50MeV/u 12C离子实验靶区出射中子角分布实验测量

本文用氟和碳阈探测器对50MeV/u ¹²C离子引起的重离子反应实验靶区E_n>11MeV和E_n>20MeV中子的角分布进行了实验测量,结果显示出明显的前冲分布,较高能量的中子具有更强的前冲趋势.     

47MeV/u 12C同133Cs反应碘同位素产额的测定

用放化法测量了47MeV/u ¹²C同¹³³Cs相互作用时碘同位素的产额.发现碘同位素产额分布曲线的峰位在¹²⁴I附近,半宽度为6.5质量单位,最可几产物的质量损失为9.2个质量单位.靶核削裂2个质子的产物¹³¹I的形成截面约0.47—0.87mb,没观察到靶核削裂2个质子,再俘获1个中子的产物¹³²I的活性.     

60MeV/u 18O离子同天然铀反应236Th的产生截面

用60MeV/u ¹⁸O离子轰击天然铀靶, 通过²³⁸U-2p多核子转移反应产生丰中子类靶同位素²³⁶Th. 从复杂的反应产物和大量的铀中放射化学分离、纯化钍, 用HPGe探测器联同多道分析器测量分离出的钍部分. 根据642.2keV, 687.6keV和229.6keV特征γ射线, 指定²³⁶Th同位素; 确定²³⁶Th同位素的产生截面为250±50μb.     

Ba同位素的截面测量

用60MeV/u¹⁸O离子轰击天然铀靶,通过²³⁸U(¹⁸O,X)反应产生钡的放射性同位素.使用放射化学分离方法从被照射过的铀靶中分离出Ba,用HPGeγ射线探测器测量Ba样品的γ射线谱,经对所得时间累计谱的处理和分析得到了Ba同位素的产生截面,并观察到Ba同位素分布中的双峰分布现象.     

28.7MeV/u的 14，16，18 O+7，9Be反应中的同位素分布研究

用同位旋相关的Boltzmann-Langevin方程研究了在入射能量为28.7MeV/u下,不同弹核^14O,^16O和^18O轰击不同靶核^7Be和^9Be的反应,计算了生成碎片的产生截面,发现用丰中子（缺中子）炮弹或丰中子（缺中子）靶进行反应,所得到的产物均有丰中子（缺中子）的碎片出现。同位素分布宽度和峰位与入射体系密切相关,产生碎片的电荷数越接近入射弹核的电荷数,则同位素分布的宽度越大,峰位偏离β稳定线值越远,其同位旋效应越明显。。     

30MeV/u 40Ar+112,124Sn反应中的同位素产额比与核温度

系统研究了30MeV/u^40Ar ^112,124Sn反应中的轻粒子同位素产额比随角度和初始激发能的变化关系,对于两个反应体系,均观察到3He/^4He和^6Ni/^7Li的产额比随角度的增加而增加,^6He/^4He和^8Li/^7Li随角度的增加而减少,统计发射的运动学效应不能完全符合实验结果,各种单同位素产额比与靶核的N／Z比有关,表现出同位旋效应,而由双同位素比提取的核温度几乎没有靶核相关性。     

46.7MeV/u 12C引起的弹核碎裂反应

测量了46.7MeV/u ¹²C束流轰击不同靶核的核反应中前方向出射的类弹碎片,发现弹核碎裂产物的最可几能量可用Abrasion图象来解释.它们的平行动量分布宽度满足Goldhaber关系式,实验中提取的约化平行动量分布宽度σ₀=80±10MeV/c,接近于相对论情形下的值,并且σ₀对于不同的反应系统有相近的值.     

Cross Sections of Barium Isotopes in Interaction of 60 MeV／u ^18O with Natural Uranium

The reactions induced by heavy ions lower than 10 MeV/u have been studied widely. Their reaction mechanism has been also understood in more detail. The contribution to the reaction cross sections in the low energy reactions comes mainly from complex nuclei and deep inelastic process. Early studies mainly focused on the nuclear collisions of low and high energies. In the recent years, great attention has been paid on the intermediate energy heavy ion collisions. Among them measurements of the cross sections and recoiling properties for the target fragmentation products have been applied widely to study the mechanism of the nuclear reactions induced by the intermediate energy heavy ions. But there are a few papers on raodioehemieal studies in the intermediate energy region up to now.     

F同位素的反应总截面测量和17F可能的质子皮结构

应用透射法对中能区F同位素与C靶的反应总截面进行了测量。发现^17F的反应总截面比其邻近同位素的反应总截面稍有增强。用Glauber模型和BUU模型对F同位素进行了差异因子d的分析。^17F的差异因子d比共附近同位素稍有增强。分析结果表明^17F可能存在质子皮结构。     

28MeV/u 18O与全阻止厚天然铅靶反应中丰中子汞同位素的截面测量

本次实验利用28MeV/u的¹⁸O束流和一套在线熔化铅靶装置以及4πΔEβ—γ符合技术,测量了该中能重离子反应中丰中子汞同位素^205—208Hg生成的相对截面比以及绝对截面的近似值.并外推出了²⁰⁹Hg的可能生成截面.发现由靶核²⁰⁸Pb削裂两个质子添加一个中子而生成²⁰⁷Hg的截面有一个突然的比较大的下降,这可以由反应的Q值的变化规律得到解释.     

Interaction of a New Fluorescent Probe with DNA and its Use in Determination of DNA

In this paper we reported a metal complex 1-Zn (2,5-di-[2-(3,5-bis(2-pyridylmethyl)amine-4-hydroxy-phenyl)-ethylene]-pyrazine-Zn) as a fluorescent probe sensing DNA. The result of the competitive experiment of the probe with ethidium bromide (EB) to bind DNA, absorption spectral change and polarization change in the presence and absence of DNA revealed that interaction between the probe and DNA was via intercalation. Ionic strength experiment showed the existence of electrostatic interaction as well. Scatchard plots also confirmed the combined binding modes. The fluorescence enhancement of the probe was ascribed to highly hydrophobic environment when it bound the macromolecules such as DNA, RNA or denatured DNA. The binding constant between the probe and DNA was estimated as 3.13 × 10⁷ mol⁻¹ L. The emission intensity increase was proportional to the concentration of DNA. Based on this, the probe was used to determine the concentration of calf thymus DNA (ct-DNA). The corresponding linear response ranged from 2.50 × 10⁻⁷ to 4.75 × 10⁻⁶ mol L⁻¹, and detection limit was 1.93 × 10⁻⁸ mol L⁻¹ for ct-DNA.