JAEA-Review-2010-065.pdf:15.99MB - 日本原子力研究開発機構
JAEA-Review-2010-065.pdf:15.99MB - 日本原子力研究開発機構
JAEA-Review-2010-065.pdf:15.99MB - 日本原子力研究開発機構
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3-23<br />
Molecular Analysis of Carbon Ion Induced Mutations in<br />
Yeast Saccharomyces cerevisiae Cells<br />
K. Shimizu a) , Y. Matuo a, b) , Y. Izumi b) , Y. Hase c) , S. Nozawa c) ,<br />
A. N. Sakamoto c) and I. Narumi c)<br />
a) Radioisotope Research Center, Osaka University, b) Research Institute of Nuclear Engineering,<br />
University of Fukui, c) Radiation-Applied Biology Division, QuBS, <strong>JAEA</strong><br />
1. Introduction<br />
This study is intended to elucidate the molecular<br />
mechanism of the mutagenesis caused by ion beam<br />
irradiation. Ion beam irradiation is expected to increase<br />
mutation frequency and spectrum, since it has a high linear<br />
energy transfer (LET). However, the detailed molecular<br />
mechanism of its action has not been proven.<br />
Recently, we reported that the main mutations induced by<br />
high-LET carbon-ion irradiation were GC to TA<br />
transversions 1) . DNA adducts such as 8-oxodG, which are<br />
produced by interactions of reactive oxygen species (ROS)<br />
with these molecules, can create various pairing formations<br />
in DNA molecules, for example, pairing with dA in the syn<br />
conformation to produce a GC to TA mutation 2) . In this<br />
study, we used the yeast mutant strains ogg1 and msh2,<br />
which are deficient in mismatch repair mechanisms.<br />
Mutations involving 8-oxodGs were caused by ion beam<br />
irradiation in the ogg1 and msh2 mutant strains.<br />
2. Materials and methods<br />
2.1. Yeast strains<br />
S. cerevisiae haploid strains used in this study were S288c<br />
(MATα, RAD), rad52 (MATα, G160/2b), ogg1 (MATα,<br />
OGG1) and msh2 (MATα, msh2).<br />
2.2. Irradiation methods<br />
To determine the biological effectiveness of high LET<br />
ion beam irradiation, yeast cells were exposed to heavy ions<br />
accelerated at the AVF cyclotron (TIARA; <strong>JAEA</strong> Takasaki,<br />
Takasaki, Japan).<br />
As for the physical properties of the carbon ions, the<br />
<strong>JAEA</strong>-<strong>Review</strong> <strong>2010</strong>-065<br />
mean LET in the yeast was estimated to be 107 keV/μm<br />
water equivalent. This LET value was calculated by means<br />
of the ELOSS code program, which uses the elementary<br />
composition and the density of the target to calculate the<br />
energy loss of ion particles.<br />
3. Results and Discussion<br />
One of the most common consequences of ROS exposure<br />
is the incorporation of oxidized nucleotides such as 8-oxodG<br />
into the genome. Mismatch repair has been shown to<br />
repair oxidative damage by lowering the level of 8-oxodG<br />
that is incorporated into the genome, presumably by<br />
recognizing mismatches different from those recognized by<br />
base excision repair.<br />
The distribution of the mutations induced by carbon ion<br />
beam irradiation is shown in Fig. 1. In the ogg1 mutant<br />
strain, there were minor hot spots at positions 330, 515, 602,<br />
and 745 (Fig. 1 (C)). The mutations in msh2 mutant were<br />
distributed evenly for base substitution, except for a minor<br />
hot spot at position 345. These results suggest that the<br />
incorporation of damaged nucleotides was not uniform.<br />
In comparison with the surrounding sequence context of<br />
mutational base sites, the C residues in the 5’- (A/T) C (A/T)<br />
-3’ sequence were found to be easily mutated (data not<br />
shown). These observations are in agreement with results<br />
obtained in wild type cells.<br />
References<br />
1) Y. Matuo et al., Mutat. Res. 602 (2006) 7.<br />
2) M. Inoue et al., J. Biol. Chem. 273 (1998) 11069.<br />
Fig. 1 The mutation spectra induced by carbon ion beam irradiation of yeast. White triangles: base substitute<br />
mutations, inverted black triangles: deletion/insertions. (A) nucleotide position number of URA3 gene; (B)<br />
mutation spectrum of wild type; (C) ogg1; (D) msh2.<br />
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