LBO晶体的布里渊散射与弹性和压电系数的测量

简述了应用布里渊散射测量晶体的弹性和压电系数的方法,推导了C_2v点群晶体(100),(010)和(001)晶面内任意波矢方向的布里渊散射张量及声速各向异性方程.根据上述方法及结果,用180°散射测量了LBO晶体不同波矢方向的布里渊散射谱,得到了LBO晶体在特超声频率下所有独立的弹性和压电系数,并依此计算了该晶体的声速各向异性曲线. 关键词：     

铌酸锂单晶一些振动模式的机电耦合系数

本文利用晶体的压电、弹性、介电矩阵,通过矩阵及张量运算,推导出铌酸锂晶体厚度模机电耦合系数的精确公式。并计算了任何切割点三个振动模式的机电耦合系数,所得曲线对使用这种晶体具有一定的参考意义。     

La3Ga5SiO14晶体的介电性质、弹性与压电性质

研究了La3Ga5SiO14晶体的介电性质、弹性和压电性质，其中弹性和压电性质是利用高频振动模式通过谐振法测定的. 关键词： 介电性质 弹性 压电性质     

一维压电Fibonacci类准周期声子晶体传输特性

基于传输矩阵法研究了一维压电Fibonacci类准周期声子晶体的传输特性, 比较了一维Fibonacci序列压电准周期声子晶体与非压电准周期声子晶体以及压电周期性声子晶体的透射性. 计算结果表明:弹性波通过一维准周期结构压电声子晶体时与周期性声子晶体一样会有带隙的出现, 且发现具有压电性的Fibonacci序列准周期声子晶体禁带宽度发生了展宽. 进一步讨论了入射角度对固定频率下声子透射系数的影响,结果表明一维压电Fibonacci序列准周期结构声子透射性依赖于入射角度的选取.     

干涉法确定晶体压电坐标轴的正向

在测量晶体的压电系数时,首先要根据文献[1]的规定选定晶体的压电坐标系,同时还要确定实际晶体压电坐标轴的正向,方能测定晶体的压电系数及确定其正负号.为了准确、迅速地确定坐标轴的正向,我们利用晶体的反压电效应,采用干涉法进行了测量.这种方法迅速、准确、直观、且不破坏样品. 一、实验装置和测试原理 干涉法确定晶体压电坐标轴正向的实验装置如图1所示. 它的主体部分是一台泰曼干涉仪.将干涉仪分束后的一束光,通过一个45°反射镜垂直反射到干涉仪的台面上,在台面上装一样品台,样品台可通过调节微调螺丝在铅直方向上下移动.样品台上的…     

压电振子参数的电纳测量方法

通过对压电振子导纳轨迹的理论分析,本文提出了压电振子参数的电纳测量方法,并用该方法具体测定了钽酸锂(LiTaO_3)晶体的有关弹性常数和压电常数。     

Ca_3NbGa_3Si_2O_(14)晶体的介电和压电特性

利用Y切和 (yxl) 30°切两种样品测量了Ca3NbGa3Si2 O1 4晶体的介电、压电和部分弹性参数 .计算了 (yxl)θ切型相关压电常数随切角的变化 .与La3Ga5SiO1 4晶体相比 ,Ca3NbGa3Si2 O1 4晶体具有更优良的压电性能 ,其压电常数d1 1=7 93× 10 - 1 2 C N ,d1 4=- 5 88× 10 - 1 2 C N .     

Ca3NbGa3Si2O14晶体的介电和压电特性

利用Y切和(yxl)30°切两种样品测量了Ca3NbGa3Si2O14晶体的介电、压 电和部分弹性参数.计算了(yxl)θ切型相关压电常数随切角的变化.与La3Ga5SiO14晶体相比，Ca3NbGa3Si2O14晶体具有更优良的压电性能，其压电常数 d11=7.93×10-12C/N，d14=-5.88×10-12C/N. 关键词： Ca3NbGa3Si2O14晶体 介电常数 压电常数     

干涉法测量晶体电光系数实验装置的改进

用一台泰曼干涉仪,以压电晶体的逆压电效应补偿晶体电光效应所引起的光程变化,提供了一种简单、迅速和高灵敏度测量晶体电光系数的方法.     

干涉法测量晶体的压电系数

我们用一台泰曼干涉仪，以ＤＫＤＰ晶体的电光效应补偿由于晶体反压电效应听引起的光程差，提供了一种简单、迅速和高灵敏度测量晶体压电系数的方法．     

Elastic constants of sodium chlorate from 77 K to 350 K

The elastic constantsC ₁₁,C ₁₂ andC ₄₄ of sodium chlorate single crystal have been evaluated using 10 MHz ultrasonic pulse echo superposition technique. The values areC ₁₁=4.90,C ₁₂=1.39,C ₄₄=1.17 (× 10¹⁰ N/m ²) at 298 K and 6.15, 2.16, 1.32 (×10¹⁰ N/m ²) at 77 K. The data agree well with the values measured earlier up to 223 K. Brief mention is also made of the low temperature bonding problems in these soft crystals.     

Elastic property of organized lipid assembly — Effect of water incorporation and chain melting

The effect of electric field on the capacitance of lipid-water dispersion properly aligned on polyvinyl alcohol coated glass electrodes, shows a transition pattern where a rapid change in orientation of the organized lipid assembly takes place for an electric field above a threshold value (V_th), similar to that of Freedericksz’s transition as observed in the case of thermotropic liquid crystals. The splay elastic constant, k₁₁ and the bend elastic constant, k₃₃ have been calculated from the measured values of capacitance of the cell below and above V_th. These values change by several orders of magnitude depending upon the presence of water as well as temperature of chain melting of the lipid moiety.     

Elastic properties of GaxIn1−xP semiconductor

A theoretical procedure is presented for the study of elastic properties of the ternary alloy Ga_xIn_1−xP. The calculations are based on the pseudopotential formalism in which local potential coupled with the virtual crystal approximation (VCA) is applied to evaluate elastic constants c₁₁, c₁₂ and c₄₄, bulk modulus, shear modulus, Young's modulus and Poisson's ratio for the entire range of the alloy composition x of the ternary alloy Ga_xIn_1−xP. The effect of compositional disorder is included. Our results for parent compounds are compared to experimental and other theoretical calculations and showed generally good agreement. The inclusion of compositional disorder increases values of all elastic constants. During the present study it is found that elastic constant c₁₁ is largely influenced by compositional disorder.     

Elastic properties of MBH4 (M=Na, K, Rb, Cs)

The elastic properties of MBH₄ (M=Na, K, Rb, Cs) are studied by first-principles calculations using a projected augmented plane-wave method and finite strain method. KBH₄ is found to be the most isotropic material among MBH₄, which can be attributed to the contribution of C₄₄. The Debye temperatures are also calculated using theoretical elastic constants and the change along the series is explained.     

氢化铒高温高压下的弹性及热力学性质

利用第一性原理平面波赝势密度泛函理论, 并结合准谐德拜模型, 计算了立方萤石结构ErH2在不同温度和压强下的体积、热膨胀系数、体弹模量和等体热容等弹性性质及热力学性质。在温度高于1 100 K的条件下,计算出的等体热容趋近于Dulong-Petit极限。得到了绝对零度、零压强下ErH2的该结构的晶格常数为0.523 2 nm,与实验值0.523 0 nm非常接近。由不同的原胞体积得出了该体系的单点能与原胞体积的关系的数据;从计算出的高压下的弹性常数,根据立方晶系的力学稳定性条件,推断出立方萤石结构ErH2的相变压力约为20 GPa。     

Elastic Collisions Between two Ground-State P and D Atoms at Low and Ultralow Temperatures

The PD（X^3∑^-） interaction potential is constructed using the CCSD（T） theory and the basis set, augcc-pV5Z. Using this potential, the spectroscopic parameters are accurately determined. The present Do, De, Re, ωe, ωeχe, αe, and Be are of 3.056 99 eV, 3.161 75 eV, 0.142 39 nm, 1701.558 cm^-1, 23.6583 cm^-1, 0.085 99 cm^-1, and 4.3963 cm^-1, respectively, which almost perfectly conform with the measurements. A total of 26 vibrational states is predicted when J = 0 by solving the radial Sehrodinger equation of nuclear motion. The complete vibrational levels, classical turning points, initial rotation and centrifugal distortion constants when J = 0 are reported for the first time, which favorably agree with the experiments. The total and various partial-wave cross sections are calculated for the elastic impact between two ground-state P and D atoms at 1.0 × 10^-12 - 1.0 × 10^-4 a.u. when they approach each other along the PD（X^3∑^-） potential. No shape resonances exist in the total elastic cross sections, though the peaks can be found for each partial wave until l=6. The shape of the total elastic cross sections is dominated by the s partial wave at very low temperatures. Due to the weakness of the shape resonances of each partial wave, they are all passed into oblivion by the strong total elastic cross sections.     

单斜相HfO2薄膜弹性常数的第一性原理计算

用电子束蒸发沉积在K9玻璃基底上镀制HfO2薄膜,沉积温度为200℃,蒸发速率为0.03nm/s。由X射线衍射谱可知薄膜出现明显结晶,且为单斜相和正交相混合结构,其中单斜相占明显优势。用Jade5软件分析得到单斜相HfO2的晶格常数a,b,c以及晶格矢量a和c之间的夹角β。基于得到的晶格常数建立了单斜相HfO2薄膜的晶体结构模型。同时建立固态单斜相HfO2的晶体结构模型进行对比。通过密度泛函理论(DFT)框架下的平面超软赝势法,采用两种不同的交换关联函数:局域密度近似(LDA)中的CA-PZ和广义梯度近似(GGA)中的质子平衡方程(PBE),计算了薄膜态和固态单斜晶相HfO2的弹性刚度系数矩阵Cij和弹性柔度系数矩阵Sij,Reuss模型、Voigt模型和Hill理论下的体积模量和剪切模量,材料平均杨氏模量和泊松比。此外还计算得到薄膜态和固态单斜晶相HfO2在不同方向上的杨氏模量。     

Elastic,electronic and optical properties of cotunnite TiO2 from first principles calculations

The ultrasoft pseudopotential technique is used to explore the elastic, electronic and optical properties of cotunnite TiO₂ using LDA and GGA proposed by Perdew Wang (PW91), Perdew–Burke–Ernzerhof (PBE) functional as defined by Wu and Cohen (PBEWC) and PBE functional for solids (PBESOL). The calculated elastic constants bulk modulus, shear modulus and Young’s modulus are in agreement with the previous theoretical reports. From our investigated shear anisotropy factors (A₁, A₂, and A₃), we infer that cotunnite TiO₂ is strong anisotropy in case of A₁ and A₂ and less anisotropy in case of A₃. The value of mean sound speed and Debye temperature are calculated using the obtained values of elastic moduli. The calculated structural parameters are in accord with the reported experiment and theoretical results. Our obtained values of direct bandgaps show an improvement over the other previous theoretical reports. The values of the dielectric constant (ε₁(ω)) of cotunnite TiO₂ calculated within LDA and GGA approximations are 7.655 (LDA (CA-PZ)), 7.578 (GGA (PW91)), 7.685 (GGA (WC)) and 7.655 (GGA (PBESOL)), which are slightly higher than the experimental values of rutile (6.69) and anatase (6.55) polymorphs. The obtained values of the refractive index are consistent with rutile TiO₂ and higher than anatase phase. The investigated imaginary part of dielectric constant and absorption spectrum reflect that the cotunnite TiO₂ is a weak photocatalytic material as compared to anatase and similar to rutile phases.     

Elastic stability and electronic structure of low energy tetragonal and monoclinic PdN2 and PtN2

This paper studies the elastic and electronic structure properties of two new low-energy structures of PdN2 and PtN2 by first-principles calculations.It finds that tetragonal and monoclinic structures are more stable than a pyrite one.The always positive eigenvalues of the elastic constant matrix confirm that both the tetragonal and monoclinic structures are elastically stable.The origin of the low bulk modulus of the two structures is discussed.The results of the calculated density of states show that both of the two low-energy structures are metallic.     

Elastic constants determination by direct measurement of the beat wavelength between A0 and S0 Lamb modes with pulsed TV holography

A whole-field optical technique of high sensitivity, namely pulsed TV holography with phase evaluation by the Spatial Fourier Transform Method, is applied to the acquisition of instantaneous displacement fields of ultrasonic Lamb waves in aluminium plates a few millimetres thick. Two Lamb modes, the A0 and S0 ones, are simultaneously generated in the plate, producing a clear beating. Several values of the beat wavelength, corresponding to different excitation frequencies, are obtained by direct measurement of the distance between nodes in the wave field. The obtained values are fitted to the theoretical Rayleigh–Lamb frequency spectrum in order to determine the elastic constants of the plate material. We conclude that it is necessary to know the value of another parameter to univocally solve the problem, and so the bulk longitudinal wave velocity is measured by the pulse-echo method. Then the Poisson's ratio is obtained and, from these two parameters, the Young's modulus can also be determined.