金属介电函数的正确运用——以金属纳米球诱导的二能级系统的基态能级移动为例

金属对电磁场的响应包括自由和束缚电荷两部分的贡献,大学物理教学中通常分别用Drude模型和Lorentz模型描述,然而,以上模型所得的介电函数只在一段较窄的频率范围内能与实验数据吻合.因此,在实际科研工作中,当物理量与较宽频率范围内的电磁场响应有关时,原则上介电函数应当采用实验测量值而不能采用模型化的结果.本文以金属纳米球诱导的二能级系统的基态能级移动为例,分别展示采用模型化的介电函数和实验介电函数时,能级移动计算结果的差异.     

基于格林函数法研究金属线栅在太赫兹波段的散射特性

本文运用格林函数法分析金属线栅在太赫兹(THz)波段的散射特性, 研究金属线栅的衍射效应对其传输特性的影响. 研究结果表明, 在零级衍射区入射电磁波的透过振幅随a/λ的增大单调增加, 在零级衍射极限处透过振幅达到最大值. 过渡区的临界频率处, 由于衍射效应的加强, 出现入射电磁波透过曲线的振荡. 衍射区受到衍射效应的影响入射电磁波透射振幅曲线总体下降, 并随a/λ的增大单调减少. 与微波传输线方法相比, 该方法摆脱了入射电磁波的波长需大于线栅常数且要求线栅的厚度远远小于金属线的宽度的限制, 能准确的分析系统的电磁场的分布特性, 更具普适性. 关键词： 金属线栅 太赫兹波 散射 格林函数法     

应用多尺度纠缠重整化算法研究量子自旋系统的量子相变和基态纠缠

应用多尺度纠缠重整化算法模拟自旋为1/2的一维量子XYX模型,通过计算局域序参量和度量纠缠的单缠节(one-tangle)、并发纠缠(concurrence)和纠缠比率R,确定系统的基态相图和纠缠相图.发现系统的纠缠相图比基态相图包含更多的物理信息.另外,从局域序参量和能隙与外磁场的标度关系,萃取出与磁化率和关联长度有关的临界指数β和v.     

负跃层浅海声传播问题的解析解及其在水下脉冲声传播研究中的应用

提出一个基于波数积分理论的解析解,可用于计算包含海面下均匀层、负跃层、海底上方均匀层以及液态均匀海底的负跃层浅海波导中的声场。对声源位于水体不同层中的情况给出详细的推导,给出深度格林函数的解析解,并介绍了如何利用其计算点源和线源这两种情况下的声场.通过一个典型的负跃层浅海算例,验证了本文所提方法的精度,以及处理点源及线源问题的能力.此外,将本文提出的方法应用于水下脉冲声传播研究。针对某次实验的实际海洋环境,利用本文方法研究接收到的脉冲信号的波形特点,并与利用射线理论分析得到的相邻脉冲到达时间间隔等理论结果进行比较·结果表明,利用本方法得到的相邻脉冲到达时间数值结果与理论值高度一致。本方法非常适用于需要大量重复计算声场的情况,如水下脉冲声传播、海底声学参数反演等问题的计算机仿真研究。     

Wigner函数的性质及其在一维无限深势阱和一维谐振子中的应用

首先介绍了Wigner函数的基本性质以及以Wigner函数为基础的相空间定态微扰理论,然后将其应用到一维无限深势阱和谐振子。 推导出一维无限深势阱所对应的Wigner函数,而且发现了存在于其纯态Wigner函数中奇特的压缩效应, 并利用不确定性关系给予了解释。同时计算出一维无限深势阱和谐振子在微扰的作用下,相应Wigner函数和能级的修正。 In this article, the qualities of Wigner function and the corresponding stationary perturbation theory are introduced and applied to one dimensional infinite potential well and one dimensional harmonic oscillator, and then the particular Wigner function of one dimensional infinite potential well is specified and a special constriction effect in its pure state Wigner function is discovered, to which, simultaneously, a detailed and reasonable explanation is elaborated from the perspective of uncertainty principle. Ultimately, the amendment of Wigner function and energy of one dimensional infinite potential well and one dimensional harmonic oscillator under perturbation are calculated according to stationary phase space perturbation theory.     

气体团簇离子束装置的设计及其在表面平坦化、自组装纳米结构中的应用

根据超声膨胀原理,n(10-10^4)个气体原子可以绝热冷却后凝聚在一起形成团簇,经过离化后,形成带一个电荷量的团簇离子,比如Arn^+.当团簇离子与固体材料相互作用时,由于平均每个原子携带的能量(~eV)较低,仅作用于材料浅表面区域,因此,气体团簇离子束是材料表面改性的优良选择.本文介绍了一台由武汉大学加速器实验室自主研制的气体团簇离子束装置,包括整体构造、工作原理及实验应用.中性团簇束由金属锥形喷嘴(F=65-135μm,q=14°)形成,平均尺寸为3000 atoms/cluster,经离化后,其离子束流达到了50μA.Ar团簇离子因其反应活性较低,本文运用Ar团簇离子(平均尺寸为1000 atoms/cluster)进行了平坦化和自组装纳米结构的研究.单晶硅片经Ar团簇离子束处理后,均方根粗糙度由初始的1.92 nm降低到0.5 nm,同时观察到了束流的清洁效应.利用Ar团簇离子束的倾斜(30°-60°)轰击,在宽大平坦的单晶ZnO基片上形成了纳米波纹,而在ZnO纳米棒表面则形成了有序的纳米台阶,同时,利用二维功率谱密度函数分析了纳米结构在基片上的表面形貌和特征分布,并计算了纳米波纹的尺寸和数量.     

用有限电流元法识别HL-2A 装置的等离子体边界

在电流丝模型对HL-2A装置等离子体边界重建取得满意结果[3]、[5]的基础上，本文用有限电流元模型对HL-2A等离子体边界进行了重建研究。计算和实验结果表明，在通常情况下，有限电流元模型比固定电流丝模型的重建误差稍小，前者误差小于3mm，后者误差小于6mm。当部分有限电流元分布在等离子体边界之外时，用有限电流元模型仍然可以成功重建边界。有限电流元的位置在一定范围内变化时，重建的误差都很小。用普通奔腾4 2.4GHz PC机计算一组等离子体放电边界的时间不超过1ms。有限电流元法能准确而快速地识别等离子体的偏滤器位形，这对于HL-2A装置的实时位形控制是基本和重要的。     

GeHn±(n=0,1,2)的势能函数和光谱常数研究

用密度泛函B3lyp/6-311++g(d,p)方法对 分子离子进行理论研究。结果表明：GeH,GeH+,GeH-1均能稳定存在,GeH+2和GeH-2有亚稳定态存在,其基态电子态分别是: 2Π(GeH),1Σ(GeH+),3Σ(GeH-),2Σ(GeH+2)和2Π(GeH-2),GeH+2和GeH-2的势能函数呈明显的‘火山态’型,导出了相应的分子离子的解析势能函数、光谱数据和力常数,比较了四参数、八参数Murrell-Sorbie势和Zhu-Wang势对不稳定分子势能函数的拟合情况,指出了用八参数Murrell-Sorbie势对‘火山态’型势能函数的拟合也是合适的;同时讨论了电荷对势能函数和能级的影响。     

Optimal design and lifetime calculation of the belt chamber by finite element method

Abstract

A mixed numerical-analytical method for an optimal strength design is presented. Optimal number n of components and optimal radii r_j are calculated for an equivalent cylindrical model of the compound vessel. An iterative numerical method is proposed for evaluation of optimal overlaps Δr_j. A finite element method (FEM) elastic-plastic program has been developed to estimate the vessel lifetime.     

Analysis of the special hollow-core photonic crystal fibre by finite element method

Two kinds of fabricated hollow-core photonic crystal fibres （HC-PCFs） arc studied using finite element method （FEM） because the structures of the fibres are special, Normalized transmission spectra and transverse intensity distribution of the modes are calculated and measured. And the dispersion characteristics of these two kinds of HC- PCFs were analysed from 400 nm to 800 nm. Simulated and measured results show that the special structure could affect the properties of HC-PCFs, By comparing the simulated values with the measured results, it can be clarified that FEM is feasible and accurate for analysing photonic crystal fibres whose structures are irregular and complex.     

超轻量化SiC反射镜有限元分析及应用

对超轻量化SiC反射镜进行了有限元分析。设计了超轻量化SiC反射镜的镜体结构。采用MSC.Nastran分析软件对其进行了有限元工程分析。分析结果表明,可满足SiC反射镜面形精度的要求和轻量化的要求。介绍了一种SiC反射镜无镜框支撑结构。     

小尺度阻尼边界封闭空间声传递函数的有限元素法计算

如何求解阻尼边界封闭空间中声源点到接收点的低频声传递函数已成为目前小尺度封闭空间可听化技术研究的关键技术，能处理任意形状及复杂边界条件的有限元素法可作为求解该问题的适合方法，以室内声声有源Helmholtz方程及其相应边界方程为基础，本文推导出了用于小尺度阻尼边界封闭空间声传递函数的有限元素求解方法，并编制了相应的计算机程序，在算例中，首先通过与模态叠加法计算结果进行比较，验证了该方法的正确性。最后计算了某型车体内腔中任意两点间声传递函数。     

Finger capacitance of a terahertz photomixer in low-temperature-grown GaAs using the finite element method

Interdigitated finger capacitance of a continuous-wave terahertz photomixer is calculated using the finite element method.For the frequently used electrode width(0.2 μm) and gap width(1.8 μm),the finger capacitance increases quasi-quadratically with the number of electrodes increasing.The quasi-quadratic dependence can be explained by a sequence of lumped capacitors connected in parallel.For a photomixer composed of 10 electrodes and 9 photoconductive gaps,the finger capacitance increases as the gap width increases at a small electrode width,and follows the reverse trend at a large electrode width.For a constant electrode width,the finger capacitance first decreases and then slightly increases as the gap broadens until the smallest finger capacitance is formed.We also investigate the finger capacitances at different electrode and gap configurations with the 8 μm× 8 μm photomixer commonly used in previous studies.These calculations lead to a better understanding of the finger capacitance affected by the finger parameters,and should lead to terahertz photomixer optimization.     

Response of thermal source in a transversely isotropic thermoelastic half-space with mass diffusion by finite element method

The two-dimensional problem of generalized thermoelastic diffusion material with thermal and diffusion relaxation times is investigated in the context of Lord-Shulman theory. As an application of the problem, a particular type of thermal source is considered and the problem is solved numerically by using a finite element method. The components of displacement, stress, temperature distribution, chemical potential, and mass concentration are obtained. The resulting quantities are depicted graphically for a special model. Appreciable effect of relaxation times is observed on various resulting quantities.     

Waves and energy in random elastic guided media through the stochastic wave finite element method

Energy propagation in random viscoelastic media is considered in this Letter. The forced response of uncertain waveguide subject to time harmonic loading is treated. This energy model is based on a spectral approach called the “Stochastic Wave Finite Element” (SWFE) method which is detailed in this Letter. Assuming that the random properties are spatially homogeneous in the media, the SWFE is a hybridization of the deterministic wave finite element and a parametric probabilistic approach. The proposed model is applicable in a wide frequency band with reduced time consumption. Numerical examples show the effectiveness of the proposed approach to predict the statistics of kinematic and quadratic variables of guided wave propagation. The results are compared to Monte Carlo simulations.     

小阻尼界面房间声传输函数和声脉冲响应函数的有限元素法

有限元法可用于以声波动方程为基础通过数值计算求解室内声场,适用于分析界面阻抗非均匀分布和复杂形状房间内声场的低频特性。本文首先介绍了小阻尼界面条件下室内声场简正方式、声衰变系数、混响时间的ＦＥＭ计算方法。在此基础上导出了房间内两点之间声传输函数和声脉冲响应函数的ＦＥＭ计算模型,并以矩形房间为例详细讨论了有关细节。本文所讨论的计算模型可以映房间内不同的声源点,接收点位置上的声压频谱特性和脉冲响应的时