Mario Pietro Carante
University of Pavia
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Featured researches published by Mario Pietro Carante.
Frontiers in Oncology | 2016
Mario Pietro Carante; F. Ballarini
A biophysical model of radiation-induced cell death and chromosome aberrations [called BIophysical ANalysis of Cell death and chromosome Aberrations (BIANCA)] was further developed and applied to therapeutic protons. The model assumes a pivotal role of DNA cluster damage, which can lead to clonogenic cell death following three main steps: (i) a DNA “cluster lesion” (CL) produces two independent chromosome fragments; (ii) fragment mis-rejoining within a threshold distance d gives rise to chromosome aberrations; (iii) certain aberration types (dicentrics, rings, and large deletions) lead to clonogenic inactivation. The yield of CLs and the probability, f, that a chromosome fragment remains un-rejoined even if other fragment(s) are present within d, were adjustable parameters. The model, implemented as a MC code providing simulated dose–responses directly comparable with experimental data, was applied to pristine and modulated Bragg peaks of the proton beam used to treat eye melanoma at INFN-LNS in Catania, Italy. Experimental survival curves for AG01522 cells exposed to the Catania beam were reproduced, supporting the model assumptions. Furthermore, cell death and chromosome aberrations at different depths along a spread-out Bragg peak (SOBP) dose profile were predicted. Both endpoints showed an increase along the plateau, and high levels of damage were found also beyond the distal dose fall-off, due to low-energy protons. Cell death and chromosome aberrations were also predicted for V79 cells, in the same irradiation scenario as that used for AG01522 cells. In line with other studies, this work indicated that assuming a constant relative biological effectiveness (RBE) along a proton SOBP may be sub-optimal. Furthermore, it provided qualitative and quantitative evaluations of the dependence of the beam effectiveness on the considered endpoint and dose. More generally, this work represents an example of therapeutic beam characterization avoiding the use of experimental RBE values, which can be source of uncertainties.
Radiation Research | 2018
Antonella Testa; F. Ballarini; Ulrich Giesen; Octávia Monteiro Gil; Mario Pietro Carante; John J. Tello; Frank Langner; Hans Rabus; Valentina Palma; Massimo Pinto; Clarice Patrono
There is a continued need for further clarification of various aspects of radiation-induced chromosomal aberration, including its correlation with radiation track structure. As part of the EMRP joint research project, Biologically Weighted Quantities in Radiotherapy (BioQuaRT), we performed experimental and theoretical analyses on chromosomal aberrations in Chinese hamster ovary cells (CHO-K1) exposed to α particles with final energies of 5.5 and 17.8 MeV (absorbed doses: ∼2.3 Gy and ∼1.9 Gy, respectively), which were generated by the microbeam at the Physikalisch-Technische Bundesanstalt (PTB) in Braunschweig, Germany. In line with the differences in linear energy transfer (approximately 85 keV/μm for 5.5 MeV and 36 keV/μm for 17.8 MeV α particles), the 5.5 MeV α particles were more effective than the 17.8 MeV α particles, both in terms of the percentage of aberrant cells (57% vs. 33%) and aberration frequency. The yield of total aberrations increased by a factor of ∼2, although the increase in dicentrics plus centric rings was less pronounced than in acentric fragments. The experimental data were compared with Monte Carlo simulations based on the BIophysical ANalysis of Cell death and chromosomal Aberrations model (BIANCA). This comparison allowed interpretation of the results in terms of critical DNA damage [cluster lesions (CLs)]. More specifically, the higher aberration yields observed for the 5.5 MeV α particles were explained by taking into account that, although the nucleus was traversed by fewer particles (nominally, 11 vs. 25), each particle was much more effective (by a factor of ∼3) at inducing CLs. This led to an increased yield of CLs per cell (by a factor of ∼1.4), consistent with the increased yield of total aberrations observed in the experiments.
Radiation and Environmental Biophysics | 2014
F. Ballarini; S. Altieri; Silva Bortolussi; Mario Pietro Carante; Elio Giroletti; Nicoletta Protti
Radiation and Environmental Biophysics | 2015
Mario Pietro Carante; S. Altieri; Silva Bortolussi; Ian Postuma; Nicoletta Protti; F. Ballarini
Radiation Physics and Chemistry | 2016
F. Ballarini; Mario Pietro Carante
Radiation Protection Dosimetry | 2015
F. Ballarini; S. Altieri; Silva Bortolussi; Mario Pietro Carante; Elio Giroletti; Nicoletta Protti
biophysics 2017, Vol. 4, Pages 465-490 | 2017
Mario Pietro Carante; F. Ballarini
DNA Repair | 2017
John James Tello Cajiao; Mario Pietro Carante; Mario Antonio Bernal Rodriguez; F. Ballarini
DNA Repair | 2018
John James Tello Cajiao; Mario Pietro Carante; Mario Antonio Bernal Rodriguez; F. Ballarini
Physics in Medicine and Biology | 2018
Mario Pietro Carante; Chiara Aimè; John James Tello Cajiao; F. Ballarini