematic manner. Lastly, iTPD was evaluatedin-silicofor clinical beam energies indicating that iTPD is in reach of sub-mm accuracy for fractionated doses < 5 Gy. iTPD can be used to accurately measure theToFof IA signals online via its phase shift in frequency domain. An application of iTPD to the clinical scenario using a single pulsed beam is feasible but requires further development to reach <1 Gy detection capabilities.
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Affiliation(s)
- H P Wieser
- Department for Medical Physics, Faculty of Physics, Ludwig-Maximilians-Universität München, D-85748 Garching b. München, Germany
| | - Y Huang
- Chair of Biological Imaging (CBI) and Center for Translational Cancer Research (TranslaTUM) Technical University Munich, D-81675 Munich, Germany.,Institute of Biological and Medical Imaging (IBMI), Helmholtz Zentrum München, D-85764 Neuherberg, Germany
| | - J Schauer
- Institute for Applied Physics and Metrology, Department of Aerospace Engineering, Universität der Bundeswehr München, D-85577 Neubiberg, Germany
| | - J Lascaud
- Department for Medical Physics, Faculty of Physics, Ludwig-Maximilians-Universität München, D-85748 Garching b. München, Germany
| | - M Würl
- Department for Medical Physics, Faculty of Physics, Ludwig-Maximilians-Universität München, D-85748 Garching b. München, Germany
| | - S Lehrack
- Department for Medical Physics, Faculty of Physics, Ludwig-Maximilians-Universität München, D-85748 Garching b. München, Germany
| | - D Radonic
- Department for Medical Physics, Faculty of Physics, Ludwig-Maximilians-Universität München, D-85748 Garching b. München, Germany
| | - M Vidal
- Centre Antoine Lacassagne-Fédération Claude Lalanne, 227 avenue de Lanterne, F-06200 Nice, France
| | - J Hérault
- Centre Antoine Lacassagne-Fédération Claude Lalanne, 227 avenue de Lanterne, F-06200 Nice, France
| | - A Chmyrov
- Chair of Biological Imaging (CBI) and Center for Translational Cancer Research (TranslaTUM) Technical University Munich, D-81675 Munich, Germany.,Institute of Biological and Medical Imaging (IBMI), Helmholtz Zentrum München, D-85764 Neuherberg, Germany
| | - V Ntziachristos
- Chair of Biological Imaging (CBI) and Center for Translational Cancer Research (TranslaTUM) Technical University Munich, D-81675 Munich, Germany.,Institute of Biological and Medical Imaging (IBMI), Helmholtz Zentrum München, D-85764 Neuherberg, Germany
| | - W Assmann
- Department for Medical Physics, Faculty of Physics, Ludwig-Maximilians-Universität München, D-85748 Garching b. München, Germany
| | - K Parodi
- Department for Medical Physics, Faculty of Physics, Ludwig-Maximilians-Universität München, D-85748 Garching b. München, Germany
| | - G Dollinger
- Institute for Applied Physics and Metrology, Department of Aerospace Engineering, Universität der Bundeswehr München, D-85577 Neubiberg, Germany
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14
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Martins J, Maier J, Gianoli C, Alhazmi A, Neppl S, Reiner M, Belka C, Veloza S, Kachelriess M, Parodi K. Towards real-time EPID-based 3D in-vivo dosimetry using machine learning. Phys Med 2021. [DOI: 10.1016/s1120-1797(22)00014-x] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Submit a Manuscript] [Subscribe] [Scholar Register] [Indexed: 11/26/2022] Open
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15
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Martins J, Maier J, Gianoli C, Alhazmi A, Neppl S, Reiner M, Belka C, Veloza S, Kachelriess M, Parodi K. Towards real-time EPID-based 3D in-vivo dosimetry using machine learning. Phys Med 2021. [DOI: 10.1016/s1120-1797(22)00158-2] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Submit a Manuscript] [Subscribe] [Scholar Register] [Indexed: 11/27/2022] Open
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16
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Schnürle K, Bortfeldt J, Englbrecht F, Gianoli C, Hartmann J, Hofverberg P, Meyer S, Vidal M, Hérault J, Schreiber J, Parodi K, Würl M. Development of integration mode proton imaging with a single CMOS detector for a small animal irradiation platform. Phys Med 2021. [DOI: 10.1016/s1120-1797(22)00094-1] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Submit a Manuscript] [Subscribe] [Scholar Register] [Indexed: 11/30/2022] Open
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17
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Hofmaier J, Walter F, Hadi I, Rottler M, von Bestenbostel R, Dedes G, Parodi K, Niyazi M, Belka C, Kamp F. PH-0598 Variance-based sensitivity analysis of inter-observer, range and setup variability in proton therapy. Radiother Oncol 2021. [DOI: 10.1016/s0167-8140(21)07370-9] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/27/2022]
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18
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Kawula M, Binder TM, Liprandi S, Viegas R, Parodi K, Thirolf PG. Sub-millimeter precise photon interaction position determination in large monolithic scintillators via convolutional neural network algorithms. Phys Med Biol 2021; 66. [PMID: 34062523 DOI: 10.1088/1361-6560/ac06e2] [Citation(s) in RCA: 4] [Impact Index Per Article: 1.3] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 02/21/2021] [Accepted: 06/01/2021] [Indexed: 11/11/2022]
Abstract
In this work, we present the development and application of a convolutional neural network (CNN)-based algorithm to precisely determine the interaction position ofγ-quanta in large monolithic scintillators. Those are used as an absorber component of a Compton camera (CC) system under development for ion beam range verification via prompt-gamma imaging. We examined two scintillation crystals: LaBr3:Ce and CeBr3. Each crystal had dimensions of 50.8 mm × 50.8 mm × 30 mm and was coupled to a 64-fold segmented multi-anode photomultiplier tube (PMT) with an 8 × 8 pixel arrangement. We determined the spatial resolution for three photon energies of 662, 1.17 and 1.33 MeV obtained from 2D detector scans with tightly collimated137Cs and60Co photon sources. With the new algorithm we achieved a spatial resolution for the CeBr3 crystal below 1.11(8) mm and below 0.98(7) mm for the LaBr3:Ce detector for all investigated energies between 662 keV and 1.33 MeV. We thereby improved the performance by more than a factor of 2.5 compared to the previously used categorical average pattern algorithm, which is a variation of the well-established k-nearest neighbor algorithm. The trained CNN has a low memory footprint and enables the reconstruction of up to 104events per second with only one GPU. Those improvements are crucial on the way to future clinicalin vivoapplicability of the CC for ion beam range verification.
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Affiliation(s)
- M Kawula
- Department of Medical Physics, Ludwig-Maximilians-Universität München, Garching b. München, Germany
| | - T M Binder
- Department of Medical Physics, Ludwig-Maximilians-Universität München, Garching b. München, Germany.,KETEK GmbH, Munich, Germany
| | - S Liprandi
- Department of Medical Physics, Ludwig-Maximilians-Universität München, Garching b. München, Germany
| | - R Viegas
- Department of Medical Physics, Ludwig-Maximilians-Universität München, Garching b. München, Germany.,University of Coimbra, Portugal
| | - K Parodi
- Department of Medical Physics, Ludwig-Maximilians-Universität München, Garching b. München, Germany
| | - P G Thirolf
- Department of Medical Physics, Ludwig-Maximilians-Universität München, Garching b. München, Germany
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19
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Gerlach S, Pinto M, Kurichiyanil N, Grau C, Hérault J, Hillbrand M, Poulsen PR, Safai S, Schippers JM, Schwarz M, Søndergaard CS, Tommasino F, Verroi E, Vidal M, Yohannes I, Schreiber J, Parodi K. Corrigendum: Beam characterization and feasibility study for a small animal irradiation platform at clinical proton therapy facilities (2020 Phys. Med. Biol.65 245045). Phys Med Biol 2021; 66. [PMID: 34037545 DOI: 10.1088/1361-6560/abf00e] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Key Words] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 03/05/2021] [Accepted: 03/18/2021] [Indexed: 11/11/2022]
Affiliation(s)
- S Gerlach
- Department for Medical Physics, Ludwig-Maximilians-Universität München, Am Coulombwall 1, D-85748 Garching, Germany
| | - M Pinto
- Department for Medical Physics, Ludwig-Maximilians-Universität München, Am Coulombwall 1, D-85748 Garching, Germany
| | - N Kurichiyanil
- Department for Medical Physics, Ludwig-Maximilians-Universität München, Am Coulombwall 1, D-85748 Garching, Germany
| | - C Grau
- Department of Oncology, Aarhus University Hospital, Aarhus, Denmark.,Danish Center for Particle Therapy, Aarhus University Hospital, Aarhus, Denmark
| | - J Hérault
- Centre Antoine Lacassagne, Nice, France.,Fédération Claude Lalanne-Université Côte d'Azur, Nice, France
| | - M Hillbrand
- Rinecker Proton Therapy Center, München, Germany
| | - P R Poulsen
- Department of Oncology, Aarhus University Hospital, Aarhus, Denmark.,Danish Center for Particle Therapy, Aarhus University Hospital, Aarhus, Denmark
| | - S Safai
- Paul Scherrer Institute, Villigen, Switzerland
| | | | - M Schwarz
- Trento Institute for Fundamental Physics and Applications, National Institute for Nuclear Physics, Povo, Italy.,Protontherapy Department, Azienda Provinciale per i Servizi Sanitari, Trento, Italy
| | - C S Søndergaard
- Danish Center for Particle Therapy, Aarhus University Hospital, Aarhus, Denmark
| | - F Tommasino
- Trento Institute for Fundamental Physics and Applications, National Institute for Nuclear Physics, Povo, Italy.,Department of Physics, University of Trento, Povo, Italy
| | - E Verroi
- Trento Institute for Fundamental Physics and Applications, National Institute for Nuclear Physics, Povo, Italy
| | - M Vidal
- Centre Antoine Lacassagne, Nice, France.,Fédération Claude Lalanne-Université Côte d'Azur, Nice, France
| | - I Yohannes
- Rinecker Proton Therapy Center, München, Germany
| | - J Schreiber
- Department for Medical Physics, Ludwig-Maximilians-Universität München, Am Coulombwall 1, D-85748 Garching, Germany
| | - K Parodi
- Department for Medical Physics, Ludwig-Maximilians-Universität München, Am Coulombwall 1, D-85748 Garching, Germany
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20
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Niepel KB, Stanislawski M, Wuerl M, Doerringer F, Pinto M, Dietrich O, Ertl-Wagner B, Lalonde A, Bouchard H, Pappas E, Yohannes I, Hillbrand M, Landry G, Parodi K. Animal tissue-based quantitative comparison of dual-energy CT to SPR conversion methods using high-resolution gel dosimetry. Phys Med Biol 2021; 66. [DOI: 10.1088/1361-6560/abbd14] [Citation(s) in RCA: 6] [Impact Index Per Article: 2.0] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 06/10/2020] [Accepted: 09/30/2020] [Indexed: 12/16/2022]
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21
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Dickmann J, Kamp F, Hillbrand M, Corradini S, Belka C, Schulte RW, Parodi K, Dedes G, Landry G. Fluence-modulated proton CT optimized with patient-specific dose and variance objectives for proton dose calculation. Phys Med Biol 2021; 66:064001. [PMID: 33545701 DOI: 10.1088/1361-6560/abe3d2] [Citation(s) in RCA: 4] [Impact Index Per Article: 1.3] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/11/2022]
Abstract
Particle therapy treatment planning requires accurate volumetric maps of the relative stopping power, which can directly be acquired using proton computed tomography (pCT). With fluence-modulated pCT (FMpCT) imaging fluence is concentrated in a region-of-interest (ROI), which can be the vicinity of the treatment beam path, and imaging dose is reduced elsewhere. In this work we present a novel optimization algorithm for FMpCT which, for the first time, calculates modulated imaging fluences for joint imaging dose and image variance objectives. Thereby, image quality is maintained in the ROI to ensure accurate calculations of the treatment dose, and imaging dose is minimized outside the ROI with stronger minimization penalties given to imaging organs-at-risk. The optimization requires an initial scan at uniform fluence or a previous x-ray CT scan. We simulated and optimized FMpCT images for three pediatric patients with tumors in the head region. We verified that the target image variance inside the ROI was achieved and demonstrated imaging dose reductions outside of the ROI of 74% on average, reducing the imaging dose from 1.2 to 0.3 mGy. Such dose savings are expected to be relevant compared to the therapeutic dose outside of the treatment field. Treatment doses were re-calculated on the FMpCT images and compared to treatment doses re-recalculated on uniform fluence pCT scans using a 1% criterion. Passing rates were above 98.3% for all patients. Passing rates comparing FMpCT treatment doses to the ground truth treatment dose were above 88.5% for all patients. Evaluation of the proton range with a 1 mm criterion resulted in passing rates above 97.5% (FMpCT/pCT) and 95.3% (FMpCT/ground truth). Jointly optimized fluence-modulated pCT images can be used for proton dose calculation maintaining the full dosimetric accuracy of pCT but reducing the required imaging dose considerably by three quarters. This may allow for daily imaging during particle therapy ensuring a safe and accurate delivery of the therapeutic dose and avoiding excess dose from imaging.
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Affiliation(s)
- J Dickmann
- Department of Medical Physics, Fakultät für Physik, Ludwig-Maximilians-Universität München (LMU Munich), D-85748 Garching bei München, Germany
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22
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Gerlach S, Pinto M, Kurichiyanil N, Grau C, Hérault J, Hillbrand M, Poulsen PR, Safai S, Schippers JM, Schwarz M, Søndergaard CS, Tommasino F, Verroi E, Vidal M, Yohannes I, Schreiber J, Parodi K. Beam characterization and feasibility study for a small animal irradiation platform at clinical proton therapy facilities. Phys Med Biol 2020; 65:245045. [DOI: 10.1088/1361-6560/abc832] [Citation(s) in RCA: 5] [Impact Index Per Article: 1.3] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/12/2022]
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23
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Kroll C, Dietrich O, Bortfeldt J, Kamp F, Neppl S, Belka C, Parodi K, Baroni G, Paganelli C, Riboldi M. Integration of spatial distortion effects in a 4D computational phantom for simulation studies in extra-cranial MRI-guided radiation therapy: Initial results. Med Phys 2020; 48:1646-1660. [PMID: 33220073 DOI: 10.1002/mp.14611] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 10/01/2019] [Revised: 09/15/2020] [Accepted: 09/16/2020] [Indexed: 12/18/2022] Open
Abstract
PURPOSE Spatial distortions in magnetic resonance imaging (MRI) are mainly caused by inhomogeneities of the static magnetic field, nonlinearities in the applied gradients, and tissue-specific magnetic susceptibility variations. These factors may significantly alter the geometrical accuracy of the reconstructed MR image, thus questioning the reliability of MRI for guidance in image-guided radiation therapy. In this work, we quantified MRI spatial distortions and created a quantitative model where different sources of distortions can be separated. The generated model was then integrated into a four-dimensional (4D) computational phantom for simulation studies in MRI-guided radiation therapy at extra-cranial sites. METHODS A geometrical spatial distortion phantom was designed in four modules embedding laser-cut PMMA grids, providing 3520 landmarks in a field of view of (345 × 260 × 480) mm3 . The construction accuracy of the phantom was verified experimentally. Two fast MRI sequences for extra-cranial imaging at 1.5 T were investigated, considering axial slices acquired with online distortion correction, in order to mimic practical use in MRI-guided radiotherapy. Distortions were separated into their sources by acquisition of images with gradient polarity reversal and dedicated susceptibility calculations. Such a separation yielded a quantitative spatial distortion model to be used for MR imaging simulations. Finally, the obtained spatial distortion model was embedded into an anthropomorphic 4D computational phantom, providing registered virtual CT/MR images where spatial distortions in MRI acquisition can be simulated. RESULTS The manufacturing accuracy of the geometrical distortion phantom was quantified to be within 0.2 mm in the grid planes and 0.5 mm in depth, including thickness variations and bending effects of individual grids. Residual spatial distortions after MRI distortion correction were strongly influenced by the applied correction mode, with larger effects in the trans-axial direction. In the axial plane, gradient nonlinearities caused the main distortions, with values up to 3 mm in a 1.5 T magnet, whereas static field and susceptibility effects were below 1 mm. The integration in the 4D anthropomorphic computational phantom highlighted that deformations can be severe in the region of the thoracic diaphragm, especially when using axial imaging with 2D distortion correction. Adaptation of the phantom based on patient-specific measurements was also verified, aiming at increased realism in the simulation. CONCLUSIONS The implemented framework provides an integrated approach for MRI spatial distortion modeling, where different sources of distortion can be quantified in time-dependent geometries. The computational phantom represents a valuable platform to study motion management strategies in extra-cranial MRI-guided radiotherapy, where the effects of spatial distortions can be modeled on synthetic images in a virtual environment.
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Affiliation(s)
- C Kroll
- Department of Medical Physics, Ludwig-Maximilians University, Garching, 85748, Germany
| | - O Dietrich
- Department of Radiology, University Hospital, LMU Munich, Munich, 81377, Germany
| | - J Bortfeldt
- Department of Medical Physics, Ludwig-Maximilians University, Garching, 85748, Germany.,European Organization for Nuclear Research (CERN), Geneva 23, 1211, Switzerland
| | - F Kamp
- Department of Radiation Oncology, University Hospital, LMU Munich, Munich, 81377, Germany
| | - S Neppl
- Department of Radiation Oncology, University Hospital, LMU Munich, Munich, 81377, Germany
| | - C Belka
- Department of Radiation Oncology, University Hospital, LMU Munich, Munich, 81377, Germany.,German Cancer Consortium (DKTK), Munich, 81377, Germany
| | - K Parodi
- Department of Medical Physics, Ludwig-Maximilians University, Garching, 85748, Germany
| | - G Baroni
- Dipartimento di Elettronica, Informazione e Bioingegneria, Politecnico di Milano, Milano, 20133, Italy.,Bioengineering Unit, Centro Nazionale di Adroterapia Oncologica, Pavia, 27100, Italy
| | - C Paganelli
- Dipartimento di Elettronica, Informazione e Bioingegneria, Politecnico di Milano, Milano, 20133, Italy
| | - M Riboldi
- Department of Medical Physics, Ludwig-Maximilians University, Garching, 85748, Germany
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24
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Ostermayr TM, Kreuzer C, Englbrecht FS, Gebhard J, Hartmann J, Huebl A, Haffa D, Hilz P, Parodi K, Wenz J, Donovan ME, Dyer G, Gaul E, Gordon J, Martinez M, Mccary E, Spinks M, Tiwari G, Hegelich BM, Schreiber J. Laser-driven x-ray and proton micro-source and application to simultaneous single-shot bi-modal radiographic imaging. Nat Commun 2020; 11:6174. [PMID: 33268784 PMCID: PMC7710721 DOI: 10.1038/s41467-020-19838-y] [Citation(s) in RCA: 3] [Impact Index Per Article: 0.8] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 01/06/2019] [Accepted: 10/29/2020] [Indexed: 11/16/2022] Open
Abstract
Radiographic imaging with x-rays and protons is an omnipresent tool in basic research and applications in industry, material science and medical diagnostics. The information contained in both modalities can often be valuable in principle, but difficult to access simultaneously. Laser-driven solid-density plasma-sources deliver both kinds of radiation, but mostly single modalities have been explored for applications. Their potential for bi-modal radiographic imaging has never been fully realized, due to problems in generating appropriate sources and separating image modalities. Here, we report on the generation of proton and x-ray micro-sources in laser-plasma interactions of the focused Texas Petawatt laser with solid-density, micrometer-sized tungsten needles. We apply them for bi-modal radiographic imaging of biological and technological objects in a single laser shot. Thereby, advantages of laser-driven sources could be enriched beyond their small footprint by embracing their additional unique properties, including the spectral bandwidth, small source size and multi-mode emission. Here the authors show a synchronized single-shot bi-modal x-ray and proton source based on laser-generated plasma. This source can be useful for radiographic and tomographic imaging.
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Affiliation(s)
- T M Ostermayr
- Ludwig-Maximilians-Universität München, Fakultät für Physik, 85748, Garching, Germany. .,Max-Planck-Institut für Quantenoptik, 85748, Garching, Germany. .,Lawrence Berkeley National Laboratory, Berkeley, CA, 94720, USA.
| | - C Kreuzer
- Ludwig-Maximilians-Universität München, Fakultät für Physik, 85748, Garching, Germany
| | - F S Englbrecht
- Ludwig-Maximilians-Universität München, Fakultät für Physik, 85748, Garching, Germany
| | - J Gebhard
- Ludwig-Maximilians-Universität München, Fakultät für Physik, 85748, Garching, Germany
| | - J Hartmann
- Ludwig-Maximilians-Universität München, Fakultät für Physik, 85748, Garching, Germany
| | - A Huebl
- Lawrence Berkeley National Laboratory, Berkeley, CA, 94720, USA
| | - D Haffa
- Ludwig-Maximilians-Universität München, Fakultät für Physik, 85748, Garching, Germany
| | - P Hilz
- Ludwig-Maximilians-Universität München, Fakultät für Physik, 85748, Garching, Germany.,Helmholtz Institute Jena, 07743, Jena, Germany
| | - K Parodi
- Ludwig-Maximilians-Universität München, Fakultät für Physik, 85748, Garching, Germany
| | - J Wenz
- Ludwig-Maximilians-Universität München, Fakultät für Physik, 85748, Garching, Germany
| | - M E Donovan
- Center for High Energy Density Science, University of Texas at Austin, Austin, TX, 78712, USA
| | - G Dyer
- Center for High Energy Density Science, University of Texas at Austin, Austin, TX, 78712, USA
| | - E Gaul
- Center for High Energy Density Science, University of Texas at Austin, Austin, TX, 78712, USA
| | - J Gordon
- Center for High Energy Density Science, University of Texas at Austin, Austin, TX, 78712, USA
| | - M Martinez
- Center for High Energy Density Science, University of Texas at Austin, Austin, TX, 78712, USA
| | - E Mccary
- Center for High Energy Density Science, University of Texas at Austin, Austin, TX, 78712, USA
| | - M Spinks
- Center for High Energy Density Science, University of Texas at Austin, Austin, TX, 78712, USA
| | - G Tiwari
- Center for High Energy Density Science, University of Texas at Austin, Austin, TX, 78712, USA
| | - B M Hegelich
- Center for High Energy Density Science, University of Texas at Austin, Austin, TX, 78712, USA
| | - J Schreiber
- Ludwig-Maximilians-Universität München, Fakultät für Physik, 85748, Garching, Germany. .,Max-Planck-Institut für Quantenoptik, 85748, Garching, Germany.
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Dickmann J, Sarosiek C, Rykalin V, Pankuch M, Rit S, Detrich N, Coutrakon G, Johnson RP, Schulte RW, Parodi K, Landry G, Dedes G. Experimental realization of dynamic fluence field optimization for proton computed tomography. ACTA ACUST UNITED AC 2020; 65:195001. [DOI: 10.1088/1361-6560/ab9f5f] [Citation(s) in RCA: 9] [Impact Index Per Article: 2.3] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 01/26/2023]
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Meijers A, Seller OC, Free J, Bondesson D, Seller Oria C, Rabe M, Parodi K, Landry G, Langendijk JA, Both S, Kurz C, Knopf AC. Assessment of range uncertainty in lung-like tissue using a porcine lung phantom and proton radiography. ACTA ACUST UNITED AC 2020; 65:155014. [DOI: 10.1088/1361-6560/ab91db] [Citation(s) in RCA: 12] [Impact Index Per Article: 3.0] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 12/25/2022]
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Pinto M, Kröniger K, Bauer J, Nilsson R, Traneus E, Parodi K. A filtering approach for PET and PG predictions in a proton treatment planning system. Phys Med Biol 2020; 65:095014. [PMID: 32191932 DOI: 10.1088/1361-6560/ab8146] [Citation(s) in RCA: 7] [Impact Index Per Article: 1.8] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/12/2022]
Abstract
Positron emission tomography (PET) and prompt gamma (PG) detection are promising proton therapy monitoring modalities. Fast calculation of the expected distributions is desirable for comparison to measurements and to develop/train algorithms for automatic treatment error detection. A filtering formalism was used for positron-emitter predictions and adapted to allow for its use for the beamline of any proton therapy centre. A novel approach based on a filtering formalism was developed for the prediction of energy-resolved PG distributions for arbitrary tissues. The method estimates PG yields and their energy spectra in the entire treatment field. Both approaches were implemented in a research version of the RayStation treatment planning system. The method was validated against PET monitoring data and Monte Carlo simulations for four patients treated with scanned proton beams. Longitudinal shifts between profiles from analytical and Monte Carlo calculations were within -1.7 and 0.9 mm, with maximum standard deviation of 0.9 mm and 1.1 mm, for positron-emitters and PG shifts, respectively. Normalized mean absolute errors were within 1.2 and 5.3%. When comparing measured and predicted PET data, the same more complex case yielded an average shift of 3 mm, while all other cases were below absolute average shifts of 1.1 mm. Normalized mean absolute errors were below 7.2% for all cases. A novel solution to predict positron-emitter and PG distributions in a treatment planning system is proposed, enabling calculation times of only a few seconds to minutes for entire patient cases, which is suitable for integration in daily clinical routine.
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Affiliation(s)
- M Pinto
- Department for Medical Physics, Ludwig-Maximilians-Universität München, Garching, Germany
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Dickmann J, Rit S, Pankuch M, Johnson RP, Schulte RW, Parodi K, Dedes G, Landry G. An optimization algorithm for dose reduction with fluence‐modulated proton CT. Med Phys 2020; 47:1895-1906. [DOI: 10.1002/mp.14084] [Citation(s) in RCA: 10] [Impact Index Per Article: 2.5] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 10/23/2019] [Revised: 01/30/2020] [Accepted: 02/05/2020] [Indexed: 01/12/2023] Open
Affiliation(s)
- J. Dickmann
- Department of Medical Physics Faculty of Physics Ludwig‐Maximilians‐Universität München Am Coulombwall 1 85748 Garching b. München Germany
| | - S. Rit
- Univ Lyon INSA‐Lyon Université Claude Bernard Lyon 1 UJM‐Saint Étienne CNRS, Inserm CREATIS UMR 5220 U1206 F‐69373 Lyon France
| | - M. Pankuch
- Northwestern Medicine Chicago Proton Center Warrenville IL 60555 USA
| | - R. P. Johnson
- Department of Physics University of California Santa Cruz Santa Cruz CA 95064 USA
| | - R. W. Schulte
- Division of Biomedical Engineering Sciences Loma Linda University Loma Linda CA 92354 USA
| | - K. Parodi
- Department of Medical Physics Faculty of Physics Ludwig‐Maximilians‐Universität München Am Coulombwall 1 85748 Garching b. München Germany
| | - G. Dedes
- Department of Medical Physics Faculty of Physics Ludwig‐Maximilians‐Universität München Am Coulombwall 1 85748 Garching b. München Germany
| | - G. Landry
- Department of Medical Physics Faculty of Physics Ludwig‐Maximilians‐Universität München Am Coulombwall 1 85748 Garching b. München Germany
- Department of Radiation Oncology University Hospital, LMU Munich 81377 Munich Germany
- German Cancer Consortium (DKTK) 81377 Munich Germany
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Magallanes L, Meyer S, Gianoli C, Kopp B, Voss B, Jakel O, Brons S, Gordon J, Parodi K. Upgrading an Integrating Carbon-Ion Transmission Imaging System With Active Scanning Beam Delivery Toward Low Dose Ion Imaging. IEEE Trans Radiat Plasma Med Sci 2020. [DOI: 10.1109/trpms.2019.2948584] [Citation(s) in RCA: 6] [Impact Index Per Article: 1.5] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/10/2022]
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Parodi K. SP-069: Latest developments in range estimation and range verification. Radiother Oncol 2019. [DOI: 10.1016/s0167-8140(20)30589-2] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/17/2022]
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31
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Bauer J, Tessonnier T, Debus J, Parodi K. Offline imaging of positron emitters induced by therapeutic helium, carbon and oxygen ion beams with a full-ring PET/CT scanner: experiments in reference targets. Phys Med Biol 2019; 64:225016. [PMID: 31561234 DOI: 10.1088/1361-6560/ab48b4] [Citation(s) in RCA: 4] [Impact Index Per Article: 0.8] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/12/2022]
Abstract
In vivo verification of light ion therapy based on positron-emission tomography (PET) imaging of irradiation induced patient activation relies on activity predictions from Monte-Carlo (MC) or analytical computational engines for comparison to the measurements. In order to achieve the necessary accuracy, experimental data are indispensable for the validation of the calculation models. For this we irradiated thick reference targets with mono-energetic helium, carbon and oxygen ion beams and measured the resulting material activation offline with a commercial full-ring PET/CT scanner located nearby the treatment room. Acquired PET data were analysed over time to separate the activity contribution of different radionuclides. Determined production yields were compared to published findings obtained from in-beam activation measurements with a limited-angle double-head PET camera. In addition, we investigated the time-dependence of the measured radionuclide-specific contributions and of the distal activity range, as well as the lateral spread of the activity signal as a function of beam penetration depth. We present radionuclide-specific depth-resolved activity distributions and production yields for the radionuclides [Formula: see text], [Formula: see text] and [Formula: see text], dominating irradiation-induced patient activation. We observe systematically lower production yields with a ratio between the dual-head and our full-ring PET measurements of, on average, 1.7 and 1.3 for the oxygen and carbon beam irradiations, and 1.7 (2.1) for the high (low) energy helium beam irradiations. Findings on the temporal development of the activity range confirm the expectation, with the oxygen beam induced signal being the most sensitive scenario. The experimental data reported in this work, acquired with a state-of-the-art full ring PET scanner, provide a comprehensive and consistent basis for the benchmarking of PET signal calculation engines. In particular, they can support a fine-tuning of the underlying physics models used by the respective implementation and therefore improve the accuracy of PET-based therapy verifications at current and future treatment facilities.
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Affiliation(s)
- J Bauer
- Heidelberg Ion-Beam Therapy Center (HIT), Department of Radiation Oncology, University Hospital, Heidelberg, Germany. National Centre for Radiation Research in Oncology (NCRO), Heidelberg Institute for Radiation Oncology (HIRO), Heidelberg, Germany
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Kroll C, Dietrich O, Bortfeldt J, Paganelli C, Baroni G, Kamp F, Neppl S, Belka C, Parodi K, Opel M, Riboldi M. Improving the modelling of susceptibility-induced spatial distortions in MRI-guided extra-cranial radiotherapy. ACTA ACUST UNITED AC 2019; 64:205006. [DOI: 10.1088/1361-6560/ab447c] [Citation(s) in RCA: 3] [Impact Index Per Article: 0.6] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/11/2022]
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33
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Dickmann J, Wesp P, Rädler M, Rit S, Pankuch M, Johnson RP, Bashkirov V, Schulte RW, Parodi K, Landry G, Dedes G. Prediction of image noise contributions in proton computed tomography and comparison to measurements. ACTA ACUST UNITED AC 2019; 64:145016. [DOI: 10.1088/1361-6560/ab2474] [Citation(s) in RCA: 19] [Impact Index Per Article: 3.8] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/11/2022]
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Hofmann T, Fochi A, Parodi K, Pinto M. Prediction of positron emitter distributions for range monitoring in carbon ion therapy: an analytical approach. Phys Med Biol 2019; 64:105022. [PMID: 30970340 DOI: 10.1088/1361-6560/ab17f9] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.2] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 10/27/2022]
Abstract
Range verification is one of the most relevant tasks in ion beam therapy. In the case of carbon ion therapy, positron emission tomography (PET) is the most widely used method for this purpose, which images the [Formula: see text]-activation following nuclear interactions of the ions with the tissue nuclei. Since the positron emitter activity profile is not directly proportional to the dose distribution, until today only its comparison to a prediction of the PET profile allows for treatment verification. Usually, this prediction is obtained from time-consuming Monte Carlo simulations of high computational effort, which impacts the clinical workflow. To solve this issue in proton therapy, a convolution approach was suggested to predict positron emitter activity profiles from depth dose distributions analytically. In this work, we introduce an approach to predict positron emitter distributions from depth dose profiles in carbon ion therapy. While the distal fall-off position of the positron emitter profile is predicted from a convolution approach similar to the one suggested for protons, additional analytical functions are introduced to describe the characteristics of the positron emitter distribution in tissue. The feasibility of this approach is demonstrated with monoenergetic depth dose profiles and spread out Bragg peaks in homogeneous and heterogeneous phantoms. In all cases, the positron emitter profile is predicted with high precision and the distal fall-off position is reproduced with millimeter accuracy.
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Affiliation(s)
- T Hofmann
- Department for Medical Physics, Ludwig-Maximilians-Universität München, Am Coulombwall 1, 85748 Garching b. München, Germany
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Landry G, Hansen D, Kamp F, Li M, Hoyle B, Weller J, Parodi K, Belka C, Kurz C. OC-0085 Correcting CBCT images for dose calculation using a U-shaped deep convolutional neural network. Radiother Oncol 2019. [DOI: 10.1016/s0167-8140(19)30505-5] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/15/2022]
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Martins J, Saxena R, Neppl S, Alhazmi A, Reiner M, Belka C, Parodi K. PO-0906 Perturbation techniques for optimizing IAEA phase spaces for different medical linacs. Radiother Oncol 2019. [DOI: 10.1016/s0167-8140(19)31326-x] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/24/2022]
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Kurz C, Maspero M, Savenije M, Landry G, Kamp F, Li M, Parodi K, Belka C, Van den Berg C. OC-0513 Cone-beam CT intensity correction using a generative adversarial network and unpaired training. Radiother Oncol 2019. [DOI: 10.1016/s0167-8140(19)30933-8] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/17/2022]
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Freislederer P, Von Münchow A, Kamp F, Heinz C, Gerum S, Roeder F, Corradini S, Floca R, Alber M, Söhn M, Reiner M, Belka C, Parodi K. OC-0525 4D Monte Carlo dose calculations on different CT image sets for SBRT using patient breathing data. Radiother Oncol 2019. [DOI: 10.1016/s0167-8140(19)30945-4] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 10/26/2022]
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39
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Hofmaier J, Dedes G, Carlson D, Parodi K, Belka C, Kamp F. OC-0569 A framework for variance-based sensitivity analysis of uncertainties in proton therapy. Radiother Oncol 2019. [DOI: 10.1016/s0167-8140(19)30989-2] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 10/26/2022]
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Hofmann T, Pinto M, Mohammadi A, Nitta M, Nishikido F, Iwao Y, Tashima H, Yoshida E, Chacon A, Safavi-Naeini M, Rosenfeld A, Yamaya T, Parodi K. Dose reconstruction from PET images in carbon ion therapy: a deconvolution approach. ACTA ACUST UNITED AC 2019; 64:025011. [DOI: 10.1088/1361-6560/aaf676] [Citation(s) in RCA: 16] [Impact Index Per Article: 3.2] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 12/30/2022]
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41
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Augusto RS, Mohammadi A, Tashima H, Yoshida E, Yamaya T, Ferrari A, Parodi K. Experimental validation of the FLUKA Monte Carlo code for dose and [Formula: see text]-emitter predictions of radioactive ion beams. Phys Med Biol 2018; 63:215014. [PMID: 30252649 DOI: 10.1088/1361-6560/aae431] [Citation(s) in RCA: 6] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/11/2022]
Abstract
In the context of hadrontherapy, whilst ions are capable of effectively destroying radio resistant, deep seated tumors, their treatment localization must be well assessed to ensure the sparing of surrounding healthy tissue and treatment effectiveness. Thus, range verification techniques, such as online positron-emission-tomography (PET) imaging, hold great potential in clinical practice, providing information on the in vivo beam range and consequent tumor targeting. Furthermore, [Formula: see text] emitting radioactive ions can be an asset in online PET imaging, depending on their half-life, compared to their stable counterparts. It is expected that using these radioactive ions the signal obtained by a PET apparatus during beam delivery will be greatly increased, and exhibit a better correlation to the Bragg Peak. To this end, FLUKA Monte Carlo particle transport and interaction code was used to evaluate, in terms of annihilation events at rest and dose, the figure of merit in using [Formula: see text] emitter, radioactive ion beams (RI [Formula: see text]). For this purpose, the simulation results were compared with experimental data obtained with an openPET prototype in various online PET acquisitions at the Heavy Ion Medical Accelerator in Chiba (HIMAC), in collaboration with colleagues from the National Institute of Radiological Sciences' (NIRS) Imaging Physics Team. The dosimetry performance evaluation with FLUKA benefits from its recent developments in fragmentation production models. The present work estimated that irradiations with RI [Formula: see text], produced via projectile fragmentation and their signal acquisition with state-of-the-art PET scanner, lead to nearly a factor of two more accurate definition of the signals' peak position. In addition to its more advantageous distribution shape, it was observed at least an order magnitude higher signal acquired from 11C and 15O irradiations, with respect to their stable counterparts.
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Affiliation(s)
- R S Augusto
- European Organization for Nuclear Research, Geneva, Switzerland. Ludwig-Maximilians-Universität München, Munich, Germany
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42
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Augusto RS, Bauer J, Bouhali O, Cuccagna C, Gianoli C, Kozłowska WS, Ortega PG, Tessonnier T, Toufique Y, Vlachoudis V, Parodi K, Ferrari A. An overview of recent developments in FLUKA PET tools. Phys Med 2018; 54:189-199. [PMID: 30017561 DOI: 10.1016/j.ejmp.2018.06.636] [Citation(s) in RCA: 13] [Impact Index Per Article: 2.2] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Journal Information] [Submit a Manuscript] [Subscribe] [Scholar Register] [Received: 02/02/2018] [Revised: 04/25/2018] [Accepted: 06/22/2018] [Indexed: 12/19/2022] Open
Abstract
The new developments of the FLUKA Positron-Emission-Tomography (PET) tools are detailed. FLUKA is a fully integrated Monte Carlo (MC) particle transport code, used for an extended range of applications, including Medical Physics. Recently, it provided the medical community with dedicated simulation tools for clinical applications, including the PET simulation package. PET is a well-established imaging technique in nuclear medicine, and a promising method for clinical in vivo treatment verification in hadrontherapy. The application of clinically established PET scanners to new irradiation environments such as hadrontherapy requires further experimental and theoretical research to which MC simulations could be applied. The FLUKA PET tools, besides featuring PET scanner models in its library, allow the configuration of new PET prototypes via the FLUKA Graphical User Interface (GUI) Flair. Both the beam time structure and scan time can be specified by the user, reproducing PET acquisitions in time, in a particle therapy scenario. Furthermore, different scoring routines allow the analysis of single and coincident events, and identification of parent isotopes generating annihilation events. Two reconstruction codes are currently supported: the Filtered Back-Projection (FBP) and Maximum-Likelihood Expectation Maximization (MLEM), the latter embedded in the tools. Compatibility with other reconstruction frameworks is also possible. The FLUKA PET tools package has been successfully tested for different detectors and scenarios, including conventional functional PET applications and in beam PET, either using radioactive sources, or simulating hadron beam irradiations. The results obtained so far confirm the FLUKA PET tools suitability to perform PET simulations in R&D environment.
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Affiliation(s)
- R S Augusto
- CERN - European Organization for Nuclear Research, CH-1211 Genève 23, Switzerland; Ludwig-Maximilians-Universität München, Am Coulombwall 1, 85748 Garching, Germany.
| | - J Bauer
- UniversitätsKlinikum Heidelberg, Heidelberger Ionenstrahl-Therapiezentrum HIT, Germany
| | - O Bouhali
- Texas A&M University at Qatar, 23874 Doha, Qatar
| | - C Cuccagna
- CERN - European Organization for Nuclear Research, CH-1211 Genève 23, Switzerland; TERA Foundation, Via Puccini 11, 28100 Novara, Italy; Université de Genève, 30 quai Ernest-Ansermet, CH-1211 Genève, Switzerland
| | - C Gianoli
- Ludwig-Maximilians-Universität München, Am Coulombwall 1, 85748 Garching, Germany
| | - W S Kozłowska
- CERN - European Organization for Nuclear Research, CH-1211 Genève 23, Switzerland; Medizinische Universität Wien, Spitalgasse 23, 1090 Vienna, Austria
| | - P G Ortega
- Grupo de Física Nuclear, Universidad de Salamanca, E-37008 Salamanca, Spain
| | - T Tessonnier
- Centre François Baclesse, 3 Avenue du Général Harris, 14000 Caen, France
| | - Y Toufique
- Texas A&M University at Qatar, 23874 Doha, Qatar; Institut Superieur des Sciences de la Santé de Settat, Morocco
| | - V Vlachoudis
- CERN - European Organization for Nuclear Research, CH-1211 Genève 23, Switzerland
| | - K Parodi
- Ludwig-Maximilians-Universität München, Am Coulombwall 1, 85748 Garching, Germany
| | - A Ferrari
- CERN - European Organization for Nuclear Research, CH-1211 Genève 23, Switzerland
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Niepel K, Kurz C, Kamp F, Hansen D, Rit S, Neppl S, Hofmaier J, Bondesson D, Thieke C, Dinkel J, Belka C, Parodi K, Landry G. PO-0940: Porcine-lung-phantom based evaluation of proton dose calculations on 4DCBCT. Radiother Oncol 2018. [DOI: 10.1016/s0167-8140(18)31250-7] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 12/01/2022]
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44
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Lindner FH, Bin JH, Englbrecht F, Haffa D, Bolton PR, Gao Y, Hartmann J, Hilz P, Kreuzer C, Ostermayr TM, Rösch TF, Speicher M, Parodi K, Thirolf PG, Schreiber J. A novel approach to electron data background treatment in an online wide-angle spectrometer for laser-accelerated ion and electron bunches. Rev Sci Instrum 2018; 89:013301. [PMID: 29390656 DOI: 10.1063/1.5001990] [Citation(s) in RCA: 3] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/07/2023]
Abstract
Laser-based ion acceleration is driven by electrical fields emerging when target electrons absorb laser energy and consecutively leave the target material. A direct correlation between these electrons and the accelerated ions is thus to be expected and predicted by theoretical models. We report on a modified wide-angle spectrometer, allowing the simultaneous characterization of angularly resolved energy distributions of both ions and electrons. Equipped with online pixel detectors, the RadEye1 detectors, the investigation of this correlation gets attainable on a single shot basis. In addition to first insights, we present a novel approach for reliably extracting the primary electron energy distribution from the interfering secondary radiation background. This proves vitally important for quantitative extraction of average electron energies (temperatures) and emitted total charge.
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Affiliation(s)
- F H Lindner
- Lehrstuhl für Experimentalphysik - Medizinische Physik, Fakultät für Physik, Ludwig-Maximilians-Universität München, Am Coulombwall 1, 85748 Garching bei München, Germany
| | - J H Bin
- Lehrstuhl für Experimentalphysik - Medizinische Physik, Fakultät für Physik, Ludwig-Maximilians-Universität München, Am Coulombwall 1, 85748 Garching bei München, Germany
| | - F Englbrecht
- Lehrstuhl für Experimentalphysik - Medizinische Physik, Fakultät für Physik, Ludwig-Maximilians-Universität München, Am Coulombwall 1, 85748 Garching bei München, Germany
| | - D Haffa
- Lehrstuhl für Experimentalphysik - Medizinische Physik, Fakultät für Physik, Ludwig-Maximilians-Universität München, Am Coulombwall 1, 85748 Garching bei München, Germany
| | - P R Bolton
- Lehrstuhl für Experimentalphysik - Medizinische Physik, Fakultät für Physik, Ludwig-Maximilians-Universität München, Am Coulombwall 1, 85748 Garching bei München, Germany
| | - Y Gao
- Lehrstuhl für Experimentalphysik - Medizinische Physik, Fakultät für Physik, Ludwig-Maximilians-Universität München, Am Coulombwall 1, 85748 Garching bei München, Germany
| | - J Hartmann
- Lehrstuhl für Experimentalphysik - Medizinische Physik, Fakultät für Physik, Ludwig-Maximilians-Universität München, Am Coulombwall 1, 85748 Garching bei München, Germany
| | - P Hilz
- Lehrstuhl für Experimentalphysik - Medizinische Physik, Fakultät für Physik, Ludwig-Maximilians-Universität München, Am Coulombwall 1, 85748 Garching bei München, Germany
| | - C Kreuzer
- Lehrstuhl für Experimentalphysik - Medizinische Physik, Fakultät für Physik, Ludwig-Maximilians-Universität München, Am Coulombwall 1, 85748 Garching bei München, Germany
| | - T M Ostermayr
- Lehrstuhl für Experimentalphysik - Medizinische Physik, Fakultät für Physik, Ludwig-Maximilians-Universität München, Am Coulombwall 1, 85748 Garching bei München, Germany
| | - T F Rösch
- Lehrstuhl für Experimentalphysik - Medizinische Physik, Fakultät für Physik, Ludwig-Maximilians-Universität München, Am Coulombwall 1, 85748 Garching bei München, Germany
| | - M Speicher
- Lehrstuhl für Experimentalphysik - Medizinische Physik, Fakultät für Physik, Ludwig-Maximilians-Universität München, Am Coulombwall 1, 85748 Garching bei München, Germany
| | - K Parodi
- Lehrstuhl für Experimentalphysik - Medizinische Physik, Fakultät für Physik, Ludwig-Maximilians-Universität München, Am Coulombwall 1, 85748 Garching bei München, Germany
| | - P G Thirolf
- Lehrstuhl für Experimentalphysik - Medizinische Physik, Fakultät für Physik, Ludwig-Maximilians-Universität München, Am Coulombwall 1, 85748 Garching bei München, Germany
| | - J Schreiber
- Lehrstuhl für Experimentalphysik - Medizinische Physik, Fakultät für Physik, Ludwig-Maximilians-Universität München, Am Coulombwall 1, 85748 Garching bei München, Germany
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Aldawood S, Thirolf P, Miani A, Böhmer M, Dedes G, Gernhäuser R, Lang C, Liprandi S, Maier L, Marinšek T, Mayerhofer M, Schaart D, Lozano IV, Parodi K. Development of a Compton camera for prompt-gamma medical imaging. Radiat Phys Chem Oxf Engl 1993 2017. [DOI: 10.1016/j.radphyschem.2017.01.024] [Citation(s) in RCA: 35] [Impact Index Per Article: 5.0] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/25/2022]
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46
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Tessonnier T, Mairani A, Brons S, Sala P, Cerutti F, Ferrari A, Haberer T, Debus J, Parodi K. Helium ions at the heidelberg ion beam therapy center: comparisons between FLUKA Monte Carlo code predictions and dosimetric measurements. ACTA ACUST UNITED AC 2017; 62:6784-6803. [DOI: 10.1088/1361-6560/aa7b12] [Citation(s) in RCA: 21] [Impact Index Per Article: 3.0] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 12/27/2022]
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47
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Tessonnier T, Böhlen TT, Ceruti F, Ferrari A, Sala P, Brons S, Haberer T, Debus J, Parodi K, Mairani A. Dosimetric verification in water of a Monte Carlo treatment planning tool for proton, helium, carbon and oxygen ion beams at the Heidelberg Ion Beam Therapy Center. ACTA ACUST UNITED AC 2017. [DOI: 10.1088/1361-6560/aa7be4] [Citation(s) in RCA: 32] [Impact Index Per Article: 4.6] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 12/15/2022]
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48
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Dedes G, De Angelis L, Rit S, Hansen D, Belka C, Bashkirov V, Johnson RP, Coutrakon G, Schubert KE, Schulte RW, Parodi K, Landry G. Application of fluence field modulation to proton computed tomography for proton therapy imaging. ACTA ACUST UNITED AC 2017; 62:6026-6043. [DOI: 10.1088/1361-6560/aa7734] [Citation(s) in RCA: 18] [Impact Index Per Article: 2.6] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/12/2022]
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49
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Mairani A, Magro G, Tessonnier T, Böhlen TT, Molinelli S, Ferrari A, Parodi K, Debus J, Haberer T. Optimizing the modified microdosimetric kinetic model input parameters for proton and4He ion beam therapy application. Phys Med Biol 2017; 62:N244-N256. [DOI: 10.1088/1361-6560/aa6be9] [Citation(s) in RCA: 20] [Impact Index Per Article: 2.9] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/12/2022]
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50
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Parodi K. SP-0106: Reducing range uncertainties: new approaches for stopping power determination and in-vivo range verification. Radiother Oncol 2017. [DOI: 10.1016/s0167-8140(17)30550-9] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 10/19/2022]
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