R. Sabattier

DNA Radiolysis by Fast Neutrons

The effects of fast neutron irradiation on DNA were studied using DNA of the pBR322 plasmid (4362 base pairs), and the results compared to those obtained with 60Co gamma rays. Irradiation of the plasmid DNA in solution with a neutrons beam (p34+Be) of the CERI (CNRS Orléans) cyclotron (with a flat energy spectrum from 34 MeV to low energies) results in half the yield of single-strand breaks (ssb), and 1.5 times higher yield of double-strand breaks (dsb) for neutrons as compared to gamma-rays. Possible specificity of the neutron-induced breaks was examined: the scavenging of OH. radicals by 0.1 mol dm-3 ethanol inhibits all neutron-induced ssb, but only 85 per cent of the dsb. For gamma-irradiation, both ssb and dsb are completely inhibited in these conditions. These results suggest at least three different origins for neutron-induced dsb. The occurrence of around 30 per cent of dsb can be explained by a radical transfer mechanism (proposed by Siddiqi and Bothe (1987) for gamma-irradiation). Around 55 per cent of dsb may be due to the non-random distribution of radicals in high-density tracks of the secondary particles of neutrons, which results in a simultaneous attack of the two strands by OH. radicals. These first two processes are both OH.-mediated and thus are sensitive to ethanol. The direct effect of fast neutrons and their secondaries (recoil protons, alpha-particles and recoil nuclei) can account for the remaining 15 per cent of dsb, not inhibited by 0.1 mol dm-3 ethanol.

Radioprotection of DNA by Polyamines

Putrescine, spermidine and spermine are natural polyamines bearing at neutral pH the net electrical charges +2, +3 and +4 respectively. We report here the radioprotective effect of these polyamines on the radiolysis of pBR322 plasmid DNA. We observe a very efficient protection against fast neutron-induced single and double-strand breakage in the presence of spermine and spermidine, and a significantly less efficient protection in the presence of putrescine. An ionic strength dependence is observed for spermidine and spermine, but not for putrescine. Circular dichroism measurements show spermidine- and spermine-induced structural modifications of DNA, i.e. the formation of tightly packaged condensates in the concentration range corresponding to radioprotection. No structural change is observed for concentrations of putrescine affording radioprotection. We explain the radioprotection by: (1) the scavenging of OH radicals in the bulk, essentially observed in the case of putrescine; (2) a local scavenging at the sites of binding of polyamines; and (3) the reduced accessibility of the attack sites in the condensed structures induced by spermine or spermidine.

Metal Ions Protect DNA Against Strand Breakage Induced by Fast Neutrons

Single and double strand breaks (SSB and DSB) are induced by fast neutrons in plasmid (pBR322) DNA in 1 mM potassium phosphate buffer (pH 7.25). Increasing the concentration of monovalent (Na+, Cs+, Li+), divalent (Mg2+, Ca2+) and trivalent (Al3+, Co3+ (NH3)6) metal cations strongly decreases the yield of DSB. The extent of the observed protection depends on the valence of the cation. The production of SSB is only slightly decreased, except for Al3+ and Co3+ (NH3)6, whose effects are particularly large (complete protection at 1 and 0.1 mM respectively). Circular dichroism spectra show that Al3+ induces an important structural change of DNA at the ion concentration where the protection becomes total. This change is probably a condensation (collapse), as in the well-known case of Co3+ (NH3)6. Our results suggest two mechanisms of protection by metal ions: (i) the induction of structural changes of DNA, that render less accessible the critical sites of attack by OH. radicals; and (ii) the stabilization of the double helical regions between two close-set nicks on opposite strands, that hinders the effective double strand breakage of DNA.

Radioprotection of DNA by a DNA-binding protein : MC1 chromosomal protein from the archaebacterium Methanosarcina sp. CHTI55

The archaebacterial chromosomal protein MC1 binds tightly and unspecifically to DNA; binding protects DNA against radiolysis by fast neutrons. At low covering of pBR322 plasmid DNA, one bound protein protects some 50 attack sites (phosphate-sugar moieties) against both single (ssb) and double strand breaks (dsb). At high covering of plasmid, protection against dsb becomes almost complete, although about half of the attack sites remain accessible to ssb. DNA restriction fragments were used to investigate the organization of the complexes, and its consequences on DNA radiolysis. Sequencing gel electrophoresis of the radiolytically-broken fragments are almost regular in the absence of protein, showing that breakage occurs at every base. In the presence of the protein, a periodic protection pattern is observed. The period of 11 base pairs is interpreted as the minimum distance between two adjacent MC1 proteins.

Combined use of FLUKA and MCNP-4A for the Monte Carlo simulation of the dosimetry of 10B neutron capture enhancement of fast neutron irradiations

Boron neutron capture enhancement (BNCE) of the fast neutron irradiations use thermal neutrons produced in depth of the tissues to generate neutron capture reactions on 10B within tumor cells. The dose enhancement is correlated to the 10B concentration and to thermal neutron flux measured in the depth of the tissues, and in this paper we demonstrate the feasibility of Monte Carlo simulation to study the dosimetry of BNCE. The charged particle FLUKA code has been used to calculate the primary neutron yield from the beryllium target, while MCNP-4A has been used for the transport of these neutrons in the geometry of the Biomedical Cyclotron of Nice. The fast neutron spectrum and dose deposition, the thermal flux and thermal neutron spectrum in depth of a Plexiglas phantom has been calculated. The thermal neutron flux has been compared with experimental results determined with calibrated thermoluminescent dosimeters (TLD-600 and TLD-700, respectively, doped with 6Li or 7Li). The theoretical results were in good agreement with the experimental results: the thermal neutron flux was calculated at 10.3 X 10(6) n/cm2 s1 and measured at 9.42 X 10(6) n/cm2 s1 at 4 cm depth of the phantom and with a 10 cm X 10 cm irradiation field. For fast neutron dose deposition the calculated and experimental curves have the same slope but different shape: only the experimental curve shows a maximum at 2.27 cm depth corresponding to the build-up. The difference is due to the Monte Carlo simulation which does not follow the secondary particles. Finally, a dose enhancement of, respectively, 4.6% and 10.4% are found for 10 cm X 10 cm or 20 cm X 20 cm fields, provided that 100 micrograms/g of 10B is loaded in the tissues. It is anticipated that this calculation method may be used to improve BNCE of fast neutron irradiations through collimation modifications.

Beam collimation and bolusing material optimizations for 10boron neutron capture enhancement of fast neutron (BNCEFN): definition of the optimum irradiation technique.

PURPOSE In boron-10 neutron capture enhancement of fast neutron irradiation (BNCEFN), the dose enhancement is correlated to the 10B concentration and thermal neutron flux. A new irradiation technique is presented to optimize the thermal neutron flux. METHODS AND MATERIALS The coupled FLUKA and MCNP-4A Monte Carlo codes were used to simulate the neutron production and transport for the Nice and Orleans facilities. RESULTS The new irradiation technique consists of a 20-cm lead blocks additional collimator, placed close to the patients head, which is embedded in a pure graphite cube. A 24-fold thermal neutron flux increase is calculated between a 5 x 5 cm2 primary collimated field, with the patients head in the air, and the same field size irradiated with the optimum irradiation technique. This increase is more important for the p(60)+Be Nice beam than for the p(34)+Be Orleans one. The thermal neutron flux is 2.1 x 10(10) n(th)/Gy for each facility. Assuming a 100 microg/g 10B concentration, a physical dose enhancement of 22% is calculated. Moreover, the thermal neutron flux becomes independent of the field size and the phantom head size. CONCLUSION This technique allows conformal irradiation of the tumor bed, while the thermal neutron flux is enhanced, and spreads far around the tumor.

Direct Effect in DNA Radiolysis. Boron Neutron Capture Enhancement of Radiolysis in a Medical Fast-Neutron Beam

Abstract Sèche, E., Sabattier, R., Bajard, J-C., Blondiaux, G., Breteau, N., Spotheim-Maurizot, M. and Charlier, M. Direct Effect in DNA Radiolysis. Boron Neutron Capture Enhancement of Radiolysis in a Medical Fast-Neutron Beam. Radiat. Res. 158, 292–301 (2002). This paper is devoted to the study of the molecular basis of the boron neutron capture enhancement of fast-neutron radiotherapy. Plasmid DNA was irradiated with a medical fast-neutron beam in the presence of either 10B or 11B. The number of induced SSBs and DSBs was much higher in samples containing 10B compared to 11B. The additional breaks are attributed to the nuclear reaction 10B(n, α)7Li induced by the capture by 10B of thermal neutrons produced in the medium by scattering and slowing down of neutrons. Irradiation in the presence of DMSO (OH radical scavenger) allows the number of nonscavengeable breaks to be determined. The ratio DSB/SSB is within the range of those observed with heavy ions, in good agreement with the hypothesis that the additional breaks are due to α particles and recoil lithium nuclei. The simulation of the energy deposition along the paths of the α and 7Li particles allows the calculation of core and penumbra track volumes. Further, the number of plasmids encountered by the core and the penumbra was evaluated. Their number was compared to the nonscavengeable additional breaks. Since the two sets of values are of the same order of magnitude, we conclude that the nonscavengeable additional SSBs and DSBs could be due to direct effects.

Radiosensitivity of DNA minicircles

DNA minicircles of 207 bp were constructed by the ligation of linear restriction fragments in the presence of various concentrations of ethidium bromide. Three topoisomers characterized by linking numbers (Lk) of 20, 19 and 18, and with helical repeats of 10.35, 10.9 and 11.5 bp/turn respectively, were obtained. They are called, respectively, relaxed minicircle or topoisomer 0, topoisomer -1 and topoisomer -2. Owing to the limited flexibility of such small circles, the stress created by the lack of 1 or 2 turns cannot be eliminated by a spatial circle-axis writhing (supercoiling) of the circular molecules. These two undertwisted, stressed topoisomers have to adopt a flat, non-crossed shape, similar to that of the relaxed minicircle. The three minicircles were irradiated with gamma-rays or fast neutrons. The same yields of single-strand breaks, double-strand breaks and alkali-induced single-strand breaks were observed for the three topoisomers showing that their base and sugar moieties are attacked equally by gamma photon- or fast neutron-induced radicals. We conclude that untwisting of a B helix does not modify the radiosensitivity of DNA.

Comparative study of DNA radiolysis by fast neutrons and γ-rays

The effect of fast neutrons on cells is different from that of gamma-rays: the relative (to gamma) biological effect (RBE) is higher than one and the oxygen enhancement ratio (OER) is lower than that of gamma-rays. We searched for differences between the effects of the two radiations on DNA, the critical target of radiations. Using a model plasmid DNA we observed that for the same absorbed dose, fast neutrons induce twice fewer single strand breaks (SSB) and 1.5 more double strand breaks (DSB) than gamma-rays. A transition metal ion, the Cu++, is a better sensitizer of DNA breakage with fast neutrons than with gamma-rays. In anoxia, cysteamine, a positively charged thiol, is a better radioprotector against neutrons than against gamma-rays. In presence of cysteamine, the OER is lower for neutrons than for gamma-rays. These results are discussed in terms of different physical properties of the two types of radiation.

Unusual Alkaline Elution Pattern Induced in Mammalian Cell DNA by Fast Neutrons p(34) + Be

Syrian hamster fibroblasts (cell line BHK 21/13) were exposed to p(34) + Be fast neutron irradiation and their DNA analysed by the alkaline elution technique. The elution profiles showed an unusual tailing off, characteristic of neutron-irradiated samples, suggesting the presence of a modification in DNA induced by the neutrons. This was not seen with 60Co gamma-irradiation. In neutron-irradiated samples the alteration of DNA appeared to persist even after 2 h of post-treatment incubation (37 degrees C) indicating the absence of repair. The modification of DNA induced by neutrons provides a possible explanation for the reduction of the shoulders in survival curves obtained with neutrons, and the high RBE of neutrons.