ABSTRACT
PURPOSE: DNA single strand breaks (SSB) and double-strand breaks (DSB) induced by Auger electrons from incorporated (125)I decay were calculated using a B-DNA model to assess contributions from direct and OH damage and effects of higher-order structure. Three decay sites, linker DNA, nucleosome, and two adjacent nucleosomes, were assessed and compared to experimental data. METHOD: A Monte Carlo track structure code for electron was used to track electrons, OH and H radicals through linear and a higher-order model of B-DNA. Direct and indirect DNA hits were scored and used to determine SSB and DSB. RESULTS: The three different (125)I decay locations produced different number of DSBs and fraction of radical damage. The average number of DSB per (125)I decay was 0.83, 0.86 and 1.33, respectively, for the three sites. OH radical attack contributed to or exclusively caused 70%, 57%, and 50%, of the DSBs located in the entire model. When only 10 base pairs on either side of the incorporation site were considered, radical damage contributions were 40%, 25% and 67%, respectively. Locations distant from the site of incorporation, however, consistently yielded 70-80% of the DSB from radical attack. CONCLUSIONS: Coiling of DNA can greatly change both the absolute number of DSB per incorporated (125)I decay and the relative contributions of radical damage to the local site of decay and, to a lesser extent, the average over all DNA. Higher order structure only slightly affects the number and quality of DNA damage to distant locations, which is mostly from radical attack.
Subject(s)
DNA Breaks, Double-Stranded/radiation effects , DNA Breaks, Single-Stranded/radiation effects , DNA/radiation effects , Iodine Radioisotopes/chemistry , Computer Simulation , DNA/chemistry , Electrons , Hydroxyl Radical/chemistry , Models, Molecular , Monte Carlo Method , Nucleic Acid Conformation , RadioactivityABSTRACT
PURPOSE: To calculate the number of 157Gadolinium (157Gd) neutron capture induced DNA double strand breaks (DSB) in tumor cells resulting from epithermal neutron irradiation of a human head when the peak tissue dose is 10 Gy. To assess the lethality of these Gd induced DSB. MATRIALS AND METHODS: DNA single and double strand breaks from Auger electrons emitted during 157Gd(n,gamma) events were calculated using an atomistic model of B-DNA with higher-order structure. When combined with gadolinium neutron capture reaction rates and neutron and photon physical dose rates calculated from the radiation transport through a model of the human head with explicit tumors, peak tissue dose can be related to the number of Auger electron induced DSB in tumor cell DNA. The lethality of these DNA DSB were assessed through a comparison with incorporated 125I decay cell survival curves and second comparison with the number of DSB resulting from neutron and photon interactions. RESULTS: These calculations on a molecular scale (microscopic calculations) indicate that for incorporated 157Gd, each neutron capture reaction results in an average of 1.56 +/- 0.16 DNA single strand breaks (SSB) and 0.21 +/- 0.04 DBS in the immediate vicinity (approximately 40 nm) of the neutron capture. In an example case of Gd Neutron Capture Therapy (GdNCT), a 1 cm radius midline tumor, peak normal tissue dose of 10 Gy, and a tumor concentration of 1000 ppm Gd, result in a maximum of 140 +/- 27 DSBs per tumor cell. CONCLUSIONS: The number of DSB from the background radiation components is one order of magnitude lower than the Gd Auger electron induced DSB. The cell survival of mammalian cell lines with a similar amount of complex DSB induced from incorporated 125I decay yield one to two magnitudes of cell killing. These two points indicate that gadolinium auger electrons could significantly contribute to cell killing in GdNCT.
