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Valceski M, Engels E, Vogel S, Paino J, Potter D, Hollis C, Khochaiche A, Barnes M, Cameron M, O'Keefe A, Roughley K, Rosenfeld A, Lerch M, Corde S, Tehei M. A novel approach to double-strand DNA break analysis through γ-H2AX confocal image quantification and bio-dosimetry. Sci Rep 2024; 14:27591. [PMID: 39528587 PMCID: PMC11554680 DOI: 10.1038/s41598-024-76683-5] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [MESH Headings] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 07/18/2024] [Accepted: 10/16/2024] [Indexed: 11/16/2024] Open
Abstract
DNA damage occurs in all living cells. γ-H2AX imaging by fluorescent microscopy is widely used across disciplines in the analysis of double-strand break (DSB) DNA damage. Here we demonstrate a method for the quantitative analysis of such DBSs. Ionising radiation, well known to induce DSBs, is used in this demonstration, and additional DBSs are induced if high-Z nanoparticles are present during irradiation. As a deliberate test of the methodology, cells are exposed to a spatially fractionated ionising radiation field, characterised by regions of high and low absorbed radiation dose that are only ever qualitatively verified biologically via γ-H2AX imaging. Here we validate our bio-dosimetric quantification method using γ-H2AX assays in the assessment of DSB enhancement. Our method reliably quantifies DSB enhancement in cells when exposed to either a spatially contiguous or fractionated irradiation fields. Using the γ-H2AX assay, we deduce the biological dose response, and for the first time, demonstrate equivalence to the independently measured physical absorbed dose. Using our novel method, we are also able quantify the nanoparticle DSB enhancement at the cellular level, which is not possible using physical dose measurement techniques. Our method therefore provides a new paradigm in γ-H2AX image quantification of DSBs, as well as an independently validated bio-dosimetry technique.
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Affiliation(s)
- Michael Valceski
- Centre for Medical Radiation Physics, University of Wollongong, Wollongong, NSW, 2522, Australia
- Molecular Horizons, University of Wollongong, Wollongong, NSW, 2522, Australia
| | - Elette Engels
- Centre for Medical Radiation Physics, University of Wollongong, Wollongong, NSW, 2522, Australia
- Australian Synchrotron - Australian Nuclear Science and Technology Organisation (ANSTO), 800 Blackburn Road, Clayton, VIC, 3168, Australia
| | - Sarah Vogel
- Centre for Medical Radiation Physics, University of Wollongong, Wollongong, NSW, 2522, Australia
- Molecular Horizons, University of Wollongong, Wollongong, NSW, 2522, Australia
| | - Jason Paino
- Centre for Medical Radiation Physics, University of Wollongong, Wollongong, NSW, 2522, Australia
| | - Dylan Potter
- Centre for Medical Radiation Physics, University of Wollongong, Wollongong, NSW, 2522, Australia
- Molecular Horizons, University of Wollongong, Wollongong, NSW, 2522, Australia
| | - Carolyn Hollis
- Centre for Medical Radiation Physics, University of Wollongong, Wollongong, NSW, 2522, Australia
- Molecular Horizons, University of Wollongong, Wollongong, NSW, 2522, Australia
| | - Abass Khochaiche
- Centre for Medical Radiation Physics, University of Wollongong, Wollongong, NSW, 2522, Australia
- Molecular Horizons, University of Wollongong, Wollongong, NSW, 2522, Australia
| | - Micah Barnes
- Centre for Medical Radiation Physics, University of Wollongong, Wollongong, NSW, 2522, Australia
| | - Matthew Cameron
- Australian Synchrotron - Australian Nuclear Science and Technology Organisation (ANSTO), 800 Blackburn Road, Clayton, VIC, 3168, Australia
| | - Alice O'Keefe
- Centre for Medical Radiation Physics, University of Wollongong, Wollongong, NSW, 2522, Australia
- Molecular Horizons, University of Wollongong, Wollongong, NSW, 2522, Australia
| | - Kiarn Roughley
- Centre for Medical Radiation Physics, University of Wollongong, Wollongong, NSW, 2522, Australia
- Molecular Horizons, University of Wollongong, Wollongong, NSW, 2522, Australia
| | - Anatoly Rosenfeld
- Centre for Medical Radiation Physics, University of Wollongong, Wollongong, NSW, 2522, Australia
| | - Michael Lerch
- Centre for Medical Radiation Physics, University of Wollongong, Wollongong, NSW, 2522, Australia
| | - Stéphanie Corde
- Centre for Medical Radiation Physics, University of Wollongong, Wollongong, NSW, 2522, Australia
- Prince of Wales Hospital, Randwick, NSW, 2031, Australia
| | - Moeava Tehei
- Centre for Medical Radiation Physics, University of Wollongong, Wollongong, NSW, 2522, Australia.
- Molecular Horizons, University of Wollongong, Wollongong, NSW, 2522, Australia.
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Ma J, Shen H, Mi Z. Enhancing Proton Therapy Efficacy Through Nanoparticle-Mediated Radiosensitization. Cells 2024; 13:1841. [PMID: 39594590 PMCID: PMC11593106 DOI: 10.3390/cells13221841] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [MESH Headings] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 10/01/2024] [Revised: 11/04/2024] [Accepted: 11/05/2024] [Indexed: 11/28/2024] Open
Abstract
Proton therapy, characterized by its unique Bragg peak, offers the potential to optimize the destruction of cancer cells while sparing healthy tissues, positioning it as one of the most advanced cancer treatment modalities currently available. However, in comparison to heavy ions, protons exhibit a relatively lower relative biological effectiveness (RBE), which limits the efficacy of proton therapy. The incorporation of nanoparticles for radiosensitization presents a novel approach to enhance the RBE of protons. This review provides a comprehensive discussion of the recent advancements in augmenting the biological effects of proton therapy through the use of nanoparticles. It examines the various types of nanoparticles that have been the focus of extensive research, elucidates their mechanisms of radiation sensitization, and evaluates the factors influencing the efficiency of this sensitization process. Furthermore, this review discusses the latest synergistic therapeutic strategies that integrate nanoparticle-mediated radiosensitization and outlines prospective directions for the future application of nanoparticles in conjunction with proton therapy.
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Affiliation(s)
| | | | - Zhaohong Mi
- Key Laboratory of Nuclear Physics and Ion-Beam Application (MOE), Institute of Modern Physics, Fudan University, Shanghai 200433, China
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ÇAĞLAR M, EŞİTMEZ D, CEBE MS. The Effect of Dose Enhancement in Tumor With Silver Nanoparticles on Surrounding Healthy Tissues: A Monte Carlo Study. Technol Cancer Res Treat 2024; 23:15330338241235771. [PMID: 38449099 PMCID: PMC10919133 DOI: 10.1177/15330338241235771] [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: 09/06/2023] [Revised: 01/18/2024] [Accepted: 02/12/2024] [Indexed: 03/08/2024] Open
Abstract
Objectives: Cancer-related death rates account for approximately one-third of all deaths, and this rate is increasing remarkably every year. In this study, we examined the dose enhancement factor (DEF) in the tumor and surrounding tissues by adding different concentrations of silver nanoparticles (AgNPs) to the brain tumor using the Monte Carlo (MC) technique. Methods: This study used MCNP6.2 simulation software. A Planning Target Volume (PTV) of 1 × 1 × 1 cm3 was placed in the center of a cubic cranial model with dimensions of 5 × 5 × 5 cm3. Five different simulations were initially generated using the simple method. These simulations included pure PTV and PTV consisting of 4 different silver concentrations (5, 10, 20, and 30 mg/g). Additionally, a model was created using the nanolattice method, considering the size, position, and distribution of the AgNPs. Irradiation was performed using a source with a 6 MV linac photon spectrum. Measurements were performed using the *f8 tally, and DEF values were calculated. Results: In the simulation study using the simple method, the DEF value of PTV increased linearly with concentration, whereas the DEF values were lower than the simulation results with the nanolattice model (1.9 vs 1.4 for 30 mg/g NP concentration). Performing the simple method, we observed no remarkable dose increase in lateral OARs surrounding PTV. While a remarkable dose decrease was observed in distal OARs, a dose increase in the proximal OAR was observed, which was consistent with that of PTV. However, according to the results obtained by performing the nanolattice method, the dose increase was observed in both the proximal OAR and the distal OAR and was similar to that of PTV. Conclusion: While enhancing the dose in the tumor by adding NPs into the tumor, it is essential to consider whether it also increases the OAR dose. In addition, simulation studies on NPs showed that the dose increase varied significantly with particle size, position, and distribution. Hence, these factors should be considered carefully.
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Affiliation(s)
- Mustafa ÇAĞLAR
- Department of Health Physics, Graduate School of Health Sciences, İstanbul Medipol University, İstanbul, Türkiye
| | - Dursun EŞİTMEZ
- Department of Health Physics, Graduate School of Health Sciences, İstanbul Medipol University, İstanbul, Türkiye
| | - Mehmet Sıddık CEBE
- Department of Health Physics, Graduate School of Health Sciences, İstanbul Medipol University, İstanbul, Türkiye
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Zhao X, Liu R, Zhao T, Reynoso FJ. Quantification of gold nanoparticle photon radiosensitization from direct and indirect effects using a complete human genome single cell model based on Geant4. Med Phys 2021; 48:8127-8139. [PMID: 34738643 DOI: 10.1002/mp.15330] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 11/12/2020] [Revised: 09/22/2021] [Accepted: 10/20/2021] [Indexed: 11/08/2022] Open
Abstract
PURPOSE To investigate the radiosensitization properties of gold nanoparticles (GNPs) and better understand the intricate deoxyribonucleic acid (DNA) damage induction mechanisms involved in GNP-aided radiotherapy, a single cell model with complete human genome based on the Geant4 Monte Carlo toolkit was applied. MATERIALS AND METHODS A Geant4-DNA model was implemented to simulate direct and indirect DNA damage generated in the physical and chemical stages. In the physical stage, a mixed-physics approach was taken by using Geant4-DNA in water and Livermore in gold. Water radiolysis was created posteriorly in the physicochemical and chemical stages to simulate indirect damage from reactions between DNA molecules and OH• radicals. A mono-energetic photon beam (100 keV) and two clinical photon sources (250-kVp, 6-MV flattening-filter free) were simulated for modeling the irradiation of a single cell with or without GNPs. In order to study the effects of GNP size on radiosensitization, 15, 30, and 100 nm GNPs were simulated. The effects of intracellular distribution were simulated using 90-nm GNPs with different characteristics of distribution within the cell. The time dependence of DNA damage enhancement was also studied with chemistry stage simulation end-time no larger than 10 ns. RESULTS Double strand break (DSB) enhancement due to direct and indirect action was quantified under different scenarios. Under realistic cellular uptake condition, the 100-nm GNPs had the most significant increase in DSBs: 40.9% and 28.5% for 100 keV and 250-kVp photon irradiation, respectively. The intracellular localization showed differing levels of radiosensitization with a maximum of 64%, 27%, and 6% DSB enhancements for 100 keV, 250-kVp, and 6-MV respectively, when 90-nm GNPs congregate around the nucleus. CONCLUSION The results indicate that photon energy, GNP size, and intracellular distribution play an important role in the enhancement of DSB from direct and indirect damage under scenarios close to cell experiments. The radiosensitization effects due to indirect damage are significant and should be considered carefully.
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Affiliation(s)
- Xiandong Zhao
- Department of Radiation Oncology, Washington University School of Medicine, St. Louis, Missouri, USA
| | - Ruirui Liu
- Department of Radiation Oncology, Washington University School of Medicine, St. Louis, Missouri, USA
| | - Tianyu Zhao
- Department of Radiation Oncology, Washington University School of Medicine, St. Louis, Missouri, USA
| | - Francisco J Reynoso
- Department of Radiation Oncology, Washington University School of Medicine, St. Louis, Missouri, USA
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Maigne L, Delsol A, Fois G, Debiton E, Degoul F, Payno H. CPOP: An open source C++ cell POPulation modeler for radiation biology applications. Phys Med 2021; 89:41-50. [PMID: 34343765 DOI: 10.1016/j.ejmp.2021.07.016] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [Abstract] [Key Words] [MESH Headings] [Track Full Text] [Journal Information] [Submit a Manuscript] [Subscribe] [Scholar Register] [Received: 01/27/2021] [Revised: 07/12/2021] [Accepted: 07/13/2021] [Indexed: 11/20/2022] Open
Abstract
PURPOSE Multicellular tumor spheroids are realistic in-vitro systems used in radiation biology research to study the effect of anticancer drugs or to evaluate the resistance of cancer cells under specific conditions. When combining the modeling of spheroids together with the simulation of radiation using Monte Carlo methods, one could estimate cell and DNA damage to be compared with experimental data. We developed a Cell Population (CPOP) modeler combined to Geant4 simulations in order to tackle how energy depositions are allocated to cells, especially when enhancing radiation outcomes using high-Z nanoparticles. CPOP manages to model large three-dimensional cell populations with independent deformable cells described with their nucleus, cytoplasm and membranes together with force law systems to manage cell-cell interactions. METHODS CPOP is an opensource platform written in C++. It is divided into two main libraries: a "Modeler" library, for cell geometry modeling using meshes, and a Multi Agent System (MAS) library, simulating all agent (cell) interactions among the population. CPOP is fully interfaced with the Geant4 Monte Carlo toolkit and is able to directly launch Geant4 simulations after compilation. We modeled a full and realistic 3D cell population from SK-MEL28 melanoma cell population cultured experimentally. The spheroid diameter of 550 ± 40 µm corresponds to a population of approximately 1000 cells having a diameter of 17.2 ± 2.5 µm and a nucleus diameter of 11.2 ± 2.0 µm. We decided to reproduce cell irradiations performed with a X-RAD 320 Biological Irradiator (Precision XRay Inc., North Branford, CT). RESULTS We simulated the energy spectrum of secondary particles generated in the vicinity of the spheroid and plotted the different energy spectra recovered internally to the spheroid. We evaluated also the impact of AGuIX (Gadolinium) nanoparticles modeled into the spheroid with their corresponding secondary energy spectra. CONCLUSIONS We succeeded into modeling cell populations and combined them with Geant4 simulations. The next step will be to integrate DNA geometrical models into cell nuclei and to use the Geant4-DNA physics and radiolysis modeling capabilities in order to evaluate early strand breaks induced on DNA.
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Affiliation(s)
- L Maigne
- Université Clermont Auvergne, CNRS/IN2P3, LPC, 63000 Clermont-Ferrand, France.
| | - A Delsol
- Université Clermont Auvergne, CNRS/IN2P3, LPC, 63000 Clermont-Ferrand, France
| | - G Fois
- Université Clermont Auvergne, CNRS/IN2P3, LPC, 63000 Clermont-Ferrand, France
| | - E Debiton
- INSERM, 1240, 58 Rue Montalembert, 63 005 Clermont-Ferrand cedex, France; Université Clermont Auvergne, Imagerie Moléculaire et Stratégies Théranostiques, BP 10448, 63000 Clermont-Ferrand, France
| | - F Degoul
- INSERM, 1240, 58 Rue Montalembert, 63 005 Clermont-Ferrand cedex, France; Université Clermont Auvergne, Imagerie Moléculaire et Stratégies Théranostiques, BP 10448, 63000 Clermont-Ferrand, France
| | - H Payno
- Université Clermont Auvergne, CNRS/IN2P3, LPC, 63000 Clermont-Ferrand, France
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Khochaiche A, Westlake M, O'Keefe A, Engels E, Vogel S, Valceski M, Li N, Rule KC, Horvat J, Konstantinov K, Rosenfeld A, Lerch M, Corde S, Tehei M. First extensive study of silver-doped lanthanum manganite nanoparticles for inducing selective chemotherapy and radio-toxicity enhancement. MATERIALS SCIENCE & ENGINEERING. C, MATERIALS FOR BIOLOGICAL APPLICATIONS 2021; 123:111970. [PMID: 33812598 DOI: 10.1016/j.msec.2021.111970] [Citation(s) in RCA: 5] [Impact Index Per Article: 1.3] [Reference Citation Analysis] [Abstract] [Key Words] [MESH Headings] [Track Full Text] [Subscribe] [Scholar Register] [Received: 10/30/2020] [Revised: 02/05/2021] [Accepted: 02/08/2021] [Indexed: 01/22/2023]
Abstract
Nanoparticles have a great potential to increase the therapeutic efficiency of several cancer therapies. This research examines the potential for silver-doped lanthanum manganite nanoparticles to enhance radiation therapy to target radioresistant brain cancer cells, and their potential in combinational therapy with magnetic hyperthermia. Magnetic and structural characterisation found all dopings of nanoparticles (NPs) to be pure and single phase with an average crystallite size of approximately 15 nm for undoped NPs and 20 nm for silver doped NPs. Additionally, neutron diffraction reveals that La0.9Ag0.1MnO3 (10%-LAGMO) NPs exhibit residual ferromagnetism at 300 K that is not present in lower doped NPs studied in this work, indicating that the Curie temperature may be manipulated according to silver doping. This radiobiological study reveals a completely cancer-cell selective treatment for LaMnO3, La0.975Ag0.025MnO3 and La0.95Ag0.05MnO3 (0, 2.5 and 5%-LAGMO) and also uncovers a potent combination of undoped lanthanum manganite with orthovoltage radiation. Cell viability assays and real time imaging results indicated that a concentration of 50 μg/mL of the aforementioned nanoparticles do not affect the growth of Madin-Darby Canine Kidney (MDCK) non-cancerous cells over time, but stimulate its metabolism for overgrowth, while being highly toxic to 9L gliosarcoma (9LGS). This is not the case for 10%-LAGMO nanoparticles, which were toxic to both non-cancerous and cancer cell lines. The nanoparticles also exhibited a level of toxicity that was regulated by the overproduction of free radicals, such as reactive oxygen species, amplified when silver ions are involved. With the aid of fluorescent imaging, the drastic effects of these reactive oxygen species were visualised, where nucleus cleavage (an apoptotic indicator) was identified as a major consequence. The genotoxic response of this effect for 9LGS and MDCK due to 10%-LAGMO NPs indicates that it is also causing DNA double strand breaks within the cell nucleus. Using 125 kVp orthovoltage radiation, in combination with an appropriate amount of NP-induced cell death, identified undoped lanthanum manganite as the most ideal treatment. Real-time imaging following the combination treatment of undoped lanthanum manganite nanoparticles and radiation, highlighted a hinderance of growth for 9LGS, while MDCK growth was boosted. The clonogenic assay following incubation with undoped lanthanum manganite nanoparticles combined with a relatively low dose of radiation (2 Gy) decreased the surviving fraction to an exceptionally low (0.6 ± 6.7)%. To our knowledge, these results present the first biological in-depth analysis on silver-doped lanthanum manganite as a brain cancer selective chemotherapeutic and radiation dose enhancer and as a result will propel its first in vivo investigation.
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Affiliation(s)
- Abass Khochaiche
- Centre for Medical Radiation Physics, University of Wollongong, Wollongong, Australia; School of Physics, University of Wollongong, Wollongong, Australia; Illawarra Health and Medical Research Institute (IHMRI), University of Wollongong, Wollongong, Australia; Molecular Horizons, School of Chemistry and Molecular, Bioscience University of Wollongong, Wollongong, Australia
| | - Matt Westlake
- Centre for Medical Radiation Physics, University of Wollongong, Wollongong, Australia; School of Physics, University of Wollongong, Wollongong, Australia; Illawarra Health and Medical Research Institute (IHMRI), University of Wollongong, Wollongong, Australia; Molecular Horizons, School of Chemistry and Molecular, Bioscience University of Wollongong, Wollongong, Australia
| | - Alice O'Keefe
- Centre for Medical Radiation Physics, University of Wollongong, Wollongong, Australia; School of Physics, University of Wollongong, Wollongong, Australia; Illawarra Health and Medical Research Institute (IHMRI), University of Wollongong, Wollongong, Australia; Molecular Horizons, School of Chemistry and Molecular, Bioscience University of Wollongong, Wollongong, Australia
| | - Elette Engels
- Centre for Medical Radiation Physics, University of Wollongong, Wollongong, Australia; School of Physics, University of Wollongong, Wollongong, Australia; Illawarra Health and Medical Research Institute (IHMRI), University of Wollongong, Wollongong, Australia; Molecular Horizons, School of Chemistry and Molecular, Bioscience University of Wollongong, Wollongong, Australia
| | - Sarah Vogel
- Centre for Medical Radiation Physics, University of Wollongong, Wollongong, Australia; School of Physics, University of Wollongong, Wollongong, Australia; Illawarra Health and Medical Research Institute (IHMRI), University of Wollongong, Wollongong, Australia; Molecular Horizons, School of Chemistry and Molecular, Bioscience University of Wollongong, Wollongong, Australia
| | - Michael Valceski
- Centre for Medical Radiation Physics, University of Wollongong, Wollongong, Australia; School of Physics, University of Wollongong, Wollongong, Australia; Illawarra Health and Medical Research Institute (IHMRI), University of Wollongong, Wollongong, Australia; Molecular Horizons, School of Chemistry and Molecular, Bioscience University of Wollongong, Wollongong, Australia
| | - Nan Li
- Centre for Medical Radiation Physics, University of Wollongong, Wollongong, Australia; School of Physics, University of Wollongong, Wollongong, Australia; Illawarra Health and Medical Research Institute (IHMRI), University of Wollongong, Wollongong, Australia
| | - Kirrily C Rule
- Australian Nuclear Science and Technology Organisation, ANSTO, Sydney, Australia
| | - Josip Horvat
- School of Physics, University of Wollongong, Wollongong, Australia
| | - Konstantin Konstantinov
- Illawarra Health and Medical Research Institute (IHMRI), University of Wollongong, Wollongong, Australia; Institute for Superconducting and Electronic Materials (ISEM), University of Wollongong, Wollongong, Australia
| | - Anatoly Rosenfeld
- Centre for Medical Radiation Physics, University of Wollongong, Wollongong, Australia; School of Physics, University of Wollongong, Wollongong, Australia; Illawarra Health and Medical Research Institute (IHMRI), University of Wollongong, Wollongong, Australia
| | - Michael Lerch
- Centre for Medical Radiation Physics, University of Wollongong, Wollongong, Australia; School of Physics, University of Wollongong, Wollongong, Australia; Illawarra Health and Medical Research Institute (IHMRI), University of Wollongong, Wollongong, Australia; Molecular Horizons, School of Chemistry and Molecular, Bioscience University of Wollongong, Wollongong, Australia
| | - Stéphanie Corde
- Centre for Medical Radiation Physics, University of Wollongong, Wollongong, Australia; School of Physics, University of Wollongong, Wollongong, Australia; Illawarra Health and Medical Research Institute (IHMRI), University of Wollongong, Wollongong, Australia; Department of Radiation Oncology, Prince of Wales Hospital, Randwick, Australia
| | - Moeava Tehei
- Centre for Medical Radiation Physics, University of Wollongong, Wollongong, Australia; School of Physics, University of Wollongong, Wollongong, Australia; Illawarra Health and Medical Research Institute (IHMRI), University of Wollongong, Wollongong, Australia; Molecular Horizons, School of Chemistry and Molecular, Bioscience University of Wollongong, Wollongong, Australia.
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Mohseni M, Kazemzadeh A, Ataei N, Moradi H, Aliasgharzadeh A, Farhood B. Study on the Dose Enhancement of Gold Nanoparticles When Exposed to Clinical Electron, Proton, and Alpha Particle Beams by Means of Geant4. JOURNAL OF MEDICAL SIGNALS & SENSORS 2021; 10:286-294. [PMID: 33575201 PMCID: PMC7866949 DOI: 10.4103/jmss.jmss_58_19] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [Abstract] [Key Words] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 10/22/2019] [Revised: 04/22/2020] [Accepted: 06/24/2020] [Indexed: 12/02/2022]
Abstract
Background: Various factors effecting deposited energy and dose enhancement ratio (DER) in the simplified model of cell caused by the interaction of a cluster of gold nanoparticles (GNPs) with electron beams were assessed, and the results were compared with other sources through Geant4 Monte Carlo simulation toolkit. Method: The effect of added GNPs on the DNA strand breaks level, irradiated to electron, proton, and alpha beams, is assessed. Results: Presence of GNPs in the cell makes DER value more pronounced for low-energy photons rather than electron beam. Moreover, the results of DER values did not show any significant increase in absorbed dose in the presence of GNP for proton and alpha beam. Moreover, the results of DNA break with GNPs for proton and alpha beam were negligible. It is demonstrated that as the sizes of the GNPs increase, the DER is enlarged until a certain size for 40 keV photons, while there is no striking change for 50 keV electron beam when the size of the GNPs changes. The results indicate that although energy deposited in the cell for electron beam is more than low-energy photon, DER values are low compared to photon. Conclusion: Larger GNPs do not show any preference over smaller ones when irradiated through electron beams. It is proved that GNPs do not significantly increase single-strand breaks (SSBs) and double-strand breaks during electron irradiation, while there exists a direct relationship between SSB and energy.
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Affiliation(s)
- Mehran Mohseni
- Department of Medical Physics, Kashan University of Medical Science, Kashan, Iran
| | - Arezoo Kazemzadeh
- Department of Medical Physics, Kashan University of Medical Science, Kashan, Iran
| | - Nafiseh Ataei
- Department of Medical Physics, Kashan University of Medical Science, Kashan, Iran
| | - Habiballah Moradi
- Department of Medical Physics, Kashan University of Medical Science, Kashan, Iran
| | - Akbar Aliasgharzadeh
- Department of Medical Physics, Kashan University of Medical Science, Kashan, Iran
| | - Bagher Farhood
- Department of Medical Physics, Kashan University of Medical Science, Kashan, Iran
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Engels E, Bakr S, Bolst D, Sakata D, Li N, Lazarakis P, McMahon SJ, Ivanchenko V, Rosenfeld AB, Incerti S, Kyriakou I, Emfietzoglou D, Lerch MLF, Tehei M, Corde S, Guatelli S. Advances in modelling gold nanoparticle radiosensitization using new Geant4-DNA physics models. Phys Med Biol 2020; 65:225017. [PMID: 32916674 DOI: 10.1088/1361-6560/abb7c2] [Citation(s) in RCA: 13] [Impact Index Per Article: 2.6] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 12/31/2022]
Abstract
Gold nanoparticles have demonstrated significant radiosensitization of cancer treatment with x-ray radiotherapy. To understand the mechanisms at the basis of nanoparticle radiosensitization, Monte Carlo simulations are used to investigate the dose enhancement, given a certain nanoparticle concentration and distribution in the biological medium. Earlier studies have ordinarily used condensed history physics models to predict nanoscale dose enhancement with nanoparticles. This study uses Geant4-DNA complemented with novel track structure physics models to accurately describe electron interactions in gold and to calculate the dose surrounding gold nanoparticle structures at nanoscale level. The computed dose in silico due to a clinical kilovoltage beam and the presence of gold nanoparticles was related to in vitro brain cancer cell survival using the local effect model. The comparison of the simulation results with radiobiological experimental measurements shows that Geant4-DNA and local effect model can be used to predict cell survival in silico in the case of x-ray kilovoltage beams.
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Affiliation(s)
- Elette Engels
- Centre for Medical Radiation Physics, University of Wollongong, Wollongong, NSW, Australia. Illawarra Health and Medical Research Institute, University of Wollongong, Wollongong, NSW, Australia
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Spiga J, Pellicioli P, Manger SP, Duffy JA, Bravin A. Experimental benchmarking of Monte Carlo simulations for radiotherapy dosimetry using monochromatic X-ray beams in the presence of metal-based compounds. Phys Med 2019; 66:45-54. [DOI: 10.1016/j.ejmp.2019.09.075] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.2] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Submit a Manuscript] [Subscribe] [Scholar Register] [Received: 02/04/2019] [Revised: 08/03/2019] [Accepted: 09/11/2019] [Indexed: 10/25/2022] Open
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10
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Engels E, Westlake M, Li N, Vogel S, Gobert Q, Thorpe N, Rosenfeld A, Lerch M, Corde S, Tehei M. Thulium Oxide Nanoparticles: A new candidate for image-guided radiotherapy. Biomed Phys Eng Express 2018. [DOI: 10.1088/2057-1976/aaca01] [Citation(s) in RCA: 16] [Impact Index Per Article: 2.3] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 01/27/2023]
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11
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McDonald M, Oktaria S, Konstantinov K, Rosenfeld A, Lerch M, Corde S, Tehei M. Radiosensitisation enhancement effect of BrUdR and Ta
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NSPs in combination with 5-Fluorouracil antimetabolite in kilovoltage and megavoltage radiation. Biomed Phys Eng Express 2018. [DOI: 10.1088/2057-1976/aabab2] [Citation(s) in RCA: 4] [Impact Index Per Article: 0.6] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 02/07/2023]
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Lazarakis P, Incerti S, Ivanchenko V, Kyriakou I, Emfietzoglou D, Corde S, Rosenfeld AB, Lerch M, Tehei M, Guatelli S. Investigation of track structure and condensed history physics models for applications in radiation dosimetry on a micro and nano scale in Geant4. Biomed Phys Eng Express 2018. [DOI: 10.1088/2057-1976/aaa6aa] [Citation(s) in RCA: 42] [Impact Index Per Article: 6.0] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/11/2022]
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Liu Y, Zhang P, Li F, Jin X, Li J, Chen W, Li Q. Metal-based NanoEnhancers for Future Radiotherapy: Radiosensitizing and Synergistic Effects on Tumor Cells. Theranostics 2018; 8:1824-1849. [PMID: 29556359 PMCID: PMC5858503 DOI: 10.7150/thno.22172] [Citation(s) in RCA: 180] [Impact Index Per Article: 25.7] [Reference Citation Analysis] [Abstract] [Key Words] [MESH Headings] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 07/31/2017] [Accepted: 01/05/2018] [Indexed: 12/13/2022] Open
Abstract
Radiotherapy is one of the major therapeutic strategies for cancer treatment. In the past decade, there has been growing interest in using high Z (atomic number) elements (materials) as radiosensitizers. New strategies in nanomedicine could help to improve cancer diagnosis and therapy at cellular and molecular levels. Metal-based nanoparticles usually exhibit chemical inertness in cellular and subcellular systems and may play a role in radiosensitization and synergistic cell-killing effects for radiation therapy. This review summarizes the efficacy of metal-based NanoEnhancers against cancers in both in vitro and in vivo systems for a range of ionizing radiations including gamma-rays, X-rays, and charged particles. The potential of translating preclinical studies on metal-based nanoparticles-enhanced radiation therapy into clinical practice is also discussed using examples of several metal-based NanoEnhancers (such as CYT-6091, AGuIX, and NBTXR3). Also, a few general examples of theranostic multimetallic nanocomposites are presented, and the related biological mechanisms are discussed.
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Affiliation(s)
- Yan Liu
- Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou, China
- Key Laboratory of Heavy Ion Radiation Biology and Medicine of Chinese Academy of Sciences, Lanzhou, China
- Key Laboratory of Basic Research on Heavy Ion Radiation Application in Medicine, Gansu Province, Lanzhou, China
- University of Chinese Academy of Sciences, Beijing, China
| | - Pengcheng Zhang
- Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou, China
- Key Laboratory of Heavy Ion Radiation Biology and Medicine of Chinese Academy of Sciences, Lanzhou, China
- Key Laboratory of Basic Research on Heavy Ion Radiation Application in Medicine, Gansu Province, Lanzhou, China
- University of Chinese Academy of Sciences, Beijing, China
| | - Feifei Li
- Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou, China
- Key Laboratory of Heavy Ion Radiation Biology and Medicine of Chinese Academy of Sciences, Lanzhou, China
- Key Laboratory of Basic Research on Heavy Ion Radiation Application in Medicine, Gansu Province, Lanzhou, China
- University of Chinese Academy of Sciences, Beijing, China
| | - Xiaodong Jin
- Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou, China
- Key Laboratory of Heavy Ion Radiation Biology and Medicine of Chinese Academy of Sciences, Lanzhou, China
- Key Laboratory of Basic Research on Heavy Ion Radiation Application in Medicine, Gansu Province, Lanzhou, China
| | - Jin Li
- State Key Laboratory of Grassland Agro-ecosystems, College of Pastoral Agriculture Science and Technology, Lanzhou University, Lanzhou, China
| | - Weiqiang Chen
- Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou, China
- Key Laboratory of Heavy Ion Radiation Biology and Medicine of Chinese Academy of Sciences, Lanzhou, China
- Key Laboratory of Basic Research on Heavy Ion Radiation Application in Medicine, Gansu Province, Lanzhou, China
| | - Qiang Li
- Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou, China
- Key Laboratory of Heavy Ion Radiation Biology and Medicine of Chinese Academy of Sciences, Lanzhou, China
- Key Laboratory of Basic Research on Heavy Ion Radiation Application in Medicine, Gansu Province, Lanzhou, China
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Brown R, Corde S, Oktaria S, Konstantinov K, Rosenfeld A, Lerch M, Tehei M. Nanostructures, concentrations and energies: an ideal equation to extend therapeutic efficiency on radioresistant 9L tumor cells using ${{\rm{Ta}}}_{2}{{\rm{O}}}_{5}$ ceramic nanostructured particles. Biomed Phys Eng Express 2017. [DOI: 10.1088/2057-1976/aa56f2] [Citation(s) in RCA: 6] [Impact Index Per Article: 0.8] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/11/2022]
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Brown JMC, Currell FJ. A local effect model-based interpolation framework for experimental nanoparticle radiosensitisation data. Cancer Nanotechnol 2017; 8:1. [PMID: 28217175 PMCID: PMC5285431 DOI: 10.1186/s12645-016-0025-6] [Citation(s) in RCA: 17] [Impact Index Per Article: 2.1] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 11/15/2016] [Accepted: 12/20/2016] [Indexed: 01/23/2023] Open
Abstract
A local effect model (LEM)-based framework capable of interpolating nanoparticle-enhanced photon-irradiated clonogenic cell survival fraction measurements as a function of nanoparticle concentration was developed and experimentally benchmarked for gold nanoparticle (AuNP)-doped bovine aortic endothelial cells (BAECs) under superficial kilovoltage X-ray irradiation. For three different superficial kilovoltage X-ray spectra, the BAEC survival fraction response was predicted for two different AuNP concentrations and compared to experimental data. The ability of the developed framework to predict the cell survival fraction trends is analysed and discussed. This developed framework is intended to fill in the existing gaps of individual cell line response as a function of NP concentration under photon irradiation and assist the scientific community in planning future pre-clinical trials of high Z nanoparticle-enhanced photon radiotherapy.
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Affiliation(s)
- Jeremy M C Brown
- School of Mathematics and Physics, Queen's University Belfast, Belfast, Northern Ireland, UK
| | - Fred J Currell
- School of Mathematics and Physics, Queen's University Belfast, Belfast, Northern Ireland, UK
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Optimizing dose enhancement with Ta 2O 5 nanoparticles for synchrotron microbeam activated radiation therapy. Phys Med 2016; 32:1852-1861. [PMID: 27866898 DOI: 10.1016/j.ejmp.2016.10.024] [Citation(s) in RCA: 18] [Impact Index Per Article: 2.0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Journal Information] [Submit a Manuscript] [Subscribe] [Scholar Register] [Received: 07/22/2016] [Revised: 10/31/2016] [Accepted: 10/31/2016] [Indexed: 11/22/2022] Open
Abstract
Microbeam Radiation Therapy (MRT) exploits tumour selectivity and normal tissue sparing with spatially fractionated kilovoltage X-ray microbeams through the dose volume effect. Experimental measurements with Ta2O5 nanoparticles (NPs) in 9L gliosarcoma treated with MRT at the Australian Synchrotron, increased the treatment efficiency. Ta2O5 NPs were observed to form shells around cell nuclei which may be the reason for their efficiency in MRT. In this article, our experimental observation of NP shell formation is the basis of a Geant4 radiation transport study to characterise dose enhancement by Ta2O5 NPs in MRT. Our study showed that NP shells enhance the physical dose depending microbeam energy and their location relative to a single microbeam. For monochromatic microbeam energies below ∼70keV, NP shells show highly localised dose enhancement due to the short range of associated secondary electrons. Low microbeam energies indicate better targeted treatment by allowing higher microbeam doses to be administered to tumours and better exploit the spatial fractionation related selectivity observed with MRT. For microbeam energies above ∼100keV, NP shells extend the physical dose enhancement due to longer-range secondary electrons. Again, with NPs selectively internalised, the local effectiveness of MRT is expected to increase in the tumour. Dose enhancement produced by the shell aggregate varied more significantly in the cell population, depending on its location, when compared to a homogeneous NP distribution. These combined simulation and experimental data provide first evidence for optimising MRT through the incorporation of newly observed Ta2O5 NP distributions within 9L cancer cells.
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