QUANTUM DIFFUSION IN TWO-DIMENSIONAL OCTAGONAL QUASICRYSTALS

We have studied the quantum diffusion in an octagonal quasiperiodic tiling. Paticular attention is paid to the analysis of long-time behavior of the autocorrelation function C(t) and the relationship between diffusion and fractal dimensions of energy spectrum. For the pure hopping model, numerical calculations show that C(t)～t^-1 , which corresponds to the case of periodic systems. For the combined model, in which the contribution of site potentials is considered, C(t)～t^-δ with 0＜δ≤1. The scaling factor δ is related to Hamiltonian parameters and the type of site where electron is initially located. Moreover, we find a crossover from δ=1 to 0＜δ＜1 with increasing site potentials.     

重费米子材料与物理

作为典型的强关联电子体系,重费米子材料表现出丰富的量子基态,如反铁磁序、铁磁序、非常规超导、非费米液体、自旋液体、轨道序和拓扑态等.相比其他强关联电子体系,重费米子体系的特征能量尺度低,可以通过压力、磁场或掺杂等参量对不同量子态进行连续调控,因而是研究量子相变、超导及其相互作用的理想体系.本文简要介绍重费米子研究的发展历史和国内外研究现状,概述几类典型的重费米子材料,并简单阐述重费米子超导、量子相变和强关联拓扑态等前沿科学问题.     

181Hf(n,γ)182Hf反应截面测量

在中国原子能科学研究院重水研究堆上用活化法对反应堆中子引起的181Hf (n,γ)182Hf反应截面进行了测量. 反应堆中样品照射位置的热中子与超热中子的通量比值约为10. 照射后样品中的182Hf/180Hf和 181Hf/180Hf的原子数比值是用热电离质谱测量的. 本工作以180Hf (n,γ)181Hf反应截面(14.80±0.60 b)为标准，测得的反应堆中子引起的181Hf (n,γ)182Hf反应截面值为80.0±5.6 b.     

面向实战化需求的流体力学教学改革与实践

流体力学课程理论性强、内容抽象、枯燥难懂,传统教学内容缺乏与实战化内容的联系,学员学习目标不明确,理论性与实战性分离,因而学员的主体性和教学内容的高阶性不足。为了解决学员学习兴趣不高、动力不足的问题,面向实战化教学需求,在教学内容上发展了“四个引入”理念,即引入流动现象、军事应用、科研成果、思想方法,在教学模式上提出了具体实施的“六个环节”,即设疑、分析、释疑、拓展、应用、创新,通过理论与实际相结合,搭建起了课堂与战场之间的桥梁。提升了学员学习动力和兴趣,改善了教学效果。     

非线性非局部边界条件的半线性耦合抛物型方程组

该文研究具有非负初始数据和非局部边界条件u|αΩ×(0,∞)=∫_Ωψ_i(x,y,t)u_i~(l_i)(y,t)dy的半线性抛物型方程组u_(it)=△u_i+c_i(x,t)u_(i+1)~(pi),(x,t)∈Ω×(0,∞).给出了方程组解的整体存在与爆破准则.这些结果表明,权重函数c_i(x,t),ψ_i(x,y,t)和指数p_i,l_i的大小在确定方程组的解是否爆破中起着关键的作用.     

一类强退化抛物方程弱解的惟一性

研究了如下形式的强退化抛物方程(C)(u)/(t)=(2A(u,x,t))/(x2)+(B(u,x,t))/(x),基于Holm gren方法,证明了弱解的惟一性.     

一个描述原子高里德伯态的数学物理方程

本文用一个具有二个正则奇点和一个非正则奇点的二阶微分方程描述原子。假设原子中价电子的势能有如下形式 V(r)=-(e~3/r)[1+δ+α′/(r+γ′)+β′/(r+y′)~3] δ是离化度,通过解含V(r)的薛定谔方程可获的解析解,各种状态的势和波函数中的參数可用量子数亏损这个量表示。波函数的形状和节点数与Hartzee-Fock-Slater(HFS)理论一致。计算了与波函数内、外区的行为有关的典型物理量,并与实验和HFS理论进行了比较。用此模型计算的高里德伯态的振子强度和极化率比较满意。     

吸附法制备CuO-Ag/SiO2纳米复合物

利用吸附法原位制备CuO/SiO2、CuO-Ag/SiO2纳米复合物,研究了不同吸附质体系中预负载的纳米Ag粒子对CuO的影响。结果表明:Ag粒子对CuO的影响因吸附质的不同而不同。以Cu(Ac)2为吸附质,纳米Ag几乎没有影响;以NaOH为吸附质,纳米Ag使得CuO的晶粒粒径增大。这一结果与铜物种对Ag晶粒粒径的影响规律完全不同。通过比较不同吸附质的吸附行为,Cu(OH)2与硅胶表面的相互作用被认为是导致这一现象的原因。     

Fabrication and properties of the meander nanowires based on ultra-thin Nb films

We report the fabrication and the study of superconducting properties of ultra-thin Nb superconducting meander nanowires, which can be used as superconducting nanowire single-photon detectors （SNSPDs）. The ultra-thin （about 7- nm thick） Nb films are patterned into micro-bridges, and 100-nm wide meander nanowires by using e-beam lithography （EBL）. The average transition temperature （Tc） of the nanowires is about 4.8 K and the critical current density jc is about 2.8 × 10^6 A/cm2. Superconducting characteristics of the specimens at different applied magnetic fields up to 8 T （parallel or perpendicular to the specimen） are systematically investigated. The normalized temperature t （= T/Tc） dependences of the parallel critical field （HcⅡ） for both the micro-bridge and the meander nanowire are almost the same, following the Ginzburg and Landau （GL） formalism for ultra-thin films. However, in perpendicular field and in the vicinity of Tc （〉 0.95Tc）, the critical field Hc⊥ of the nanowire exhibits a down-turn curvature nonlinear temperature dependence while the micro-bridge displays a linear temperature dependence. The nonlinear behavior of Hc⊥ in the nanowire is believed to be due to the fact that in the vicinity of Tc the coherence length becomes larger than the line width. Additionally, the localization of carriers in the nanowire could also contribute to the nonlinear behavior. The resistive transitions could be described by the phase-slip model for quasi-one-dimensional system. Moreover, the hysteresis in I-V curve of the meander nanowires can be illustrated by a simple model of localized normal hotspot maintained by Joule heating.     

1,8-二甲氧基乙基萘的合成

以1,8-二萘酸酐为原料,经氢化铝锂还原得1,8-二羟甲基萘(2);2经浓盐酸酸化生成1,8-二氯甲基萘(3);3经氢化铝锂还原为1,8-二甲基萘(4);用强碱丁基锂和叔丁醇钾将4转化成二钾盐后与甲氧基氯甲烷反应合成了1,8-二甲氧基乙基萘,其结构经1H NMR和13C NMR和HR-MS表征.