998 resultados para 190-1178A


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由60MeV/μ18O离子照射天然钍靶所引起的232Th-2p反应产生230Ra,通过放射化学分离方法从被照射的靶中提取出镭元素并制成薄源,经230Ra230Ac得到230Ac.用云母裂变径迹探测器和PHGeγ射线探测器对来自源中的裂变碎片和γ谱进行记录和测量,借助于所测得的两个裂变事件和γ谱,鉴别了β-延发裂变核230Ac,得到了它的β-延发裂变概率为(1.19±0.85)×10-8.

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基于荷能离子与固体相互作用特点 ,提出了一种新的制备光致发光材料的方法——高能重离子辐照 .用这种方法研究了 Si O2 薄膜的光致发光特性 ,发现高能 84 Kr和 4 0 Ar离子辐照可在注碳Si O2 薄膜样品中产生强的蓝 -紫光发射带 ,掺杂碳增强了辐照样品的发光特性

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用细胞质分裂阻断微核技术(简称CB微核法)研究了癌细胞的放射敏感性,结果表明;CB 微核法可用来预测癌细胞对重离子和γ射线的放射敏感性,具有省时且成功率高的特点。细胞 受重离子作用后,每双核细胞的微核与剂量的效应关系适合方程 Y= c+ kDn或 Y=c+aD+βD2,受γ射线作用后,每双核细胞的微核与剂量的效应关系适合方程 Y=c+ aD。在相同剂量下,重离子效应高于r射线效应。

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Excited states in Tl-188,Tl-190 have been studied experimentally by means of in-beam gamma spectroscopy techniques, and resulted in the identification of a strongly coupled band based on the pi h(9/2) circle times nu i(13/2) configuration with oblate deformation. The oblate band in doubly odd Tl nuclei shows low-spin signature inversion. It is the first experimental observation of low-spin signature inversion for a band associated with the oblate pi h(9/2) circle times nu i(13/2) configuration.

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High-spin level structure of Au-188 has been studied via the Yb-173(F-19, 4n gamma) reaction using techniques of in-beam gamma-ray spectroscopy. Based on the experimental results, the level scheme of 188Au has been revised significantly. The previously reported positive parity levels have been modified and a new 20(+) level was proposed to feed the 18(+) states via two low-energy transitions. The existence of the 20(+) and the level structures above it are similar to those in the neighboring odd-odd Au-190,Au-192, therefore, the pi h(11/12)(-1)circle times-vi(13/2)(-2)h(9/2)(-1) configuration was assigned to the 20(+) state.

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Calculations of the 4d absolute photoabsorption cross sections of the Xe-like Cs+ ion covering the energy region from 80 to 190 eV have been performed by using the multi-configuration Dirac-Fock method. The calculated cross sections are compared with the absolute experimental photoabsorption cross-section spectrum (Kjeldsen et al 2002 J. Phys. B: At. Mol. Opt. Phys. 35 2845) and other available theoretical results. In the 80-90 eV region, the discrete structure resulting from photoexcitation of a 4d electron into nf and np orbits are successfully identified. Above the 4d threshold, i.e. in the 90-190 eV energy region, a reasonable agreement between experiment and computations is found for the intense 4d -> epsilon f shape resonance.

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本论文分为两部分,分别沿自旋和同位旋自由度开展研究工作。第一部分介绍原子核高自旋态研究的相关背景知识、基础理论等,描述在束γ谱学研究的实验技术和方法,分析和讨论形变核179Pt转动带能级结构的特性,并采用相关理论对其进行分析。通过融合蒸发反应149sm(35cl,P4n)布居奇A核179Pt的高自旋激发态。指认179Pt的组态为1/2-[521],5/2-[512〕和7/2+〔633〕的三条转动带。在hco=0.27 Mev附近,观测到1/2-〔521]带内顺排角动量突然增大,建议该现象是由一对113/2中子发生顺排造成的。另外观察到在7/2+〔633]带中出现较大的旋称劈裂。建议由于三轴形变加强了波函数中来自几=1/2轨道的组分,从而导致较大的旋称劈裂的出现。论文第二部分介绍重丰中子核衰变性质研究以及新核素合成、鉴别工作的相关背景知识、理论基础及实验技术。并对相关的研究工作分别进行阐述。通过快中子反应合成并鉴别了新核素19705和新的同核异能素186rnTa,利用γ(x)谱学方法首次建立了19705的部分衰变纲图。测得它们的半衰期分别为2.8士0.6 min和1.50.1 min,并与理论计算结果进行了比较;进行了原子核基态β延发裂变(pDF)的实验研究,经测量首次发现了230Ac的两个pDF事件,测得23OAc的pDF几率为(1.19±0.40)

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对长白山北坡海拔 70 0~ 190 0m的 13个森林群落进行了群落组成、结构随海拔上升变化情况的研究。结果表明 ,随着海拔的升高 ,群落的建群种组成、层次结构等 ,都表现出由复杂多样逐渐向简单单一过渡的变化趋势 ,从 70 0m至 170 0m ,针叶树所占的比例随海拔的升高呈明显的增加趋势 ,阔叶树比例随之减少 ,到林线时针阔叶树种均急剧减少 ,沿海拔梯度存在明显的树种更替现象。从群落的平均胸径及胸高断面积和可知 ,最大值出现于 90 0~ 110 0m及 16 0 0m ,这 2个海拔段正是不同森林群落类型间的过渡区。除海拔 180 0m的岳桦林之外 ,其它群落径级结构都呈倒J形分布 ,即各径级树木中 ,更新幼苗、幼树在数量上占绝对优势 ,随着胸径的增大 ,立木株数逐渐减少 ,这种径级结构表明 ,长白山北坡各海拔群落更新良好 ,群落处于稳定的发展状态。

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以“空间代时间”的方法 ,以种群径级结构代替年龄结构 ,采用静态生命表、生存分析和空间格局分析方法 ,探讨了长白山北坡不同海拔分布的岳桦种群的结构和动态规律。结果表明 ,在海拔 180 0、190 0和 2 0 0 0m ,随海拔升高 ,岳桦种群密度增大 ,径级分布范围减小 ,种群存活曲线由DeeveyⅡ型过渡到DeeveyⅠ型 ,种群由稳定型过渡为增长型 ,说明岳桦种群由低海拔向高海拔 ,群落处于不同的演替和发展阶段。而且随着岳桦径级的增大 ,其分布格局由集群分布过渡到随机分布。

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应用王刚提出的生态位重叠值公式 ,计测了长白山主要生态系统中 4 1个样点 4 2种主要地面藓类的生态位重叠值。以此为指标 ,分别应用主坐标排序、图论聚类及系统聚类分析方法 ,作出了反映 4 2种地面藓类的种间生态关系的二维投影图、最小生成树和动态聚类图。 3种方法相结合 ,能够对生态位重叠值矩阵进行直观地表达 ,并使所表达的藓类种间关系具有确切的生态学含义。研究表明 ,按生态位重叠值大小 ,长白山主要生态系统中地面主要藓类可区分出落叶松 -沼泽藓类、高山苔原藓类和暗针叶林 -岳华林藓类 3大类。 4 2种藓类中 ,生态位宽度 ( B)与种数 ( N)符合公式 :N=38.1 985×e- 14 .62 60× B,绝大部分藓类的生态幅很窄。

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The fabrication and performance evaluation of a miniature twin-fuel-cell on silicon wafers are presented in this paper. The miniature twin-fuel-cell was fabricated in series using two membrane-electrode-assemblies sandwiched between two silicon substrates in which electric current, reactant, and product flow. The novel structure of the miniature twin-fuel-cell is that the electricity interconnect from the cathode of one cell to the anode of another cell is made on the same plane. The interconnect was fabricated by sputtering a layer of copper over a layer of gold on the top of the silicon wafer. Silicon dioxide was deposited on the silicon wafer adjacent to the copper layer to prevent short-circuiting between the twin cells. The feed holes and channels in the silicon wafers were prepared by anisotropic silicon etching from the back and front of the wafer with silicon dioxide acting as intrinsic etch-stop layer. Operating on dry H-2/O-2 at 25 degreesC and atmospheric pressure, the measured peak power density was 190.4 mW/cm(2) at 270 mA/cm(2) for the miniature twin-fuel-cell using a Nafion 112 membrane. Based on the polarization curves of the twin-fuel-cell and the two single cells, the interconnect resistance between the twin cells was calculated to be in the range from 0.0113 Omega (at 10 mA/cm(2)) to 0.0150 Omega (at 300 mA/cm(2)), which is relatively low. (C) 2003 Elsevier Science Ltd. All rights reserved.