Existence of Collective-excitation Energy Losses from an Electron Beam passing through Biological Materials

Regular threshold-energy increase with charge for neutral-particle emission in collisions of electrons with oligonucleotide anions

Electron-DNA anion collisions were studied using an electrostatic storage ring with a merging electron-beam technique. The rate of neutral particles emitted in collisions started to increase from definite threshold energies, which increased regularly with ion charges in steps of about 10 eV. These threshold energies were almost independent of the length and sequence of DNA, but depended strongly on the ion charges. Neutral particles came from breaks of DNAs, rather than electron detachment. The step of the threshold energy increase approximately agreed with the plasmon excitation energy. It is deduced that plasmon excitation is closely related to the reaction mechanism.

Action spectra for single- and double-strand break induction in plasmid DNA: studies using synchrotron radiation

Ionizing radiations deposit a wide range of energies in and around DNA and this leads to a corresponding spectrum of complexity of the lesions induced. The relationships between the amount of energy deposited and the yields and types of damage induced are important in modelling the physical and chemical stages of radiation effect and linking them to biological outcome. To study these relationships experimentally, plasmids were mounted as a monolayer and exposed in vacuum to near-monoenergetic photons from the Daresbury Synchrotron. After irradiation, the DNA was washed off and assayed for single-(ssb) and double-strand breaks (dsb) using agarose gel electrophoresis. Dose-effect relationships for ssb and dsb induction were obtained at various energies in the range 8-25 eV. The initial responses in the low-dose region allowed damage yields to be estimated. However, a common feature is that the responses showed energy-dependent plateaus at higher doses as if a fraction of the DNA were shielded. Various measures were taken both to minimize and to correct for this effect. The data appear to show that the yields of ssb and dsb increase only slowly with photon energies > 10 eV, with a suggestion of similar threshold energies for both lesions. In the energy range covered, the yield of ssb is 12-20-fold greater than that of dsb. The data indicate that ssb and dsb may have a common precursor in this system. Earlier work with low-energy electrons showed that at 25 eV ssb were induced but no dsb were detected.

Measurement of DNA damage by electrons with energies between 25 and 4000 eV

All ionizing radiations deposit energy stochastically along their tracks. The resulting distribution of energies deposited in a small target such as the DNA helix leads to a corresponding spectrum in the severity of damage produced. So far, most information about the probable spectra of DNA lesion complexity has come from Monte Carlo studies which endeavour to model the relationship between the energy deposited in DNA and the damage induced. The aim of this paper is to establish methods of determining this relationship by irradiating pBR322 plasmid DNA using low energy electrons with energies comparable with the minimum energy thought to produce critical damage. The technique of agarose gel electrophoresis has been used to ascertain the fraction of DNA single- and double-strand breaks induced by monoenergetic electrons with energies as low as 25 eV. Our data show that the threshold electron energy for induction of single-strand breaks is < 25 eV, and for double-strand breaks between 25 and 50 eV.

Energy requirements for damaging DNA molecules. III. The mechanisms of inactivation of bacteriophage chiX 174 DNA by vacuum ultra-violet radiation

Strand break formation and biological inactivation of infectious DNA of bacteriophage phi chi 174 exposed to vacuum-ultra-violet radiation of 4-9 to 21-2 eV quantum energy is investigated. At 21-2 eV as many as 84 per cent of the DNA molecules are inactivated by breaks whereas breaks do not contribute to inactivation at 4-9 eV. The quantum yield of break formation increases from 1-7 X 10(-5) (4-9 EV) to 0-55 (21-2 eV) and shows a dependence on energy similar to that of electron emission (due to ionization) above 8 eV. The mechanisms leading to break formation and inactivation are discussed taking the absorption spectrum of DNA in the vacuum-ultra-violet region into consideration.