Al的微观组态与LaNi3.75Al1.25的结构和弹性第一性原理研究

在全电子水平上，采用广义梯度近似密度泛函理论和全势能线性缀加平面波方法并结合二维立方拟合方法，对LaNi_3.75Al_1.25合金的晶体结构与弹性性质进行了理论研究.计算结果给出合金的晶格常数a=b=0.5137　nm，c=0.4018　nm，Al原子在晶胞中的微观分布为同时占据部分3g和2c等价格位，弹性常数C₁₁+C₁₂=281.2，C₁₃=82.3，C₃₃=227.3，以及体弹性模量B＝124.5、切变模量G＝68.2　GPa.还对态密度、能带结构和电荷密度进行了计算分析，并给出材料LaNi_3.75Al_1.25的电子线性比热系数23.45　mJ/molK². 关键词： 3.75Al_1.25')" href="#">LaNi_3.75Al_1.25 储氢合金 全势能线性缀加平面波 弹性常数     

SrHfO3和SrTiO3光学特性的第一性原理研究

用全电势线性缀加平面波法(FLAPW)计算了SrTiO₃和SrHfO₃的光学特性，即介电函数虚部ε₂(ω)、光学吸收系数I(ω)和反射率R(ω).对它们光学特性进行了对比分析，给出了它们光学特性的差别，并进行了解释.计算的SrTiO₃光学谱分别在4.4，7.4，8.3和23.6eV处出现峰值，且其在4.4eV处的峰值比较高而尖.计算结果与实验值符合得很好. 关键词： 平面波法计算 光学常量和参数 铁电体     

压力及杂质氢对金属锂弹性特性的影响

针对六角密堆金属锂16个原子超晶胞(supercell)、填隙一个氢原子的周期单元，采用基于密度泛函理论的平面波-赝势方法，研究了零温条件下压力及填隙氢掺杂对体系弹性性质的影响.结果表明氢掺杂导致体系的体模量增加.常压下掺杂体系的弹性常数C₁₁，C₃₃，C₆₆和C₁₂高于单质体系，剪切模量C₄₄有所下降，而C₁₃则与单质体系持平.压力作用下C₁₁，C₃₃和C₆₆一直大于单质体系，但C₁₂的值低于单质体系.在2GPa—4GPa压力区间内，弹性常数C₁₃呈反常变化，小于单质体系；在高压区掺杂体系的C₄₄和C₁₃则高于单质体系的相应量值，压力导致掺杂体系和单质体系之间剪切模的偏离加剧.掺杂体系在压力作用下依然保持压缩模的各向同性，具有和单质体系相似的特性. 关键词： 第一性原理 压力效应 弹性常数 金属锂     

四方铁电体PbFe0.5Nb0.5O3精细结构的第一性原理研究

采用全电势线性缀加平面波法(FPLAPW),计算了PbFe0.5Nb0.5O3的总能量,从而确定了它的四方铁电稳态结构,即B位离子(Fe和Nb)在四方铁电相的平衡构型.计算结果表明,Fe相对于氧八面体沿[001]方向的位移为0.022nm,而Nb的偏心位移为0.0020nm,其中铁电非稳性主要归因于前者 关键词： 铁电体 密度泛函理论 平面波法     

光折变晶体KTa0.5Nb0.5O3光学特性的第一性原理研究

用全电势线性缀加平面波法(FLAPW)计算了KTa0.5Nb0.5O3四方相和立方相 的光学特性，即介电函数虚部ε２(ω)、光学吸收系数I(ω)和反射率R(ω). 在四方相，介电虚部沿a，b轴，在3，7和23eV附近，分别有三个介电峰.沿c轴的三个介电峰分别位于4，8和23eV.其中4eV附近的介电峰非常尖锐而且高.从8至18eV，沿a，b ，c轴三个方向都有许多低的介电峰.通过对两相光学特性的对比分析发现铁电相KTa0.5Nb0.5O3具有更强的各向异性. 关键词： 平面波法计算 光学常量和参数 铁电体     

高压下有序晶态合金Fe3Pt的低能声子不稳定性及磁性反常

有序晶态Fe₃Pt因瓦合金处于一种特殊的磁临界状态, 这种磁临界状态下体系的晶格动力学稳定性对压力极为敏感. 基于密度泛函理论的第一性原理的投影缀加平面波方法研究了不同晶态合金的Fe₃Pt的焓和磁性随压力的变化规律, 结果表明, 在压力小于18.54 GPa下, P4/mbm结构是热力学稳定的相. Pm3m结构、I4/mmm结构、DO₂₂结构的Fe₃Pt在铁磁性坍塌临界压力附近体系的总磁矩急剧下降并具有振荡现象, 且I4/mmm结构和DO₂₂结构的Fe₃Pt 在临界压力附近出现了Fe1原子磁矩反转现象. 在43 GPa下, DO₂₂结构的Fe₃Pt出现了亚铁磁微观磁特性突然增强且伴随着体积突然增大的现象. 在高压下, 对Pm3m结构Fe₃Pt的晶格动力学计算表明, 压力小于26.95 GPa的铁磁态下体系的自发磁化诱导了体系横向声学支声子软化, 表明体系中存在很强的自发体积磁致伸缩. 特别是在铁磁性坍塌临界压力41.9 GPa至磁性完全消失的57.25 GPa压力区间, 晶格动力学稳定性对压力更加敏感. 压力大于57.25 GPa时, 压力诱导了体系声子谱的稳定.     

平面波展开法计算二维磁振子晶体带结构

磁振子晶体是光子晶体或声子晶体在磁性材料领域内的替代品,是近来的一个研究热点. 本文提出了磁振子晶体领域内的一种平面波展开法,其较传统的平面波展开法能节约一半以上的计算时间. 采用此方法,数值计算了由Fe/EuO二种铁磁材料构成的二维磁振子晶体带结构. 数值计算结果表明,在一定的体积填充率下,有自旋波带隙的出现;影响磁振子晶体带隙结构形成的主要因素是有效场中的交换作用场,其他作用场的影响相对很小. 关键词： 磁振子晶体 带隙 平面波展开法     

K(Ta0.56Nb0.44)O3四方铁电结构的第一性原理研究

在广义梯度近似(GGA)下利用全电势线性化的缀加平面波法(FLAPW)的总能量计算,确定了K(Ta_0.56Nb_0.44)O₃固溶体的四方精细结构,即B位离子(Ta和Nb)在铁电相的平衡构型.结果表明,Ta相对于氧八面体沿[001]方向有约为0005nm的偏心位移,而Nb的偏心位移约为0016nm,铁电非稳的发生主要应归因于后者. 关键词：     

SrHfO3和SrTiO3光学特性的第一性原理研究

用全电势线性缀加平面波法(FLAPW)计算了SrTiO3和SrHfO3的光学特性,即介电函数虚部ε2(ω)、光学吸收系数I(ω)和反射率R(ω).对它们光学特性进行了对比分析,给出了它们光学特性的差别,并进行了解释.计算的SrTiO3光学谱分别在4.4,7.4,8.3和23.6eV处出现峰值,且其在4.4eV处的峰值比较高而尖.计算结果与实验值符合得很好.     

第一性原理对金的高压相变和零温物态方程的计算

在密度泛函理论下，用缀加平面波加局域轨道方法，分别采用广义梯度近似(GGA)和局域密度近似(LDA)对金的面心立方晶格结构(fcc)、体心立方晶格结构(bcc)和六角密堆积结构(hcp)的结构能量进行了计算.在GGA下，计算得出fcc向hcp和hcp向bcc的相变分别发生在380GPa 和1250GPa；而LDA下相变分别发生在490GPa和790GPa.当计算压强达到2TPa时，bcc在这两种近似下仍然保持稳定的结构.根据不同体积下不同结构的电子态密度的特征，对发生相变的物理原因进行了定性的分析，在此基础上得到了金的零温状态方程. 关键词： 缀加平面波方法 固态相变 电子态密度 物态方程     

Measurement of the elastic constants of a columnar SiC thin film

The technique of resonant ultrasound spectroscopy was used to measure the elastic properties of a polycrystalline cubic silicon carbide (3C-SiC) thin film. The film, grown on a silicon (100) substrate, was 1.69 microns thick with columnar crystalline grains and a (111) texture. The substrate with the film was placed between two transducers and the resonant frequencies were measured; measurements were repeated after selective, timed dry etching of the film, allowing a determination of the elastic constants of the film alone. The film elastic constants, c(11)=371 and c(12)=146 GPa, were within a few percent of the literature values (c(11)=386, c(12)=136 GPa) of crystalline 3C-SiC. However, the film elastic constant c(44), 111 GPa, was significantly smaller than the bulk literature value, 254 GPa. For the film, c44 approximately (c(11)-c(12))/2, indicating that, quite unlike a bulk 3C-SiC crystal, the thin film is elastically isotropic.     

过渡金属锇在高压下的力学特性

 基于密度泛函理论平面波赝势法的第一性原理计算,研究了过渡金属锇在高压下的状态方程、弹性常数和其它力学性质。 计算结果表明：过渡金属锇具有很高的体积模量B₀（423.9 GPa）和弹性常数C₁₁（771.3 GPa）与C₃₃（852.0 GPa）,与金刚石的（B₀=452.8 GPa,C₁₁=C₃₃=1 082.9 GPa）比较,具有超低压缩特性;表征材料抵抗剪切变形能力的弹性常数C₄₄（269.8 GPa）和切变模量（276.8 GPa）只有金刚石的（C₄₄=586.9 GPa,G=537.5 GPa）一半,而所成的又是纯金属键,因此锇不具有超硬性。最后,定性分析了它的高体积模量和低硬度的微观电子机制,这对于设计与合成新的超硬性材料具有启发意义。     

First-principle calculations of structural,electronic, optical,elastic and thermal properties of $$\hbox {MgXAs}_{2}$$ ($$\hbox {X}=\hbox {Si}, \hbox {Ge}$$X=Si,Ge) compounds

First-principle calculations on the structural, electronic, optical, elastic and thermal properties of the chalcopyrite \(\hbox {MgXAs}_{2}\) (\(\hbox {X}=\hbox {Si}, \hbox {Ge}\)) have been performed within the density functional theory (DFT) using the full-potential linearized augmented plane wave (FP-LAPW) method. The obtained equilibrium structural parameters are in good agreement with the available experimental data and theoretical results. The calculated band structures reveal a direct energy band gap for the interested compounds. The predicted band gaps using the modified Becke–Johnson (mBJ) exchange approximation are in fairly good agreement with the experimental data. The optical constants such as the dielectric function, refractive index, and the extinction coefficient are calculated and analysed. The independent elastic parameters namely, \(C_{11}\), \(C_{12}\), \(C_{13}\), \(C_{33}\), \(C_{44}\) and \(C_{66 }\) are evaluated. The effects of temperature and pressure on some macroscopic properties of \(\hbox {MgSiAs}_{2}\) and \(\hbox {MgGeAs}_{2}\) are predicted using the quasiharmonic Debye model in which the lattice vibrations are taken into account.     

金属钒弹性波速与热力学函数的理论计算

在全电子水平上,基于广义梯度近似(GGA)的密度泛函理论和全势能线性缀加平面波方法(FLAPW)计算了钒的晶格参数,弹性波速和格临爱森参数.在德拜模型的基础上,利用弹性波速方法和原子位移方法分别计算了钒的德拜频率,以及在标准条件下(298.15 K,1atm)的热容,熵等热力学函数,并与实验值进行了比较.     

Structural and elastic properties of TiN under high pressure

We have investigated the structural and elastic properties of TiN at high pressures by the first-principles plane wave pseudopotential density functional theory method at applied pressures up to 45.4 GPa. The obtained normalized volume dependence of the resulting pressure is in excellent agreement with the experimental data investigated using synchrotron radial x-ray diffraction (RXRD) under nonhydrostatic compression up to 45.4 GPa in a diamond-anvil cell. Three independent elastic constants at zero pressure and high pressure are calculated. From the obtained elastic constants, the bulk modulus, Young's modulus, shear modulus, acoustic velocity and Debye temperature as a function of the applied pressure are also successfully obtained.     

石墨弹性波速与热力学函数的理论计算

在全电子水平上,基于广义梯度近似(GGA)的密度泛函理论和全势能线性缀加平面波方法(FLAPW)计算了石墨的晶体参数和弹性波速;在德拜模型的基础上,利用弹性波速方法和原子位移方法分别计算了石墨的德拜频率;采用统计物理方法计算了石墨在标准条件下(298.5 k,1 atm)的热容,熵,升华焓等热力学函数,并与实验值进行了比较.     

Theoretical investigation of sulfur defects on structural,electronic,and elastic properties of ZnSe semiconductor

The structural, electronic, and elastic properties of Zn Se1-xSx for the zinc blende structures have been studied by using the density functional theory. The calculations were performed using the plane wave pseudopotential method, as implemented in Quantum ESPRESSO. The exchange-correlation potential is treated with the local density approximation pz-LDA for these properties. Moreover, LDA+U approximation is employed to treat the "d" orbital electrons properly. A comparative study of the band gap calculated within both LDA and LDA+U schemes is presented. The analysis of results show considerable improvement in the calculation of band gap. The inclusion of compositional disorder increases the values of all elastic constants. In this study, it is found that elastic constants C11, C12, and C44 are mainly influenced by the compositional disorder. The obtained results are in good agreement with literature.     

FLAPW calculations of the EFG in semimetallic arsenic and antimony under varying pressure

The variation of the electric field gradient (EFG) at nuclear sites with pressure in semimetallic arsenic and antimony has been calculated using the full-potential linearized augmented plane wave (FLAPW) method. The results are compared with NQR data, which are available up to a pressure of 2 GPa. The calculated EFG depends sensitively on the values of the lattice parameters used. A theoretical investigation of the relationship between c/a and the internal parameter z, using FLAPW methods, has been carried out and compared with available X-ray diffraction data for arsenic and antimony. For antimony, the FLAPW calculations give results which are consistent with the experimental pressure variation of both the lattice parameters and the EFG. In the As case, the use of theoretical values of z leads to good agreement with the measured pressure variation of the EFG. This revised version was published online in August 2006 with corrections to the Cover Date.     

Determination of elastic constants using a scanning acoustic microscope

A cubic single crystal of GaAs with two polished (100)-surfaces was examined with a scanning acoustic microscope (SAM) in transmission mode. The images of the transmitted ultrasound amplitude measured at frequencies of 350–400 MHz contain sufficient information about the acoustic anisotropy of the crystal to determine the complete set of the three elastic constants C₁₁, C₁₂, C₄₄ numerically. This was done by an interactive fitting procedure correlating simulated images with the measured one. This technique seems to be universally applicable to virtually all sorts of single crystals. Compared to plane wave investigations it saves preparatory labour since one single crystal orientation suffices for a determination of all elastic constants.