12C和X射线辐照人肺癌细胞H1299的生物学效应

用高传能线密度（LET）的12C离子束和低LET的X射线辐照体外培养的非小细胞肺癌H1299(p53基因缺失), 研究它们的辐照生物学效应的差异。 用克隆形成率法测定了细胞对射线的辐射敏感性; 用AnnexinV/PI试剂盒检测了细胞早期凋亡; 用流式细胞仪检测了细胞周期变化。 实验结果表明, 12C离子束辐照H1299细胞的存活率明显低于用X射线辐照的; 12C离子束引起H1299细胞的早期凋亡率明显高于X射线辐照引起的, 且持续时间更长; 12C离子束引起的H1299细胞G2/M期的抑制更明显。 说明H1299细胞对高LET的12C离子束的辐射敏感性高于对X射线的, 重离子对p53基因缺失型肿瘤的治疗可实施较低的照射剂量、 较少的照射次数和较长的时间间隔。     

^12C和X射线辐照人肺癌细胞H1299的生物学效应

用高传能线密度（LET）的^12C离子束和低LET的X射线辐照体外培养的非小细胞肺癌H1299（p53基因缺失）,研究它们的辐照生物学效应的差异。用克隆形成率法测定了细胞对射线的辐射敏感性;用AnnexinV/PI试剂盒检测了细胞早期凋亡;用流式细胞仪检测了细胞周期变化。实验结果表明,^12C离子束辐照H1299细胞的存活率明显低于用X射线辐照的;^12C离子束引起H1299细胞的早期凋亡率明显高于X射线辐照引起的,且持续时间更长;^12C离子束引起的H1299细胞G2/M期的抑制更明显。说明H1299细胞对高LET的^12C离子束的辐射敏感性高于对X射线的,重离子对p53基因缺失型肿瘤的治疗可实施较低的照射剂量、较少的照射次数和较长的时间间隔。     

~(12)C~(6+)离子束辐照紫苏干种子当代效应

利用兰州重离子研究装置(HIRFL)提供的12C6+离子束辐照紫苏干种子(辐照剂量为40,80和120Gy,剂量率4Gy/min),探讨了重离子束辐照对紫苏M1代的生物学效应。结果发现,经不同剂量的12C6+离子束辐照后,紫苏种子的发芽率、发芽势、存活率、株高、分枝数、单株产量和千粒重等生物学性状均发生了变化,其中发芽势、单株产量和千粒重随辐照剂量的提高而降低,且有明显的剂量效应关系,但发芽率、大田成活率、株高和分枝数却随辐照剂量的增大,呈现出明显的"抛物线"趋势;紫苏幼苗根尖细胞的微核率和染色体畸变率随辐照剂量增加呈线性增加关系。这表明:12C6+重离子束辐照紫苏种子,具有明显的当代损伤效应,在本试验剂量范围内,低剂量辐照对发芽率和成活率有促进作用。     

碳离子束混合LET辐照的EBT3辐射变色胶片剂量修正方法

针对EBT3辐射变色胶片对碳离子束混合LET辐照的剂量欠响应比较了两种剂量修正方法。利用260 MeV/u的碳离子束通过被动降能得到多种剂量平均LET的碳离子束,利用这些碳离子束进行了胶片剂量响应刻度辐照,选择最佳的拟合公式得到了胶片剂量刻度曲线。使用RE(Relative Efficiency)量化了EBT3胶片随LET的剂量欠响应,并使用RE剂量修正法修正了混合LET辐照胶片的剂量。此外,根据剂量刻度曲线公式中拟合参数随不同LET所占剂量比例的变化规律,提出了拟合参数剂量修正法并修正了混合LET辐照胶片的剂量。最后比较了这两种方法的结果,表明拟合参数方法得到的剂量偏差在5%以内,优于RE方法10%以内的剂量偏差。     

~(12)C~(6+)离子束与电子束辐照对薰衣草当代诱变效应的比较

采用100 MeV的~(12)C~(6+)离子束和1.2 MeV的电子束辐照薰衣草干种子,研究了2个品种的薰衣草干种子对不同辐射源的辐照生物学效应,以期找到薰衣草干种子的最佳诱变参数。结果表明:不论是薰衣草701还是702,经~(12)C~(6+)离子辐照后,其发芽率表现为先增大后减小的趋势;经电子束辐照后,发芽率随着剂量的升高而降低,电子束辐照后的发芽率要低于~(12)C~(6+)离子束。另外,2个品种的薰衣草经~(12)C~+离子辐照后,其胚轴胚根长度以及幼苗鲜重也较电子束辐照后的大。由此可知,重离子的辐照效果优于电子束的,有利于后期筛选出新的薰衣草突变株。     

不同辐照源对黑松花粉粒的生物学效应

研究了N+离子束、 紫外线和γ射线辐照对黑松花粉粒的影响, 对3种辐射源在诱发花粉粒细胞出现损伤效应上的差异性进行了比较分析。 研究结果表明, 3种辐照源对黑松花粉粒萌发和花粉管生长所表现出的效应存在明显的差异。 γ射线的剂量效应曲线表现为近S型; 紫外线辐照的剂量效应曲线呈现出近L型; 离子束的生物学效应主要在两个方面表现出特异性, 即离子束所导致的剂量 效应曲线呈“马鞍型”趋势和N+离子束注入后会诱发花粉管顶端产生出明显的肿胀现象。The effects of pollens and pollen tubes of Pinus thunbergii induced respectively by N+ beam, γ ray and ultraviolet ray were measured , and the differences of the effects caused by the different radiant factors were distinguished. The results showed that there was obvious difference in the damages of the pollen germination and the pollen tube growth led by the radiant factors. The curve of dose effects from γ ray irradiation was similarly S type, and that from ultraviolet ray treatment approximately L type . The effects from ion implantation expressed the two characteristics, the curve of the saddle type and the top inflation of pollen tube.     

65 nm互补金属氧化物半导体场效应和晶体管总剂量效应及损伤机制

对65 nm互补金属氧化物半导体工艺下不同尺寸的N型和P型金属氧化物半导体场效应晶体管(NMOSFET和PMOSFET)开展了不同偏置条件下电离总剂量辐照实验.结果表明:PMOSFET的电离辐射响应与器件结构和偏置条件均有很强的依赖性,而NMOSFET表现出较强的抗总剂量性能;在累积相同总剂量时,PMOSFET的辐照损伤远大于NMOSFET.结合理论分析和数值模拟给出了PMOSFET的辐射敏感位置及辐射损伤的物理机制.     

12C6+离子束辐照黄花蒿干种子当代生物学效应

利用12C6+重离子束对黄花蒿干种子辐照后,利用发芽率、根长、下胚轴长和株高4个指标研究不同剂量12C6+离子束辐照对黄花蒿的生物学效应。结果表明,随着辐照剂量的增加,黄花蒿的存活率和根长都呈现逐渐降低的趋势,而下胚轴长先上升后下降,株高总体呈现下降的趋势,但在60和90 Gy同时存在矮化与增高的植株。利用SRAP （sequence related amplified polymorphism）技术对辐照后M1代的黄花蒿植株进行研究,结果表明对照组和处理组之间的差异体现为特异性条带的变化。综合分析表明,12C6+的重离子辐照黄花蒿干种子可以产生显著的当代损伤效应,同时引起植物DNA的多态性变化。     

超深亚微米器件总剂量辐射效应三维数值模拟

本文分析了浅槽隔离(STI)结构辐射诱导电荷的分布情况,给出一种模拟超深亚微米器件总剂量辐射效应的新方法.研究结果表明,如果在栅附近沿着STI侧墙不加辐照缺陷,仿真出的0.18 μm超深亚微米晶体管亚阈区I-V特性没有反常的隆起,并且能够很好地反映试验结果.在研究总剂量辐照特性改善方面,在剂量不是很大的情况下,采用超陡倒掺杂相对于均匀掺杂能有效地减小辐照所引起的泄漏电流.如果采用峰值(Halo)掺杂,不仅有利于提高超深亚微米器件的抗辐照能力,而且在大剂量的情况下,可以得到明显的效果. 关键词： 总剂量 超陡倒掺杂 Halo掺杂 辐射效应     

碳离子束辐照对油葵当代结实特性的影响

利用兰州重离子研究装置(HIRFL)的碳离子束辐照油葵干种子,统计出苗率、存活率、花粉活力、柱头可授性和不同授粉条件下的结实率,研究碳离子束辐照对油葵当代结实特性的影响。结果表明,出苗率、存活率、花粉活力、结实率随着辐照剂量增加而降低;与对照相比,80 Gy辐照后出苗率下降55.68%、存活率下降64.66%;20～160 Gy辐照显著降低了自交结实率,40～160 Gy辐照显著降低了混交结实率;花粉活力由对照组的92.01%降低为160 Gy的47.59%;随着辐照剂量的增加,具有较强可授性柱头的百分比逐渐降低,具有较弱可授性柱头和不具可授性柱头的百分比逐渐增加。研究表明,碳离子束辐照对油葵当代的损伤作用,影响了花器官的育性,降低了结实率;根据存活率的半致死剂量,结合混交结实率的半不育剂量,确定油葵适宜辐照剂量范围55～153 Gy,为碳离子束辐照油葵育种选择适宜辐照剂量提供了参考。     

细胞松弛素B阻断微核法鉴定男性个体辐射敏感性的方法初探

初步研究了男性个体辐射敏感性的鉴定方法及标准。采集50名男性志愿者的外周血，分别给予不同剂量X射线照射，采用细胞松弛素B阻断双核法测定微核率(MNF)，通过二阶多项拟合法，绘制微核剂量效应选项中心标准曲线，将个人微核剂量效应曲线与标准曲线比对后判断个体辐射敏感性。 $0.0\sim2.5 $ Gy剂量范围内，剂量效应二阶多项拟合的中心方程为(MNF=0.014 7+0.036 2D+0.023 1D 2， r=0.726)。50名志愿者中，辐射敏感的有13人，辐射抗性的有14人，基本符合正态分布。Spearman秩和相关分析结果显示，MNF在各个辐射剂量点与辐射敏感性均存在正相关,与辐射抗性呈负相关,MNF随剂量增加而增加。本研究初步建立了“以线代点”男性个体辐射敏感性鉴定方法,并发现男性外周血淋巴细胞的本底微核率与个体辐射敏感性呈正相关。     

Investigation of metabolic changes in blood and tissue of mice γ-irradiated with sublethal doses by direct observation of EPR signals from Hb-NO complexes

The metabolic changes in probes of blood and tissue (spleen, liver and kidney) of mice under total γ-irradiation with the doses varied in the interval of 1–10 Gy at the dose rate of 0.073 Gy/min were studied in the early postirradiation period by ex vivo electron paramagnetic resonance (EPR). It was established that the impact with the lower dose rate leads to more intensive nitric monoxide biosynthesis in comparison with higher dose rates. In the early postirradiation period (from 2 up to 6 h), irradiation with doses higher than 2 Gy brings about an increase of the NO concentration and, hence, the appearance of nitrosyl complexes which were registered directly by EPR in blood and spleen. The observed line is identified as the signal from α-(Fe²⁺-NO)₂β(Fe³⁺)₂ or α-(Fe²⁺-NO) α(Fe²⁺)β(Fe³⁺)₂ complexes since the methemoglobin concentration also increases in comparison with the control level. The concentration of Hb-NO complexes in blood and spleen depends on the dose and individual radiosensitivity of the organism. Therefore, the intensity of the Hb-NO signal may serve as a criterion of the radiation injury level during the first hours after the irradiation. 30 h after the impact, the Hb-NO complexes were no longer detected. For the first day, the concentration of Fe³⁺-transferrin in blood increases with the dose and time passed after the irradiation. The intensity of the EPR signal from Fe³⁺-transferrin in blood may also serve as a measure of the radiation injury level.     

甲基化抑制剂5-氮杂2′-脱氧胞苷对三维培养A549细胞辐射敏感性的影响

为探讨DNA去甲基化试剂5-氮杂-2′-脱氧胞苷(5-aza-2′-deoxycytidine,5-Aza-CdR)对三维(3D)培养模式下的肺腺癌细胞A549辐射敏感性的作用,开展了系列实验。使用不同浓度5-Aza-CdR处理单层(2D)A549细胞72 h后,MTT法检测其对A549细胞的增殖抑制作用。选取低浓度(2,5μmol/L)5-Aza-CdR预处理2D和3D培养的A549细胞72 h,X射线分别辐照1,2,4,6 Gy,检测微核形成率和克隆存活。实验结果显示,不同浓度的5-Aza-CdR均能抑制2D的A549细胞增殖,且呈剂量依赖性。5μmol/L药物预处理2D与3D细胞并联合辐照后诱导的细胞微核形成率均显著高于相应的对照组,并且细胞存活率显著降低。不过,较低浓度5-Aza-CdR(2μmol/L)预处理的3D培养A549细胞4,6 Gy辐照后微核数目较未用药处理组显著增加,克隆存活率较未用药组显著降低(P0.05),而在2D培养A549细胞中未观测到上述现象。研究结果表明,5-Aza-CdR能抑制A549细胞增殖,3D培养A549细胞药物预处理更能增加其辐射敏感性。结果暗示,为减少对正常细胞的毒性作用,在临床放疗中,可低剂量使用5-Aza-CdR,实现肿瘤的有效靶向治疗。     

Absorbed dose measurements on LDEF and comparisons with predictions

The radiation environment on LDEF was monitored by cumulative absorbed dose measurements made with TLDs at different locations and shielding depths. The TLDs were included in four experiments: A0015(a) Biostack, P0004 Seeds in Space and P0006 Linear Energy Transfer Spectrum Measurements at the trailing edge (west side) of the satellite; M0004 Fiber Optics Data Link at the leading edge (east side); and A0015(b) Biostack at the Earth side. The shielding depths varied between 0.48 and 15.4 g/cm², Al equivalent. Both the directional dependence of trapped protons incident on the satellite and the shielding thickness were reflected in absorbed dose values.

The trapped proton anisotropy was measured by TLDs at the east and west sides of LDEF. At the east side doses ranged from 2.10 to 2.58 Gy under shielding of 2.90 to 1.37 g/cm² (M0004) while on the west side doses ranged from 2.66 to 6.48 Gy under shielding of 15.4 to 0.48 g/cm² (P0006). The west side doses were more than a factor of two higher, where the vertical shielding thicknesses to space were equal. Other west side doses of 3.04 to 4.49 Gy under shielding of 11.7 to 3.85 g/cm² (A0015(a)) and 2.91 to 6.64 Gy under shielding of 11.1 to 0.48 g/cm² (P0004) generally agreed with the P0006 results. The Earth side doses of 2.41 to 3.93 Gy under shielding of 10.0 to 1.66 g/cm² (A0015(b)) were intermediate between the east side and west side doses.

Calculations utilizing a model of trapped proton spectra were performed by Watts et al. (1993) and comparisons of dose measurement and calculations may be found in a companion paper (Armstrong et al., 1996).     

Radiosensitivity of CD3−CD8+CD56+ NK cells

The effect of lower doses (0.5–3.0 Gy) of gamma radiation on radiosensitivity of CD3?/CD8+ NK cells subpopulation isolated from the peripheral blood of healthy volunteers was studied 48 h after the irradiation. Only a subtle increase in terms of induction of apoptosis (A+ cells), was observed in Annexin positive CD3?/CD8+ NK cells. The assessment of the relative presence of CD3^?/CD8⁺ NK cells in Annexin negative populations of lymphocytes considerably contributes to the elimination of individual variability and could be useful in biodosimetry.Living CD3?/CD8+; Annexin negative NK cells were analyzed using five-color flow cytometry 16 h after irradiation by the doses of 1–10 Gy. The study was carried out on NK cells subsets CD3?/CD8? CD16+, CD56 (dim) and CD56 (bright). NK cells characterized with their low-density expression of CD56 (dim) are more cytotoxic and express CD16. Those with high-density expression of CD56 (bright) are known for their capacity to produce cytokines following activation of monocytes but their natural cytotoxicity is low; they are classified as CD16? or CD16 (dim). A dose-depending decrease in the relative presence of CD3?/CD8+ NK cells was observed 16 h after ionizing radiation (1–10 Gy). The decrease was highly pronounced in CD56 (bright) subset of NK cells and this subpopulation was considered as the most radiosensitive one. Unfortunately, the most radiosensitive subpopulation of NK cells – CD56bright cannot be used as a biodosimetric marker due to its insufficient amount in peripheral blood.     

Effects of gamma radiation on hard dental tissues of albino rats using scanning electron microscope – Part 1

In the present study, 40 adult male albino rats were used to study the effect of gamma radiation on the hard dental tissues (enamel surface, dentinal tubules and the cementum surface). The rats were irradiated at 0.2, 0.5, 1.0, 2.0, 4.0 and 6.0 Gy gamma doses. The effects of irradiated hard dental tissues samples were investigated using a scanning electron microscope. For doses up to 0.5 Gy, there was no evidence of the existence of cracks on the enamel surface. With 1 Gy irradiation dose, cracks were clearly observed with localized erosive areas. At 2 Gy irradiation dose, the enamel showed morphological alterations as disturbed prismatic and interprismatic areas. An increase in dentinal tubules diameter and a contemporary inter-tubular dentine volume decrease were observed with higher irradiation dose. Concerning cementum, low doses,<0.5 Gy, showed surface irregularities and with increase in the irradiation dose to≥1 Gy, noticeable surface irregularities and erosive areas with decrease in Sharpey's fiber sites were observed. These observations could shed light on the hazardous effects of irradiation fields to the functioning of the human teeth.     

碳离子辐照对人肺癌细胞A549细胞周期进程的影响

选取对数生长期人肺癌细胞A549接受0—6.0 Gy 碳离子照射， 用克隆形成法检测细胞的存活率； 并于照射后12和24 h收集细胞， 用流式细胞术检测细胞周期各时相的细胞百分比， 观察不同剂量碳离子辐照对A549细胞周期进程的影响。 结果显示: 0—6.0 Gy 碳离子照射后细胞存活率显著下降； 照射后12 h细胞发生G0/G1期阻滞， 而照射后24 h， 1.0 Gy 照射组细胞在G0/G1期阻滞， 2.0—6.0 Gy 照射组细胞在G2/M期阻滞。 上述结果表明， 在A549细胞接受碳离子照射后的12 和24 h内， 1.0 Gy 照射可持续激活细胞G1期检查点， 而2.0—6.0 Gy 碳离子照射后其细胞周期进程是随时间变化的。 To investigate the effects of cell cycle progression of A549 cell induced by 12C6+ ion irradiation at different doses, the survival fractions of the A549 cells were determined by colony forming assay; cell cycles were analyzed by FACS at 12 h or 24 h after irradiation. The results showed that the percentage of survival in the A549 cells decreased with irradiation doses. Compared with control group， the percentage of the cells in G0/G1 phase significantly increased at 12 h after irradiation with different doses of 12C6+ ions. However， at 24 h after irradiation the percentage of the cells in G0/G1 phase significantly increased with 1.0 Gy 12C6+ ions， while the cells showed increasing percentage in G2/M phase with 2.0, 4.0 or 6.0 Gy 12C6+ ions. The results suggested that G1 cell cycle checkpoint was activated in 12—24 h after irradiation with 1.0 Gy 12C6+ ions， but after irradiation with 2.0—6.0 Gy 12C6+ ions， the cell cycle progression of the A549 cells changed with time.     

Impact of gamma radiation on the eruption rate of rat incisors

The present work aims to test the effect of gamma radiation on the rate of eruption of rat incisors. One hundred and five adult male albino rats were used and irradiated at different gamma doses. The effects of irradiation were investigated by numerical measurements of eruption rate, histological investigation using light microscope and spectral analysis using Fourier Transform Infra-Red (FTIR). No detectable changes were observed in the groups with smaller radiation doses. There was a significant decrease in the eruption rate starting from the 4?Gy radiation dose. The observation of histological sections revealed disturbance in cellular elements responsible for eruption as well as periodontal disturbance in the samples irradiated with 4 and 6?Gy. FTIR Spectroscopy of control group and the group irradiated by 0.5?Gy showed similar absorption bands with minor differences. However, samples irradiated by 1?Gy showed significant changes in both molecular structure and conformation related to carbonates and hydroxyl groups. From the previous results, it could be concluded that gamma irradiation negatively affects the eruption rate of the rat incisors especially with higher doses.     

Gamma-photon induced modifications in Polyvinylchloride (PVC) film

Gamma photon induced modifications in Polyvinylchloride (PVC) polymer have been studied in the dose range of 10¹-10⁶Gy at room temperature. Polyvinylchloride films have been irradiated with different doses of gamma radiation from a ⁶⁰Co source. To monitor the chemical and structural changes caused by gamma radiation IR and UV-Vis spectroscopy of pristine and irradiated PVC have been performed and using the spectral data some changes in the properties have been investigated. The spectral studies have indicated that at a dose of 10⁶Gy scissioning of the C-a bonds takes place. This scissioning of the chain initiates decomposition at a lower temperature. Thermal stability of the polymer reduces due to irradiation but the decomposition patterns remain the same. The optical band-gap is found to decrease due to irradiation at doses bigher than 10³Gy.     

电子束辐照浓香型白酒催陈效果的研究

以能量为1.5 MeV/u,剂量分别为500,750,1000,1250,1500 Gy的电子束对1,2,4,6,8年等5种年份浓香型白酒进行辐照处理;扫描各酒样200～400 nm波段的紫外光谱,根据紫外光谱图的差异,计算了280～300 nm波段的光谱曲线相似度,分析光谱曲线变化规律。结果表明,对于前4种白酒,对照样与辐照样光谱曲线相似度值越小,催陈效果越好;白酒存放时间越久,酒体风格转向老熟所需剂量越小,越容易达到最佳催陈效果;对于8年白酒,辐照剂量超过750 Gy后,白酒体系动态平衡被打破,各单体物质增加,出现返生现象。因此,电子束辐照技术对低年份浓香型白酒催陈效果显著,是一种先进、高效的催陈方法。