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Jia SB, Shamsabadi R. Secondary cancer risk assessments following the proton therapy of lung cancer as the functions of field characteristics and patient age. Int J Radiat Biol 2024; 100:183-189. [PMID: 37747407 DOI: 10.1080/09553002.2023.2263546] [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: 05/08/2023] [Accepted: 09/19/2023] [Indexed: 09/26/2023]
Abstract
INTRODUCTION Radiation-induced secondary cancers relevant to proton therapy are still a main concern among cancer survivors. This study aims to determine the effects of age at exposure and treatment field size on radiation-induced secondary tumors following the proton therapy of lung cancer within out of field organs through the Monte Carlo (MC) simulation approach. MATERIAL AND METHODS A full MC model of ICRP-110 male phantom was simulated to calculate the absorbed dose corresponding to secondary radiations within distant organs from the tumor volume. Then, the risks of secondary malignancies were estimated by employing the recommended risk model by the Committee of Biological Effects of Ionizing Radiation (BEIR) for different treatment field sizes and various patient ages at exposure. RESULTS The results revealed that by increasing the patient age from 25 to 45 years, lifetime attributable risk (LAR) values were decreased. Maximum and minimum mortality rates were obtained for the liver and thyroid at the fixed age of 25 years, respectively. Calculated risk values for most near organs to the tumor were higher than those for distant organs. Changing the aperture size from 5 × 5 cm2 to 8 × 10 cm2 resulted in LAR increments with maximum variations of 12.5% for the stomach and a rough variation of 1.12 times in LAR for all exposure ages. CONCLUSION Our work on whole-body phantom addresses the impact of age at exposure and aperture size on LAR during the proton therapy of lung cancer. To minimize secondary cancer risks relevant to proton therapy of lung cancer, extra attention should be considered.
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Affiliation(s)
| | - Reza Shamsabadi
- Physics Department, Hakim Sabzevari University, Sabzevar, Iran
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2
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Hérault J, Gérard A, Carnicer A, Aloi D, Peyrichon ML, Barnel C, Vidal M, Angellier G, Fayaud D, Grini JC, Giusto A, Armando C, Donadey G, Cabannes M, Dumas S, Payan Y, Di Carlo JF, Salicis C, Bergerot JM, Rolion M, Trimaud R, Hofverberg P, Mandrillon P, Sauerwein W, Thariat J. 30 years of ocular proton therapy, the Nice view. Cancer Radiother 2022; 26:1016-1026. [PMID: 35803860 DOI: 10.1016/j.canrad.2022.03.004] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 11/29/2021] [Accepted: 03/15/2022] [Indexed: 11/08/2022]
Abstract
PURPOSE Radiotherapy with protons (PT) is a standard treatment of ocular tumors. It achieves excellent tumor control, limited toxicities, and the preservation of important functional outcomes, such as vision. Although PT may appear as one homogenous technique, it can be performed using dedicated ocular passive scattering PT or, increasingly, Pencil Beam Scanning (PBS), both with various degrees of patient-oriented customization. MATERAIAL AND METHODS MEDICYC PT facility of Nice are detailed with respect to their technical, dosimetric, microdosimetric and radiobiological, patient and tumor-customization process of PT planning and delivery that are key. 6684 patients have been treated for ocular tumors (1991-2020). Machine characteristics (accelerator, beam line, beam monitoring) allow efficient proton extraction, high dose rate, sharp lateral and distal penumbrae, and limited stray radiation in comparison to beam energy reduction and subsequent straggling with high-energy PBS PT. Patient preparation before PT includes customized setup and image-guidance, CT-based planning, and ocular PT software modelling of the patient eye with integration of beam modifiers. Clinical reports have shown excellent tumor control rates (∼95%), vision preservation and limited toxicity rates (papillopathy, retinopathy, neovascular glaucoma, dry eye, madarosis, cataract). RESULTS Although demanding, dedicated ocular PT has proven its efficiency in achieving excellent tumor control, OAR sparing and patient radioprotection. It is therefore worth adaptations of the equipments and practice. CONCLUSIONS Some of these adaptations can be transferred to other PT centers and should be acknowledeged when using non-PT options.
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Affiliation(s)
- J Hérault
- Institut Méditerranéen de ProtonThérapie, Centre Antoine Lacassagne, 227, avenue de la Lanterne, 06200 Nice, France.
| | - A Gérard
- Institut Méditerranéen de ProtonThérapie, Centre Antoine Lacassagne, 227, avenue de la Lanterne, 06200 Nice, France
| | - A Carnicer
- IDOM Consulting, Engineering, Architecture, Avinguda de la Fama, 11-15, Arboretum Business Park, Arce Building, 08940 Cornellà de Llobregat, Barcelona, Spain
| | - D Aloi
- Institut Méditerranéen de ProtonThérapie, Centre Antoine Lacassagne, 227, avenue de la Lanterne, 06200 Nice, France
| | - M-L Peyrichon
- Institut Méditerranéen de ProtonThérapie, Centre Antoine Lacassagne, 227, avenue de la Lanterne, 06200 Nice, France
| | - C Barnel
- Institut Méditerranéen de ProtonThérapie, Centre Antoine Lacassagne, 227, avenue de la Lanterne, 06200 Nice, France
| | - M Vidal
- Institut Méditerranéen de ProtonThérapie, Centre Antoine Lacassagne, 227, avenue de la Lanterne, 06200 Nice, France
| | - G Angellier
- Institut Méditerranéen de ProtonThérapie, Centre Antoine Lacassagne, 227, avenue de la Lanterne, 06200 Nice, France
| | - D Fayaud
- Institut Méditerranéen de ProtonThérapie, Centre Antoine Lacassagne, 227, avenue de la Lanterne, 06200 Nice, France
| | - J-C Grini
- Institut Méditerranéen de ProtonThérapie, Centre Antoine Lacassagne, 227, avenue de la Lanterne, 06200 Nice, France
| | - A Giusto
- Institut Méditerranéen de ProtonThérapie, Centre Antoine Lacassagne, 227, avenue de la Lanterne, 06200 Nice, France
| | - C Armando
- Institut Méditerranéen de ProtonThérapie, Centre Antoine Lacassagne, 227, avenue de la Lanterne, 06200 Nice, France
| | - G Donadey
- Institut Méditerranéen de ProtonThérapie, Centre Antoine Lacassagne, 227, avenue de la Lanterne, 06200 Nice, France
| | - M Cabannes
- Institut Méditerranéen de ProtonThérapie, Centre Antoine Lacassagne, 227, avenue de la Lanterne, 06200 Nice, France
| | - S Dumas
- Institut Méditerranéen de ProtonThérapie, Centre Antoine Lacassagne, 227, avenue de la Lanterne, 06200 Nice, France
| | - Y Payan
- Institut Méditerranéen de ProtonThérapie, Centre Antoine Lacassagne, 227, avenue de la Lanterne, 06200 Nice, France
| | - J-F Di Carlo
- Institut Méditerranéen de ProtonThérapie, Centre Antoine Lacassagne, 227, avenue de la Lanterne, 06200 Nice, France
| | - C Salicis
- Institut Méditerranéen de ProtonThérapie, Centre Antoine Lacassagne, 227, avenue de la Lanterne, 06200 Nice, France
| | - J-M Bergerot
- Institut Méditerranéen de ProtonThérapie, Centre Antoine Lacassagne, 227, avenue de la Lanterne, 06200 Nice, France
| | - M Rolion
- Institut Méditerranéen de ProtonThérapie, Centre Antoine Lacassagne, 227, avenue de la Lanterne, 06200 Nice, France
| | - R Trimaud
- Institut Méditerranéen de ProtonThérapie, Centre Antoine Lacassagne, 227, avenue de la Lanterne, 06200 Nice, France
| | - P Hofverberg
- Institut Méditerranéen de ProtonThérapie, Centre Antoine Lacassagne, 227, avenue de la Lanterne, 06200 Nice, France
| | - P Mandrillon
- AIMA Development, 227, avenue de la Lanterne, 06200 Nice, France
| | - W Sauerwein
- NCTeam, Strahlenklinik, Universitätsklinikum Essen, Hufelandstraße 55, 45122 Essen, Germany
| | - J Thariat
- Department of Radiation Oncology, Centre François Baclesse, 14000 Caen, France; Laboratoire de Physique Corpusculaire IN2P3/ENSICAEN-UMR6534-Unicaen-Normandie Université, 14000 Caen, France
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3
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Romero-Expósito M, Toma-Dasu I, Dasu A. Determining Out-of-Field Doses and Second Cancer Risk From Proton Therapy in Young Patients—An Overview. Front Oncol 2022; 12:892078. [PMID: 35712488 PMCID: PMC9197425 DOI: 10.3389/fonc.2022.892078] [Citation(s) in RCA: 4] [Impact Index Per Article: 2.0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 03/08/2022] [Accepted: 05/02/2022] [Indexed: 11/13/2022] Open
Abstract
Proton therapy has the potential to provide survival and tumor control outcomes comparable and frequently superior to photon therapy. This has led to a significant concern in the medical physics community on the risk for the induction of second cancers in all patients and especially in younger patients, as they are considered more radiosensitive than adults and have an even longer expected lifetime after treatment. Thus, our purpose is to present an overview of the research carried out on the evaluation of out-of-field doses linked to second cancer induction and the prediction of this risk. Most investigations consisted of Monte Carlo simulations in passive beam facilities for clinical scenarios. These works established that equivalent doses in organs could be up to 200 mSv or 900 mSv for a brain or a craniospinal treatment, respectively. The major contribution to this dose comes from the secondary neutrons produced in the beam line elements. Few works focused on scanned-beam facilities, but available data show that, for these facilities, equivalent doses could be between 2 and 50 times lower. Patient age is a relevant factor in the dose level, especially for younger patients (by means of the size of the body) and, in addition, in the predicted risk by models (due to the age dependence of the radiosensitivity). For risks, the sex of the patient also plays an important role, as female patients show higher sensitivity to radiation. Thus, predicted risks of craniospinal irradiation can range from 8% for a 15-year-old male patient to 58% for a 2-year-old female patient, using a risk model from a radiological protection field. These values must be taken with caution due to uncertainties in risk models, and then dosimetric evaluation of stray radiation becomes mandatory in order to complement epidemiological studies and be able to model appropriate dose–response functions for this dose range. In this sense, analytical models represent a useful tool and some models have been implemented to be used for young patients. Research carried out so far confirmed that proton beam therapy reduces the out-of-field doses and second cancer risk. However, further investigations may be required in scanned-beam delivery systems.
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Affiliation(s)
- Maite Romero-Expósito
- The Skandion Clinic, Uppsala, Sweden
- Oncology Pathology Department, Karolinska Institutet, Stockholm, Sweden
- *Correspondence: Maite Romero-Expósito,
| | - Iuliana Toma-Dasu
- Oncology Pathology Department, Karolinska Institutet, Stockholm, Sweden
- Medical Radiation Physics, Stockholm University, Stockholm, Sweden
| | - Alexandru Dasu
- The Skandion Clinic, Uppsala, Sweden
- Medical Radiation Sciences, Department of Immunology, Genetics and Pathology, Uppsala University, Uppsala, Sweden
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4
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Leite AMM, Ronga MG, Giorgi M, Ristic Y, Perrot Y, Trompier F, Prezado Y, Créhange G, De Marzi L. Secondary neutron dose contribution from pencil beam scanning, scattered and spatially fractionated proton therapy. Phys Med Biol 2021; 66. [PMID: 34673555 DOI: 10.1088/1361-6560/ac3209] [Citation(s) in RCA: 3] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 07/22/2021] [Accepted: 10/21/2021] [Indexed: 11/11/2022]
Abstract
The Orsay Proton therapy Center (ICPO) has a long history of intracranial radiotherapy using both double scattering (DS) and pencil beam scanning (PBS) techniques, and is actively investigating a promising modality of spatially fractionated radiotherapy using proton minibeams (pMBRT). This work provides a comprehensive comparison of the organ-specific secondary neutron dose due to each of these treatment modalities, assessed using Monte Carlo (MC) algorithms and measurements. A MC model of a universal nozzle was benchmarked by comparing the neutron ambient dose equivalent,H*(10), in the gantry room with measurements obtained using a WENDI-II counter. The secondary neutron dose was evaluated for clinically relevant intracranial treatments of patients of different ages, in which secondary neutron doses were scored in anthropomorphic phantoms merged with the patients' images. The MC calculatedH*(10) values showed a reasonable agreement with the measurements and followed the expected tendency, in which PBS yields the lowest dose, followed by pMBRT and DS. Our results for intracranial treatments show that pMBRT yielded a higher secondary neutron dose for organs closer to the target volume, while organs situated furthest from the target volume received a greater quantity of neutrons from the passive scattering beam line. To the best of our knowledge, this is the first study to compare MC secondary neutron dose estimates in clinical treatments between these various proton therapy modalities and to realistically quantify the secondary neutron dose contribution of clinical pMBRT treatments. The method established in this study will enable epidemiological studies of the long-term effects of intracranial treatments at ICPO, notably radiation-induced second malignancies.
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Affiliation(s)
- A M M Leite
- Institut Curie, PSL Research University, Radiation Oncology Department, Proton Therapy Centre, Centre Universitaire, F-91898 Orsay, France.,Institut Curie, PSL Research University, University Paris Saclay, Inserm U 1021- CNRS UMR 3347, F-91898 Orsay, France
| | - M G Ronga
- Institut Curie, PSL Research University, Radiation Oncology Department, Proton Therapy Centre, Centre Universitaire, F-91898 Orsay, France
| | - M Giorgi
- Institut Curie, PSL Research University, Radiation Oncology Department, Proton Therapy Centre, Centre Universitaire, F-91898 Orsay, France
| | - Y Ristic
- Institut de Radioprotection et de Sûreté Nucléaire, Service de Dosimétrie, Laboratoire de Dosimétrie des Rayonnements Ionisants, F-92262 Fontenay-aux-Roses Cedex, France
| | - Y Perrot
- Institut de Radioprotection et de Sûreté Nucléaire, Service de Dosimétrie, Laboratoire de Dosimétrie des Rayonnements Ionisants, F-92262 Fontenay-aux-Roses Cedex, France
| | - F Trompier
- Institut de Radioprotection et de Sûreté Nucléaire, Service de Dosimétrie, Laboratoire de Dosimétrie des Rayonnements Ionisants, F-92262 Fontenay-aux-Roses Cedex, France
| | - Y Prezado
- Institut Curie, PSL Research University, University Paris Saclay, Inserm U 1021- CNRS UMR 3347, F-91898 Orsay, France
| | - G Créhange
- Institut Curie, PSL Research University, Radiation Oncology Department, Proton Therapy Centre, Centre Universitaire, F-91898 Orsay, France
| | - L De Marzi
- Institut Curie, PSL Research University, Radiation Oncology Department, Proton Therapy Centre, Centre Universitaire, F-91898 Orsay, France.,Institut Curie, PSL Research University, University Paris Saclay, Inserm LITO, F-91898 Orsay, France
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5
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Bentley-Ford MR, Engle SE, Clearman KR, Haycraft CJ, Andersen RS, Croyle MJ, Rains AB, Berbari NF, Yoder BK. A mouse model of BBS identifies developmental and homeostatic effects of BBS5 mutation and identifies novel pituitary abnormalities. Hum Mol Genet 2021; 30:234-246. [PMID: 33560420 DOI: 10.1093/hmg/ddab039] [Citation(s) in RCA: 6] [Impact Index Per Article: 2.0] [Reference Citation Analysis] [Abstract] [Journal Information] [Subscribe] [Scholar Register] [Received: 08/13/2020] [Revised: 01/04/2021] [Accepted: 01/29/2021] [Indexed: 12/22/2022] Open
Abstract
Primary cilia are critical sensory and signaling compartments present on most mammalian cell types. These specialized structures require a unique signaling protein composition relative to the rest of the cell to carry out their functions. Defects in ciliary structure and signaling result in a broad group of disorders collectively known as ciliopathies. One ciliopathy, Bardet-Biedl syndrome (BBS; OMIM 209900), presents with diverse clinical features, many of which are attributed to defects in ciliary signaling during both embryonic development and postnatal life. For example, patients exhibit obesity, polydactyly, hypogonadism, developmental delay and skeletal abnormalities along with sensory and cognitive deficits, but for many of these phenotypes it is uncertain, which are developmental in origin. A subset of BBS proteins assembles into the core BBSome complex, which is responsible for mediating transport of membrane proteins into and out of the cilium, establishing it as a sensory and signaling hub. Here, we describe two new mouse models for BBS resulting from a targeted LacZ gene trap allele (Bbs5-/-) that is a predicted congenital null mutation and conditional (Bbs5flox/flox) allele of Bbs5. Bbs5-/- mice develop a complex phenotype consisting of increased pre-weaning lethality craniofacial and skeletal defects, ventriculomegaly, infertility and pituitary anomalies. Utilizing the conditional allele, we show that the male fertility defects, ventriculomegaly and pituitary abnormalities are only present when Bbs5 is disrupted prior to postnatal day 7, indicating a developmental origin. In contrast, mutation of Bbs5 results in obesity, independent of the age of Bbs5 loss.
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Affiliation(s)
- Melissa R Bentley-Ford
- Department of Cell, Developmental and Integrative Biology, University of Alabama at Birmingham, Birmingham, AL 35294, USA
| | - Staci E Engle
- Department of Biology, Indiana University-Purdue University Indianapolis, Indianapolis, IN 46202, USA
| | - Kelsey R Clearman
- Department of Cell, Developmental and Integrative Biology, University of Alabama at Birmingham, Birmingham, AL 35294, USA
| | - Courtney J Haycraft
- Department of Cell, Developmental and Integrative Biology, University of Alabama at Birmingham, Birmingham, AL 35294, USA
| | - Reagan S Andersen
- Department of Cell, Developmental and Integrative Biology, University of Alabama at Birmingham, Birmingham, AL 35294, USA
| | - Mandy J Croyle
- Department of Cell, Developmental and Integrative Biology, University of Alabama at Birmingham, Birmingham, AL 35294, USA
| | - Addison B Rains
- Department of Cell, Developmental and Integrative Biology, University of Alabama at Birmingham, Birmingham, AL 35294, USA
| | - Nicolas F Berbari
- Department of Biology, Indiana University-Purdue University Indianapolis, Indianapolis, IN 46202, USA
| | - Bradley K Yoder
- Department of Cell, Developmental and Integrative Biology, University of Alabama at Birmingham, Birmingham, AL 35294, USA
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6
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Wochnik A, Stolarczyk L, Ambrožová I, Davídková M, De Saint-Hubert M, Domański S, Domingo C, Knežević Ž, Kopeć R, Kuć M, Majer M, Mojżeszek N, Mares V, Martínez-Rovira I, Caballero-Pacheco MÁ, Pyszka E, Swakoń J, Trinkl S, Tisi M, Harrison R, Olko P. Out-of-field doses for scanning proton radiotherapy of shallowly located paediatric tumours-a comparison of range shifter and 3D printed compensator. Phys Med Biol 2021; 66:035012. [PMID: 33202399 DOI: 10.1088/1361-6560/abcb1f] [Citation(s) in RCA: 12] [Impact Index Per Article: 4.0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/11/2022]
Abstract
The lowest possible energy of proton scanning beam in cyclotron proton therapy facilities is typically between 60 and 100 MeV. Treatment of superficial lesions requires a pre-absorber to deliver doses to shallower volumes. In most of the cases a range shifter (RS) is used, but as an alternative solution, a patient-specific 3D printed proton beam compensator (BC) can be applied. A BC enables further reduction of the air gap and consequently reduction of beam scattering. Such pre-absorbers are additional sources of secondary radiation. The aim of this work was the comparison of RS and BC with respect to out-of-field doses for a simulated treatment of superficial paediatric brain tumours. EURADOS WG9 performed comparative measurements of scattered radiation in the Proteus C-235 IBA facility (Cyclotron Centre Bronowice at the Institute of Nuclear Physics, CCB IFJ PAN, Kraków, Poland) using two anthropomorphic phantoms-5 and 10 yr old-for a superficial target in the brain. Both active detectors located inside the therapy room, and passive detectors placed inside the phantoms were used. Measurements were supplemented by Monte Carlo simulation of the radiation transport. For the applied 3D printed pre-absorbers, out-of-field doses from both secondary photons and neutrons were lower than for RS. Measurements with active environmental dosimeters at five positions inside the therapy room indicated that the RS/BC ratio of the out-of-field dose was also higher than one, with a maximum of 1.7. Photon dose inside phantoms leads to higher out-of-field doses for RS than BC to almost all organs with the highest RS/BC ratio 12.5 and 13.2 for breasts for 5 and 10 yr old phantoms, respectively. For organs closest to the isocentre such as the thyroid, neutron doses were lower for BC than RS due to neutrons moderation in the target volume, but for more distant organs like bladder-conversely-lower doses for RS than BC were observed. The use of 3D printed BC as the pre-absorber placed in the near vicinity of patient in the treatment of superficial tumours does not result in the increase of secondary radiation compared to the treatment with RS, placed far from the patient.
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Affiliation(s)
- A Wochnik
- Institute of Nuclear Physics PAN, Radzikowskiego 152, Krakow 31-342, Poland
| | - L Stolarczyk
- Institute of Nuclear Physics PAN, Radzikowskiego 152, Krakow 31-342, Poland.,Skandionkliniken, von Kraemers Allé 26, Uppsala 752 37, Sweden.,Dansk Center for Partikelterapi, Palle Juul-Jensens Boulevard 25, 8200 Aarhus N, Denmark
| | - I Ambrožová
- Department of Radiation Dosimetry, Nuclear Physics Institute Czech Academy of Sciences, Prague CZ-250 68 Řež, Czech Republic
| | - M Davídková
- Department of Radiation Dosimetry, Nuclear Physics Institute Czech Academy of Sciences, Prague CZ-250 68 Řež, Czech Republic
| | - M De Saint-Hubert
- Belgium Nuclear Research Centre (SCK CEN), Boeretang 200, Mol BE-2400, Belgium
| | - S Domański
- National Centre for Nuclear Research, Otwock-Świerk 05-400, Poland
| | - C Domingo
- Departament de Física, Universitat Autònoma de Barcelona (UAB), Bellaterra E-08193, Spain
| | - Ž Knežević
- Ruđer Bošković Institute, Bijenička c. 54, Zagreb 10000, Croatia
| | - R Kopeć
- Institute of Nuclear Physics PAN, Radzikowskiego 152, Krakow 31-342, Poland
| | - M Kuć
- National Centre for Nuclear Research, Otwock-Świerk 05-400, Poland
| | - M Majer
- Ruđer Bošković Institute, Bijenička c. 54, Zagreb 10000, Croatia
| | - N Mojżeszek
- Institute of Nuclear Physics PAN, Radzikowskiego 152, Krakow 31-342, Poland
| | - V Mares
- Helmholtz Zentrum München, Institute of Radiation Medicine, Ingolstädter Landstraße 1, Neuherberg 85764, Germany
| | - I Martínez-Rovira
- Departament de Física, Universitat Autònoma de Barcelona (UAB), Bellaterra E-08193, Spain
| | - M Á Caballero-Pacheco
- Departament de Física, Universitat Autònoma de Barcelona (UAB), Bellaterra E-08193, Spain
| | - E Pyszka
- Institute of Nuclear Physics PAN, Radzikowskiego 152, Krakow 31-342, Poland
| | - J Swakoń
- Institute of Nuclear Physics PAN, Radzikowskiego 152, Krakow 31-342, Poland
| | - S Trinkl
- Helmholtz Zentrum München, Institute of Radiation Medicine, Ingolstädter Landstraße 1, Neuherberg 85764, Germany.,Technische Universität München, Physik-Department, Garching 85748, Germany
| | - M Tisi
- Helmholtz Zentrum München, Institute of Radiation Medicine, Ingolstädter Landstraße 1, Neuherberg 85764, Germany
| | - R Harrison
- University of Newcastle upon Tyne, Tyne and Wear, Newcastle upon Tyne NE1 7RU, United Kingdom
| | - P Olko
- Institute of Nuclear Physics PAN, Radzikowskiego 152, Krakow 31-342, Poland
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7
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Hashemi Z, Tatari M, Naik H. Simulation of dose distribution and secondary particle production in proton therapy of brain tumor. Rep Pract Oncol Radiother 2020; 25:927-933. [PMID: 33088228 DOI: 10.1016/j.rpor.2020.08.015] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 01/13/2020] [Revised: 08/01/2020] [Accepted: 08/26/2020] [Indexed: 11/18/2022] Open
Abstract
Aim The aim of this study is simulation of the proton depth-dose distribution and dose evaluation of secondary particles in proton therapy of brain tumor using the GEANT4 and FLUKA Monte Carlo codes. Background Proton therapy is a treatment method for variety of tumors such as brain tumor. The most important feature of high energy proton beams is the energy deposition as a Bragg curve and the possibility of creating the spread out Bragg peak (SOBP) for full coverage of the tumor. Materials and methods A spherical tumor with the radius of 1 cm in the brain is considered. A SNYDER head phantom has been irradiated with 30-130 MeV proton beam energy. A PMMA modulator wheel is used for covering the tumor. The simulations are performed using the GEANT4 and FLUKA codes. Results Using a modulator wheel, the Spread Out Bragg Peak longitudinally and laterally covers the tumor. Flux and absorbed dose of secondary particles produced by nuclear interactions of protons with elements in the head are considerably small compared to protons. Conclusions Using 76.85 MeV proton beam and a modulator wheel, the tumor can be treated accurately in the 3-D, so that the distribution of proton dose in the surrounding tissues is very low. The results show that more than 99% of the total dose of secondary particles and protons is absorbed in the tumor.
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Affiliation(s)
- Zahra Hashemi
- Physics Department, Faculty of Science, Yazd University, Yazd 89195-741, Iran
| | - Mansoureh Tatari
- Physics Department, Faculty of Science, Yazd University, Yazd 89195-741, Iran
| | - Haladhara Naik
- Radiochemistry Division, Bhabha Atomic Research Centre, Mumbai 400085, India
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8
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Patterns of proton therapy use in pediatric cancer management in 2016: An international survey. Radiother Oncol 2019; 132:155-161. [DOI: 10.1016/j.radonc.2018.10.022] [Citation(s) in RCA: 31] [Impact Index Per Article: 6.2] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 09/12/2018] [Revised: 10/10/2018] [Accepted: 10/22/2018] [Indexed: 01/19/2023]
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9
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Stolarczyk L, Trinkl S, Romero-Expósito M, Mojżeszek N, Ambrozova I, Domingo C, Davídková M, Farah J, Kłodowska M, Knežević Ž, Liszka M, Majer M, Miljanić S, Ploc O, Schwarz M, Harrison RM, Olko P. Dose distribution of secondary radiation in a water phantom for a proton pencil beam-EURADOS WG9 intercomparison exercise. Phys Med Biol 2018; 63:085017. [PMID: 29509148 DOI: 10.1088/1361-6560/aab469] [Citation(s) in RCA: 25] [Impact Index Per Article: 4.2] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/12/2022]
Abstract
Systematic 3D mapping of out-of-field doses induced by a therapeutic proton pencil scanning beam in a 300 × 300 × 600 mm3 water phantom was performed using a set of thermoluminescence detectors (TLDs): MTS-7 (7LiF:Mg,Ti), MTS-6 (6LiF:Mg,Ti), MTS-N (natLiF:Mg,Ti) and TLD-700 (7LiF:Mg,Ti), radiophotoluminescent (RPL) detectors GD-352M and GD-302M, and polyallyldiglycol carbonate (PADC)-based (C12H18O7) track-etched detectors. Neutron and gamma-ray doses, as well as linear energy transfer distributions, were experimentally determined at 200 points within the phantom. In parallel, the Geant4 Monte Carlo code was applied to calculate neutron and gamma radiation spectra at the position of each detector. For the cubic proton target volume of 100 × 100 × 100 mm3 (spread out Bragg peak with a modulation of 100 mm) the scattered photon doses along the main axis of the phantom perpendicular to the primary beam were approximately 0.5 mGy Gy-1 at a distance of 100 mm and 0.02 mGy Gy-1 at 300 mm from the center of the target. For the neutrons, the corresponding values of dose equivalent were found to be ~0.7 and ~0.06 mSv Gy-1, respectively. The measured neutron doses were comparable with the out-of-field neutron doses from a similar experiment with 20 MV x-rays, whereas photon doses for the scanning proton beam were up to three orders of magnitude lower.
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Affiliation(s)
- L Stolarczyk
- Institute of Nuclear Physics PAN, Radzikowskiego 152, 31-342 Krakow, Poland. Skandionkliniken, von Kraemers Allé 26, 752 37 Uppsala, Sweden. Author to whom any correspondence should be addressed
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Hakimi A, Sohrabi M. Photoneutron depth dose equivalent distributions in high-energy X-ray medical accelerators by a novel position-sensitive dosimeter. Phys Med 2017; 36:73-80. [PMID: 28410689 DOI: 10.1016/j.ejmp.2017.03.010] [Citation(s) in RCA: 10] [Impact Index Per Article: 1.4] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Journal Information] [Submit a Manuscript] [Subscribe] [Scholar Register] [Received: 07/03/2016] [Revised: 03/17/2017] [Accepted: 03/18/2017] [Indexed: 10/19/2022] Open
Abstract
PURPOSE The purpose of this study was to; (1) investigate employing a novel position-sensitive mega-size polycarbonate (MSPC) dosimeter for photoneutron (PN) depth, profile and dose equivalent distributions studies in a multilayer polyethylene phantom in a Siemens ONCOR accelerator, and (2) develop depth dose equivalent distribution matrix data at different depths and positions of the phantom for patient PN dose equivalent determination and in particular for PN secondary cancer risk estimation. METHODS Position-sensitive MSPC dosimeters were successfully exposed at 9 different depths of the phantom in a 10×10cm2 X-ray field. The dosimeters were processed in mega-size electrochemical chambers at optimum conditions. Each MSPC dosimeter was placed at a known phantom depth for PN depth dose equivalents and profiles on transverse, longitudinal and diagonal axes and isodose equivalent distribution studies in and out of the X-ray beam. RESULTS PN dose equivalent distributions at any depth showed the highest value at the beam central axis and decreases as the distance increases. PN dose equivalent at any position studied in the axes has a maximum value on the phantom surface which decreases as depth increases due to flux reduction by multi-elastic scattering interactions. CONCLUSIONS Extensive PN dose equivalent matrix data at different depths and positions in the phantom were determined. The position-sensitive MSPC dosimeters proved to be highly efficient for PN depth, profile and isodose equivalent distribution studies. The extensive data obtained highly assists for determining PN dose equivalent of a patient undergoing high-energy X-ray therapy and for PN secondary cancer risk estimation.
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Affiliation(s)
- Amir Hakimi
- Health Physics and Dosimetry Research Laboratory, Department of Energy Engineering and Physics, Amirkabir University of Technology, Tehran, Iran
| | - Mehdi Sohrabi
- Health Physics and Dosimetry Research Laboratory, Department of Energy Engineering and Physics, Amirkabir University of Technology, Tehran, Iran.
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Measurement of stray neutron doses inside the treatment room from a proton pencil beam scanning system. Phys Med 2017; 34:80-84. [DOI: 10.1016/j.ejmp.2017.01.013] [Citation(s) in RCA: 16] [Impact Index Per Article: 2.3] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Submit a Manuscript] [Subscribe] [Scholar Register] [Received: 08/30/2016] [Revised: 01/09/2017] [Accepted: 01/18/2017] [Indexed: 11/18/2022] Open
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12
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Cadini F, Bolst D, Guatelli S, Beltran C, Jackson M, Rosenfeld AB. Neutron shielding for a new projected proton therapy facility: A Geant4 simulation study. Phys Med 2016; 32:1862-1871. [PMID: 28024848 DOI: 10.1016/j.ejmp.2016.12.003] [Citation(s) in RCA: 4] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [Abstract] [Key Words] [MESH Headings] [Track Full Text] [Journal Information] [Submit a Manuscript] [Subscribe] [Scholar Register] [Received: 07/25/2016] [Revised: 11/30/2016] [Accepted: 12/04/2016] [Indexed: 01/11/2023] Open
Abstract
In this work, we used the Monte Carlo-based Geant4 simulation toolkit to calculate the ambient dose equivalents due to the secondary neutron field produced in a new projected proton therapy facility. In particular the facility geometry was modeled in Geant4 based on the CAD design. Proton beams were originated with an energy of 250MeV in the gantry rooms with different angles with respect to the patient; a fixed 250MeV proton beam was also modeled. The ambient dose equivalent was calculated in several locations of interest inside and outside the facility, for different scenarios. The simulation results were compared qualitatively to previous work on an existing facility bearing some similarities with the design under study, showing that the ambient dose equivalent ranges obtained are reasonable. The ambient dose equivalents, calculated by means of the Geant4 simulation, were compared to the Australian regulatory limits and showed that the new facility will not pose health risks for the public or staff, with a maximum equivalent dose rate equal to 7.9mSv/y in the control rooms and maze exit areas and 1.3·10-1mSv/y close to the walls, outside the facility, under very conservative assumptions. This work represents the first neutron shielding verification analysis of a new projected proton therapy facility and, as such, it may serve as a new source of comparison and validation for the international community, besides confirming the viability of the project from a radioprotection point of view.
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Affiliation(s)
- Francesco Cadini
- Politecnico di Milano, Dipartimento di Energia, Via La Masa 34, I-20156 Milano, Italy; Centre for Medical Radiation Physics, University of Wollongong, NSW, Australia.
| | - David Bolst
- Centre for Medical Radiation Physics, University of Wollongong, NSW, Australia
| | - Susanna Guatelli
- Centre for Medical Radiation Physics, University of Wollongong, NSW, Australia; Illawarra Health Medical Research Institute, University of Wollongong, NSW, Australia
| | | | - Michael Jackson
- Department of Radiation Oncology, Prince of Wales Hospital, Randwick, Australia
| | - Anatoly B Rosenfeld
- Centre for Medical Radiation Physics, University of Wollongong, NSW, Australia; Illawarra Health Medical Research Institute, University of Wollongong, NSW, Australia
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