The level and distribution of chromosomal aberration of tomato seeds at different penetration depths of carbon ions

The relationship between the penetration depth and the level and distribution of chromosomal aberration of the root tip cells were investigated by exposure of the superposed tomato seeds to 80 MeV/u carbon ions. The results showed that on the entrance of the beam the chromosomal aberration level was low. Damage such as breaks and gaps were dominant. At the Bragg peak, the chromosomal aberration level was high. The yields of dicentrics, rings and disintegrated small chromosomes increased but the yields of breaks and gaps decreased. These results are consistent with the distribution of the physical depth dose pro. le of carbon ions. It is effective to deposit the Bragg peak on the seeds to induce hereditary aberration in the mutation breeding with heavy ions.

Microstructural evolution in silicon implanted with chlorine ions

In the present work p-type Si specimens were implanted with Cl ions of 100 keV to successively increasing fluences of 1 x 10(15), 5 x 10(15), 1 x 10(16) and 5 x 10(16) ions cm(-2) and subsequently annealed at 1073 K for 30 min. The microstructure was investigated with the transmission electron microscopy (TEM) in both the plane-view and the cross-sectional view. The implanted layer was amorphized after chlorine implantation even at the lowest ion fluence, while re-crystallization of the implanted layer occurs on subsequent annealing at 1073 K. In the annealed specimens implanted above the lowest fluence three layers along depth with different microstructures were found, which include a shallow polycrystalline porous layer, a deeper single-crystalline layer containing high density of gas bubbles, a well separated deeper layer composed of dislocation loops in low density. With increasing ion fluence the thickness of the porous polycrystalline layer increases. It is indicated that chlorine can suppress the epitaxial re-crystallization of implanted silicon, when the implant fluence of Cl ions exceeds a certain level.

Production cross section of Th-236 in the interaction of U-238 with 60 MeV/u O-18 ions

The neutron-rich target-like isotope Th-236 has been produced in the U-238-2p multinucleon transfer reaction between a 60 MeV/u O-18 beam and natural U-238 targets. The activities of thorium were determined after radiochemical separation of Th from the mixture of uranium and reaction products. The Th-236 isotope was identified by the characteristic gamma-rays of 642.2, 687.6 and 229.6 keV. The production cross section of Th-236 was determined to be 250 +/- 50 mu b.

Liquid-liquid extraction of protactinium(V) using tri-iso-octylamine

Solvent extraction of protactinium with tri-iso-octyl-amine (TIOA) in xylene, benzene, carbon tetrachloride and chloroform from HCl, HF, HNO3, HClO4 and H2SO4 media was studied using Pa-233 as a radiotracer. The extraction efficiencies of protactinium were determined as a function of shaking time, concentrations of mineral acids in aqueous phase, extractant concentrations and diluents in organic phase. The extraction mechanism was discussed. The results show that the extracted species in the organic phase is [(R3N-H)(n)Pa(OH)(x)Cl-y(5-x-y)].

Color center formation in alpha-Al2O3 induced by high energy heavy ions

Single crystals of alpha-alumina were irradiated at room temperature with 1.157 (GeVFe)-Fe-56, 1.755 (GeVXe)-Xe-136 and 2.636 (GeVU)-U-238 ions to fluences range from 8.7 x 10(9) to 6 x 10(12) ions/cm(2). Virgin and irradiated samples were investigated by ultraviolet visible absorption measurements. The investigation reveals the presence of various color centers (F, F+, F-2(2+), F-2(+) and F-2 centers) appearing in the irradiated samples. It is found that the ratio of peak absorbance of F-2 to F centers increases with the increase of the atomic numbers of the incident ions from Fe, Xe to U ions, so do the absorbance ratio of F-2(2+) to F+ centers and of large defect cluster to F centers, indicating that larger defect clusters are preferred to be produced under heavier ion irradiation. Largest color center production cross-section was found for the U ion irradiation. The number density of single anion vacancy scales better with the energy deposition through processes of nuclear stopping, indicating that the nuclear energy loss processes determines the production of F-type defects in heavy ion irradiated alpha-alumina.

低速~(40)Ar~(17+)离子入射金属Be表面发射的近红外光谱线和X射线谱；Infrared Light and X-ray Emissions of ~(40)Ar~(17+) Impacting on Be Surface ；

用速度不同的(动能EK=272和357keV,速度v=1.14×106和1.72×106m/s)的高电荷态离子40Ar17+分别入射金属Be表面,同时测量这种相互作用过程中产生的近红外光谱线和X射线谱。实验结果表明,在低速范围内(速度小于玻尔速度vBohr=2.19×106m/s),速度较小的40Ar17+离子在到达金属的表面临界距离Rc到进入表面(2—3原子层)的进程中,形成了较多的高激发态Ar原子,其退激辐射较强的光谱线,进而验证了经典过垒模型。

CSRm外靶实验装置中快塑料闪烁体阵列型探测器研制

随着HIRFL-CSR工程的顺利完工，更高能量和更多种类的束流可以用于实验，大大拓展了可开展的核物理实验研究的内容。为了更好的利用束流，促进核物理实验研究的深入，设计和建造新的大规模探测设备成为必然。本论文工作针对CSR主环外靶实验终端建设，完成了利用飞行时间方法探测中子和带电粒子的两种快塑料闪烁体探测器阵列的研制。其中中子探测器有效体积为1.5  1.5  1 m3，包含252个，两种不同结构的探测单元；每组带电粒子探测器（TOFW）由60个探测单元构成，有效探测面积为1.21.2m2。论文工作通过解决材料加工、抛光、粘接、单元包装、测试等一系列工艺难题，完成了中子探测器和三组TOFW探测器的安装和测试。利用宇宙射线测试得到两种类型中子探测单元和TOFW探测单元的平均时间分辨分别为278 ± 59、272 ± 44和258 ± 51 ps，扣除各种因素后，探测单元的本证时间分辨可以达到80、100和150 ps；对后者利用12C重离子束流在线测试，得到本证时间分辨好于70 ps,完全满足设计的要求。论文工作中还设计完成了探测单元中光电倍增管高压系统的控制和监测系统，并建立了以LED为光源的光刻度系统，用于探测单元的刻度和工作状态的在线监测。在终端现场对探测器进行的初步在束测试表明，两种探测器工作稳定，运行良好，其性能均满足实验需求

重离子引起DNA损伤及其对细胞周期进程的影响

目的：木论文重点研究重离子不同剂量离子辐照后DNA损伤程度的变化，以及进而引起的细胞周期改变等现象。为重离子治癌的临床应用积累必要的基础数据。材料与方法：采用兰州重离子研究装置（HIRFL）加速的碳、氖等重离子辐照体外培养的贴璧肿瘤细胞，以单细胞电泳法（SCGE）检测DNA的损伤程度；以流式细胞技术（FCM）检测细胞的周期改变现象。结果：1．SMMC-7721月干癌细胞经重离子（氖、碳）辐照后，DNA损伤现象明显，表现为单细胞电泳中出现的普遍的拖尾现象（t-test，P<0.001，compared with control。2．80MeV／u 2ONe10＋辐照后立即检测发现：2Gy造成100％的细胞损伤：8Gy照射造成80％的细胞严重损伤：且彗尾拖尾长度随剂量增加早．指数关系增长，仔值为0.99058。3．辐照后12小时，若干不同剂量辐照的样品其彗尾长度趋于相同：如05协、Ic）和ZGy辐照样品的彗尾长度分别为132.3±12.8、132.9±9.5和133.1±11.7μm，24h，时为35.0±3.9、35.5±4.1和48.2±6.Oμm，这说明在一定剂量范围内（0.5-2Gy）的辐照下，随着修复时间的延长，细胞DNA的损伤程度将趋于相同。同时，细胞继续孵育12小时，对于0.55-2Gy辐照组来说DNA的损伤情况是24小时内操作最严重的。4．辐照后24小时，0.5-2Gy辐照组埙份明显修复，略高于对照，但是对于4Gy和SGy辐照组仍带有明显的损伤现魏。簇说眼熏离子辐照（>4Gy）所致DNA报伤的不足修复性。5，DNA的损伤将导致细胞通过一系列调节机制抑制细胞周期的进行，为DNA修复系统提供充足的时间进行DNA修复，从而造成明显的细胞周期阳．滞现琢，这在重离子辐照实验中同样得到证实，尤其是S期、G2／M期阻净带现象非常明显。

xylE基因用于监测根瘤菌在土壤中存活的研究

通过细菌接合将质粒ｐＬＶ１０１６（含ｘｖｌＥ基因）转移至ＲｈｉｚｏｂｉｕｍｆｒｅｄｉｉＱＢ１１３０和Ｒｈｉｚｏｂｉｕｍｌｅｇｕｍｉｎｏｓａｒｕｍｂｖ．ｖｉｃｉａｅＢ４０，ｘｙｌＥ基因在根瘤菌内表达活性较高．质粒ｐＬＶ１０１６携带的ＸｙｌＥ基因用于监测根瘤菌在灭菌和未灭菌土壤中的存活，结果表明，在灭菌土壤中含质粒与不含质粒菌株存活菌数量之间无显著差异（Ｐ＜０．０５），大接种量有利于细菌的生长与繁殖，Ｂ４０（ｐＬＶ１０１６）质粒丢失比例很低．以低于１０６ＣＦＵ·ｇ－１干土浓度接种时，ＱＢ１１３０（ｐＬＶ１０１６）质粒丢失率随接种浓度的降低而增大．未灭菌土壤中生物因素抑制了释放菌株的生长，大接种量有利于细菌存活．以低浓度（１０６ＣＦＵ·ｇ－１干土）接种时，ＱＢ１１３０（ｐＬＶ１０１６）质粒丢失比例高于Ｂ４０（ｐＬＶ１０１６）．

Thermodynamic investigation of the azeotropic mixture composed of water and benzene

The molar heat capacity of the azeotropic mixture composed of water and benzene was measured by an adiabatic calorimeter in the temperature range from 80 to 320 K. The phase transitions took place in the temperature range from 265.409 to 275.165 K and 275.165 to 279.399 K. The phase transition temperatures were determined to be 272.945 and 278.339 K, which were corresponding to the solid-liquid phase transitions of water and benzene, respectively. The thermodynamic functions and the excess thermodynamic functions of the mixture relative to standard temperature 298.15 K were derived from the relationships of the thermodynamic functions and the function of the measured heat capacity with respect to temperature.

长白山红松针阔叶混交林林冠层叶面积指数模拟分析

根据长白山原始红松针阔叶混交林光合有效辐射的连续3年自动观测结果,结合便携式叶面积仪的季节观测,建立了以林冠上下光合有效辐射估算森林冠层叶面积指数的半经验公式.结果表明,该方法可以很好地反映叶面积的季节动态.通过3年叶面积指数的季节动态比较发现,该森林冠层叶面积的起始生长日期随气温稳定通过0℃的日期延迟而延迟,整个生长季的叶面积动态可划分成上升期、相对稳定期和下降期,每个阶段都与大于0℃的积温存在较好的相关关系,分别用Logistic曲线和线性方程表达.并对叶面积的观测和估算方法中存在的问题进行了讨论.

Study on conical columns for semi-preparative liquid chromatography

The dynamic flow profiles and column efficiencies in conically shaped semi-preparative liquid chromatographic columns (inlet ID larger than outlet ID) with two different conical angles (7degrees and 15degrees) were studied. The dynamic flow profiles were studied by an on-column visualization method. Conical columns were compared with cylindrical column of the same length and internal volume. The results showed that the flow profile of a sample band in the conical column of 7degrees (50 mm x 17 mm --> 11 mm ID) was parabolic in shape. The sample band migrated slower in the wall region than in the central region, as in the cylindrical column (50 mm x 14 mm ID). However, the sample band in the conical column of 15degrees (50 mm x 20 mm --> 7 mm ID) migrated slower in the central region than in the wall region, resulting in a reverse parabolic flow profile, in contrast to that in cylindrical column. This indicated that a flat flow profile might be realized in a conical column with a conical angle between 7degrees and 15degrees. The conical column of 15degrees had the highest column efficiency among the three columns under the same conditions. Compared with the cylindrical column packed with identical packing material, the conical column of 15degrees had 22%-45% higher column efficiency and 11%-27% higher peak height.