Research Center for Charged Particle Therapy, National Institute of Radiological Sciences, Chiba 263-8555, Japan.
Mutat Res. 2013 Aug 30;756(1-2):101-7. doi: 10.1016/j.mrgentox.2013.05.005. Epub 2013 May 17.
We have studied the induction of chromosome aberrations in human fibroblasts exposed in G0/G1 to X-rays or heavy ions to study the influence of G1 cell cycle arrest. Confluent normal fibroblasts were exposed to X-rays or accelerated particles with different LET values and chromosome aberrations were investigated in the first G0/G1 and G2//M phase. The particles used here were 490MeV/nucleon Si, 500MeV/nucleon Fe, and 200MeV/nucleon Fe ions. Cells were subcultured 24h after exposure and premature chromosome condensation (PCC) was performed by fusion-induced method for analysis of G0/G1 cells, and chemically-induced method for analysis of G2 and metaphase cells. Chromosome damage was assessed in chromosomes 1 and 3 using whole chromosome fluorescence in situ hybridization (FISH). Cell cycle was analyzed by flow cytometry at different incubation times following subculture. After irradiation with 2Gy of high-LET particles, the yields of chromosome aberrations and fragments were significantly higher in G0/G1 phase than in G2/M phase, whereas similar yields of damage were measured in both phases after exposure to X-rays. In contrast, the yield of misrepair, assessed by the number of color junctions, was similar in the G0/G1 and G2/M phases after exposure to either X-rays or high-LET particles. The yields of chromosome aberrations, fragments, and color junctions in both the G0/G1 and the G2/M phases, increased with LET up to 200keV/μm, then decreased for 440keV/μm Fe particles. A good correlation was found between chromosome aberrations in both G0/G1 and G2/M cells and survival fractions after 2Gy of different LET radiations, although the slopes were steeper for the G0/G1 cells. Flow cytometry analysis indicated that high-LET particles induce more non cycling G0/G1 cells within 48h of subculture than X-rays, suggesting that chromosome aberrations scored at the G2/M phase may not accurately describe the true radiation effect.
我们研究了人类成纤维细胞在 G0/G1 期受到 X 射线或重离子照射后染色体畸变的诱导,以研究 G1 细胞周期阻滞的影响。将汇合的正常成纤维细胞暴露于不同 LET 值的 X 射线或加速粒子下,并在第一次 G0/G1 和 G2//M 期研究染色体畸变。这里使用的粒子是 490MeV/nucleon Si、500MeV/nucleon Fe 和 200MeV/nucleon Fe 离子。暴露后 24 小时进行细胞传代培养,并通过融合诱导法进行 PCC(早熟染色体凝聚)分析 G0/G1 细胞,通过化学诱导法分析 G2 和中期细胞。使用整条染色体荧光原位杂交(FISH)分析 1 号和 3 号染色体的染色体损伤。细胞传代培养后不同时间点通过流式细胞术分析细胞周期。用高 LET 粒子照射 2Gy 后,G0/G1 期染色体畸变和片段的产额明显高于 G2/M 期,而用 X 射线照射后,在两个时期测量到相似的损伤产额。相比之下,用 X 射线或高 LET 粒子照射后,G0/G1 和 G2/M 期的错误修复产额(通过颜色连接数评估)相似。G0/G1 和 G2/M 期的染色体畸变、片段和颜色连接的产额随 LET 增加到 200keV/μm 而增加,然后在 440keV/μm Fe 粒子时减少。发现 2Gy 不同 LET 射线照射后,G0/G1 和 G2/M 细胞的染色体畸变与存活分数之间存在良好的相关性,尽管 G0/G1 细胞的斜率更陡。流式细胞术分析表明,高 LET 粒子在细胞传代培养后 48 小时内诱导更多的非循环 G0/G1 细胞,这表明在 G2/M 期计数的染色体畸变可能不能准确描述真实的辐射效应。