Ar离子辐照非晶态合金引起的尺寸变化

利用兰州重离子加速器(HIRFL)提供的2.79MeV/u Ar离子,在50K以下的低温辐照了Fe₄₇Ni₂₉V₂Si₆B₁₆等4种非晶态合金样品,室温下使用光学显微镜对辐照前、后的同一样品拍照,对比测量了样品的宏观尺寸. 结果表明:在辐照剂量为1.5×10¹⁴离子/cm²时,非晶态合金形变不明显,测量到的样品宽度相对增长Δb/b₀均小于1.0%;当辐照剂量增加到1.6×10¹⁵离子/cm²时,所有非晶态合金样品都发生了显著的形变,其宽度相对增长分布在4.3%—12.0%之间,对此结果进行了定性的分析.     

替代式合金系统的电阻率

本文将文献[1]的无序晶态合金电阻率理论推广到包含长程有序的系统,从而建立了适用于晶态金属,无序及有序替代式合金的Ziman型电阻率理论。根据这个理论我们详细讨论了这类系统电阻率的温度依赖性。文中着重指出:合金系统结构因子的超结构峰对电阻率有重要贡献。这个贡献在低温下是一个T²项,它比电子-电子散射引起的T²项大得多,因而合金系统电阻率在T<<Θ(Θ是德拜温度)时有ρ≈ρ₀+ρ_a(T/Θ)²+ρ_i(T/Θ)⁵的形式。据此,许多A-15化合物正常态电阻率在低温下的反常行为很容易解释。作为例子,我们将低温电阻率的理论表达式与V₃Si的测量值作了比较,符合得很好。     

铕的快中子俘获截面

使用大液体闪烁探测器,相对于金的俘获截面测量了铕(Eu)六个能量点的中子俘获截面值;用光学模型和统计理论计算了¹⁵¹Eu和¹⁵³Eu在0.1—2.0MeV能区的中子俘获截面;对实验测量和理论计算结果进行了分析和讨论.     

高能重离子碰撞中的末态分布与夸克物质信号

本文结合液体动力学模型与状态方程,分析讨论了高能重离子碰撞过程中是否发生相变以及相变的级次对末态分布的影响.由于集体效应随入射能量和核质量的增加而加强,预计对于RHIC(每对核子能量S=100+100GeV)上进行的¹⁹⁷Au-¹⁹⁷Au碰撞,快度分布有可能作为夸克物质形成的信号.     

PGBs对高能e+e－湮没产生顶夸克对的单圈量子效应

在一代Technicolor(TC)模型中计算了PGBs(PseudoGoldenstoneBosons)对高能e⁺e^－→tt过程的单圈量子效应.给出了重整化的形状因子和矩阵元.计算了PGBs对总截面前后不对称参数A_FB和左右不对称参数A_LR的虚贡献,结果表明选取适当的参数值,新物理对以上可测量的贡献最大分别可达:－12.3%、－3.3%和－11.7%.在下一代对撞机上这一理论结果能为TC理论打开实验的窗口.同样的计算表明PGBs对e⁺e^－→bb过程的单圈贡献小于－1.0%.     

Hf-基非晶合金的力学性能研究

 利用MTS810实验机和分离式霍普金森压杆（SHPB）,对Hf_44.5Cu₂₇Ni_13.5Ti₅Al₁₀块体非晶合金进行了准静态和动态压缩实验,应变速率范围为10^-4~10³ s^-1,给出了不同应变速率下非晶合金的应力-应变曲线,并对其压缩断口形貌进行了扫描电镜观察。结果表明：在准静态压缩条件下,Hf_44.5Cu₂₇Ni_13.5Ti₅Al₁₀非晶合金不具有应变速率敏感性,在由放射区和扇形区组成的断口形貌上观察到纳米级韧窝和60 nm左右的周期性条纹结构;在动态压缩条件下,随着应变速率的增加,动态屈服强度明显减小,合金具有应变速率敏感性,同时断裂表面为夹杂着脉络条纹的絮状结构。进一步观察发现,动态压缩断口上存在3种特征断裂形貌：树枝状条纹、典型脉络花纹和合金熔体。     

58Ni(n,p),60Ni(n,p),62Ni(n,α)和54Fe(n,p)反应截面的测量与评价

本实验用活化法测量了中子能量在13.60MeV—17.77MeV的⁵⁸Ni(n,p)^58m+gCo,⁶⁰Ni(n,p)⁶⁰Co和⁶²Ni(n,α)⁵⁹Fe三个反应道的反应截面值,并计算了反应截面测量误差的协方差矩阵.实验的测量误差在3%—7%范围内.     

离子液体凝胶聚合物电解质PP13TFSI-LiTFSI-P(VdF-HFP)的电化学性能 (cited: 1)

采用溶液浇铸法将N-甲基-N-丙基哌啶二(三氟甲基磺)亚胺(PP13TFSI)、二(三氟甲基磺)亚胺锂与偏氟乙烯-六氟丙烯共聚物(P(VdF-HFP))混合制备离子液体凝胶聚合物电解质(ILGPEs). 通过扫描电子显微镜观察发现,这种离子液体凝胶聚合物电解质由于液体相的均匀分布而具有疏松的结构. 采用电化学阻抗、计时电流法、线性扫描伏安法测试了电解质的离子电导率、锂离子迁移数和电化学窗口. 室温下离子液体凝胶聚合物电解质的离子电导率和锂离子迁移数分别是0.79 mS/cm和0.71,电化学窗口为0～5.1 Vvs. Li⁺/Li. 电池性能测试表明,这种离子液体凝胶聚合物电解质在Li/LiFePO₄电池中是稳定的,放电容量在30、75和150mA/g倍率下分别为135、117和100 mAh/g,电池经100个循环后容量保持在100%而几乎没有衰减.     

吡啶离子液体与水混合体系中蒽醌-2-磺酸钠的激光闪光光解机理

利用激光闪光光解技术研究了蒽醌-2-磺酸钠(AQS)在吡啶离子液体N-丁基吡啶四氟硼酸盐([BPy][BF₄])与水(H₂O)混合体系中的光化学反应过程. 实验结果表明,AQS的激发三重态(³AQS^*) 会与H₂O快速反应,不断增加[BPy][BF₄]在混合体系中的体积比(V_IL),瞬态吸收光谱发生了很大变化. 510 nm附近的瞬态吸收带变化最大,在0< V_IL< 0.1时,吸光度会随着[BPy][BF₄]的增加而增加;而在V_IL>0.1时,吸光度则随着比例的增加而减小. 然而380 nm附近吸收带的吸光度却一直在增加. 通过拟合近似地得到了瞬态物种B和³AQS^*的表观动力学参数. 另外还讨论了³AQS^* 与阳离子之间的夺氢反应,通过对350~420 nm处光谱图的分析,推断出这一范围的瞬态吸收光谱是³AQS^*与AQSH^·的叠加谱. 在混合体系中,³AQS^*分别与H₂O和[BPy][BF₄]的反应是一对竞争反应. 还发现在高浓度的离子液体环境下,体系的整体反应速率会减弱.     

锆离子注入锆-4合金缺陷的慢正电子研究

采用慢正电子束多普勒展宽谱研究了Zr离子注入Zr-4合金产生的缺陷及其退火回复行为，发现经过大于离子注入剂量为1×10¹⁶cm^-2的样品所产生的缺陷在注入过程中已经回复，而对剂量为1×10¹⁵cm^-2样品做300℃退火处理，其缺陷基本回复，得出合金缺陷回复能较低的结论. 考虑到材料的缺陷含量越高，其抗腐蚀性能越差，在辐照环境下通过给材料保持一定温度，即可使其缺陷得到较好回复，从而提高材料的抗腐蚀性能.     

Three-dimensional temperature measurement in turbulent thermal convection by extended range scanning liquid crystal thermometry

The usable temperature range of liquid crystal thermometry has been extended and used to measure three-dimensional temperature fields in turbulent thermal convection. The color of the liquid crystals is calibrated against temperature using the standard method in which hue is the single input variable and two new methods: hue/intensity as input variable, and hue, saturation and intensity as input variables to a neural network. Relative to the hue calibration, the new methods extend the range over which temperature can be measured by more than 100%. Three-dimensional temperature measurements of turbulent thermal convection over smooth surfaces were carried out at a flux Rayleigh number of 3 × 10⁹ by scanning a white light sheet normal to the visualized image plane and capturing a number of sequential images at various positions of the light sheet. Stacks of the planar data were composed into three-dimensional temperature distributions. The results indicate the presence of an irregular spoke pattern over the surface and the generation of plumes from the intersections of the patterns, consistent with other investigations.     

Theory of collective dynamics of liquid polyvalent metal: Hg

Recently suggested microscopic theory of collective dynamics of a liquid has been used to successfully explain the detailed experimental dynamic structure factor of liquid mercury at room temperature, observed experimentally recently using high resolution inelastic X-ray scattering for various momentum transfers lying in the range 3 nm⁻¹–37.1 nm⁻¹.     

Thermophysical properties and structure of stable and metastable liquid cobalt

The thermophysical properties and structure of liquid cobalt are investigated in the temperature range from 1000 to 2400 K. The properties include density, molar volume, enthalpy and specific heat at both normal and undercooled states. The density decreases linearly with the increase of temperature. At the melting point, the value of density is 7.71 g cm⁻³, and its temperature coefficient is . The molar volume increases with the increase of temperature in a nonlinear manner. The enthalpy increases linearly with the rise of temperature. This indicates that the specific heat changes little with temperature: 40.11 J mol⁻¹ K⁻¹. Furthermore, the liquid structure is studied by analyzing the pair correlation function. With the increase of undercooling, the degree of short range order of liquid cobalt becomes more and more remarkable, which is deduced by the appearance of a saddle at the second neighbor distance.     

Channeling study of boron implanted silicon: Liquid nitrogen temperature implantation

Silicon samples have been boron implanted at 150 keV at liquid nitrogen temperature to a dose of 3.6 × 10¹⁵/cm². This dose rendered the implanted layer amorphous as viewed by helium ion backscattering. Four kinds of room temperature measurements were made on the same set of samples as a function of the isochronal annealing temperature. The measurements made were the determination of the substitutional boron content by the channeling technique using the B¹¹(p, α) nuclear reaction, observation of the disorder by helium ion backscattering, determination of the carrier concentration by van der Pauw Hall measurements, and the sheet resistivity by four point probe measurements. These measurements are compared with results from samples implanted at room temperature. The carrier concentration correlates well with the substitutional boron content for both room temperature and liquid nitrogen temperature implantations. Following annealing temperatures in the 600 to 800°C range, a much larger percentage of the boron lies on substitutional lattice sites, and therefore the carrier concentration is larger, if the implantation is done at liquid nitrogen temperature rather than at room temperature. Following liquid nitrogen temperature implantation, reverse annealing is observed from 600 to 800°C in the substitutional boron content, carrier concentration and sheet resistivity. The boron is more than 90 per cent substitutional after annealing to 1100°C for both the room temperature and liquid nitrogen temperature implantations. The low temperature implantation produced a buried amorphous layer, and this layer was observed to regrow from both the surface and substrate sides at approximately equal rates.     

The structure of liquid In - Te and Tl - Te alloys

The atomic structure of liquid In—Te and Tl—Te alloys have been investigated as a function of composition and temperature by means of X-ray diffraction. The following features emerge from this experiment. The structure of liquid In—Te alloys is similar to that of pure Te in the range of composition from 35 to 100 at % Te. This implies that the structure of pure Te plays a significant role in these alloys. At the composition of In₂Te₃, the second peak near the region ofQ=3.2Å^–1 disappears with the increase of temperature. This corresponds to the breakdown of the electron localization based on the measurement of magnetic susceptibility. On the other hand, there is no substantial change in the structure of liquid Tl—Te alloys as the delocalization temperature of the electrons is approached.     

Messung kleiner Wärmekapazitäten bei tiefen Temperaturen

A sensitive method for the direct determination of specific heats in the liquid helium temperature range is described. The reached precision allows the measurement of heat capacities as small as 10^?5 cal °K^?1.     

Charge transport study on single crystals of β-LiAl

Charge transport properties of β-LiAl were studied in the composition range of 48.0–50.2 at.% Li. Measurements were made on single crystal samples and down to the liquid He temperature. The resistivity changes linearly with temperature above 125 K, with a thermal coefficient of 72–95nΩ cm K^?1. The Matthiessen law was obeyed very well. A component dependent on temperature, which was described by the Grüneisen formula, is insensitive to a change of the chemical composition. On the other hand, the residual resistivity depends largely on the composition and contributes up to 58% of the total resistivity in Li_0.498. It is chiefly due to the substituted Li atoms on the Al sublattice.     

Liquid xenon study under shock and quasi-isentropic compression

Abstract

The shock adiabat for liquid xenon in the density range of 5.2–7.9 g/cm³ and pressure range of 8–70 GPa was investigated. The brightness temperature of a shock wave front from 5000 K to ?15,000 K, as well as the electrical conductivity behind the front from 4·10³ to 1.2·10⁵ 1/Ohm m, were measured. X-ray technique was used to measure quasi-isentropic compression of liquid xenon up to ～13 g/cm³.

The equations of state for liquid and solid phases of xenon were found. Anomalous behavior of xenon at p=8.37 g/cm³ was revealed, that is due to a structural transition.     

Fluctuation theory of hydrogen bonding applied to vibration spectra of HOD molecules in liquid water. II. Infrared spectra: contour shape,integrated intensity,temperature dependence

The infrared spectra of HOD molecules in liquid water are calculated at constant density over the temperature range of 10 to 400°C from the statistical distributions of the vibration frequencies of water OH-groups determined previously from the experimental Raman spectra. Their shape and position are extrapolated over a wider temperature range. The dependence of contour shape and integrated intensity of the IR band on the frequency of its maximum, the first moment of a statistical contour and temperature are described numerically and analytically. Calculations are in qualitative agreement with all available experimental material and fitted quantitatively at a density of water of ～1?g?cm^?3. The success of the proposed model applied to infrared spectra supports once more the continuum treatment of liquid water structure.