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用扭摆及静电音频内耗仪研究了CuO在100~160K的内耗行为,实验结果表明在该温区存在一激活能为0.2eV的弛豫峰,而CuO的介电行为研究也表明在此范围有一弛豫峰,激活能为0.21eV。实验还进一步说明高温超导材料在该温区的反常行为与CuO无关。 相似文献
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采用固相反应法制备了Tb0.8Eu0.2MnO3多晶材料.对样品的X射线衍射(XRD)分析表明Eu3+固溶于TbMnO3中.测量了样品在低温(100 K ≤T≤ 300 K)和低频下(200 Hz≤f≤100 kHz)的复介电性质.在此温度区间内发现了两个介电弛豫峰.经分析认为低温峰(T≈170 K)起源于局域载流子漂移引起的偶极子极化效应,而高温峰(T≈290 K)则是由离子电导产生的边界和界面层的电容效应引起的.电阻率的测量显示在低温下(T≈230 K)存在明显的导电机制转变. 相似文献
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采用固相反应法制备了Tb0.8Eu0.2MnO3多晶材料.对样品的X射线衍射(XRD)分析表明Eu3+固溶于TbMnO3中.测量了样品在低温(100 K ≤T≤ 300 K)和低频下(200 Hz≤f≤100 kHz)的复介电性质.在此温度区间内发现了两个介电弛豫峰.经分析认为低温峰(T≈170 K)起源于局域载流子漂移引起的偶极子极化效应,而高温峰(T≈290 K)则是由离子电导产生的边界和界面层的电容效应引起的.电阻率的测量显示在低温下(T≈230 K)存在明显的导电机制转变.关键词:多铁性材料掺杂介电性质 相似文献
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PT-PEK-c电光聚合物薄膜的厚度和介电性质 总被引:2,自引:0,他引:2
研制了新的PT-PEK-c电光聚合物薄膜材料,用准波导耦合m线方法测量了PT-PEK-c电光聚合物薄膜的厚度,并测量了该聚合物薄膜在1×102Hz到1×107Hz频率范围内的室温介电常数.测量结果为:厚度d=2.328±0.315μm,在10KHz下,介电常数εr=4023±0.063,介电损耗tanδ=0.003. 相似文献
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对于BaTiO3/SrTiO3(BTO/STO)沿[001]方向有序的1:1超晶格,从最高对称性的P4/mmm结构出发,用第一性原理计算了布里渊区中心声子,通过冻结不稳定声子得到P4mm和Amm2结构,进一步冻结不稳定声子得到其基态单斜Cm结构.计算了三种畸变结构的自发极化及Cm结构的电子和声子对介电和压电的贡献.分析表明:ε22和e26主要来自于频率为197,146和97 cm-1的A′′声子的贡献;ε33和e33主要来自于频率为189和139 cm-1的A′声子的贡献;ε11和e11主要来自于频率为246 cm-1的A′声子的贡献.根据离子对介电和压电张量各分量的贡献可知,Ti和O离子对介电和压电有比较大的贡献. 相似文献
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制备了Bi7Ti4NbO21,Bi4Ti3O12及Nb掺杂Bi4Ti3O12(Nb-Bi4Ti3O12)层状结构铁电陶瓷材料.结合Nb-Bi4Ti3O12的介电温谱和退极化实验结果,研究了Bi7Ti4NbO21的晶体结构对其介电、压电性能的影响.高分辨透射电镜结果表明,在Bi7Ti4NbO21中,沿着c轴方向,(Bi2Ti3O10)^2-和(BiTiNbO7)^2-。两个类钙钛矿层分别与(Bi2O2)^2 层叠加堆积而成.这种晶体结构决定了Bi7Ti4NbO21的介电温谱在668℃和845℃出现介电双峰.结合极化样品的退化实验分析,说明材料在这两个温度附近发生了铁电一铁电相变、铁电一顺电相变,分别是(Bi2Ti3O10)^2-和(BiTiNbO7)^2-层状结构发生微观结构相变的结果.在退极化过程中,由于受热时钙钛矿层内空位引起的缺陷偶极子的定向排列受到破坏,引起材料部分退极化,表现为300℃热处理后Bi7Ti4NbO21的压电活性降低了10%,显示了室温下材料的压电性能来源于自发极化的固有电偶极子和缺陷偶极子的共同贡献. 相似文献
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热膨胀处理的聚丙烯蜂窝膜驻极体的压电性 总被引:1,自引:0,他引:1
研究了两种商用聚丙烯蜂窝膜(PPCellular)(EUH75和SHD50)的压电性.通过热膨胀技术处理测得上述两种商品膜的压电d33系数分别可达219pC/N和196pC/N.它们比未经处理的样品提高了约两个数量级,而比著名的铁电聚合物PVDF高出一个数量级以上.在强介电气体六氟化硫(SF6)中用高达60kV的电晕电压对EUH75和SHD50样品充电后,讨论了对其压电d33系数的影响的明显差异及其差异的结构根源.关键词:PP蜂窝膜压电性热膨胀技术介电气体 相似文献
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Sunanda Kakroo Arvind Kumar S.K. Mishra Vijay Singh Pramod K. Singh 《Phase Transitions》2016,89(3):211-220
In the present work, lead-free piezoelectric ceramics (Na0.5Bi0.5)TiO3 –xCuO–yNiO (for x = 0.0, 0.02, 0.04 and 0.06) have been prepared by a conventional solid-state reaction method. An investigation of CuO and NiO doping in bismuth sodium titanate (BNT) and a study of the structure, morphology, and dielectric and ferroelectric properties of the NBT–CuNi system have been conducted. Phase and microstructural analysis of the (Na0.5Bi0.5)TiO3 (NBT) based ceramics has been carried out using X-ray diffraction and scanning electron microscopy (SEM) techniques. Field emission scanning electron microscopy (FE-SEM) images showed that inhibition of grain growth takes place with increasing Cu and Ni concentration. The results indicate that the co-doping of NiO and CuO is effective in improving the dielectric and ferroelectric properties of NBT ceramics. Temperature-dependent dielectric studies have also been carried out at room temperature to 400 °C at different frequencies. The NBT ceramics co-doped with x = 0.06 and y = 0.06 exhibited an excellent dielectric constant ?r = 1514. The study suggests that there is enormous scope of application of such materials in the future for actuators, ultrasonic transducers and high-frequency piezoelectric devices. 相似文献
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聚丙烯蜂窝膜驻极体压电系数的测量及压电性的改善 总被引:3,自引:0,他引:3
利用介电谐振谱分析了聚丙烯蜂窝状原生膜(PPCellular,PQ50型)的力学及介电参数,测得其压电系数d33约为18pC/N.经合理的压力膨化工艺处理后,其d33可增加至367pC/N,比久负盛名的铁电聚合物聚偏氟乙烯(PVDF)的d33高20倍以上,也高于压电陶瓷锆钛酸铅(PZT)的相应值.结合扫描电镜照片及根据PP蜂窝膜压电理论模型分析了这类空间电荷型非极性孔洞薄膜驻极体呈现高压电系数的结构和物理根源.关键词:聚丙烯蜂窝膜压电性介电谐振压力膨化处理 相似文献
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Multiferroic properties in a polycrystalline terbium orthoferrite are investigated. Different thermomagnetic behaviors are observed in different magnetic fields, which is attributed to the suppression of the low temperature magnetic phase by an external magnetic field. Further studies reveal that the ferroelectricity originates from the spin configuration below3.5 K. In addition, the magnetic field control of electric polarization and dielectric constant is observed, which suggests a magnetoelectric effect in TbFeO3. The origin of ferroelectricity in this rare-earth orthoferrite is discussed. 相似文献
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A phenomenological Landau–Devonshire theory is developed to investigate the ferroelectric, dielectric, and piezoelectric properties of(110) oriented Pb(Zr_(1-x)Ti_x)O_3(x = 0.4, 0.5, 0.6, and 0.7) thin films. At room temperature, the tetragonal a_1 phase, the orthorhombic a_2c phase, the triclinic γ_1 phase, and the triclinic γ_2 phase are stable. The appearance of the negative polarization component P_2 in the a_2c phase and the γ_1 phase is attributed to the nonlinear coupling terms in the thermodynamic potential. The γ phase of the Pb(Zr_(1-x)Ti_x)O_3 thin films has better dielectric and piezoelectric properties than the a_2c phase and the a_1 phase. The largest dielectric and piezoelectric coefficients are obtained in the Pb(Zr_(0.5)Ti_(0.5))O_3 thin film. The piezoelectric coefficient of 110–150 pm/V is obtained in the(110) oriented Pb(Zr_(0.5)Ti_(0.5))O_3 thin film, and the Pb(Zr_(0.3)Ti_(0.7))O_3 thin film has the remnant polarization and relative dielectric constant of 50 μC/cm~2 and 100, respectively,which are in agreement with the experimental measurements reported in the literature. 相似文献
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采用改良的固相烧结工艺制备了Bi5-xPrxFe0.5Co0.5Ti3O15(BPFCT-x,x=0.25,0.50,0.75,0.80)陶瓷样品.X射线衍射结构分析表明:镨(Pr)含量对样品微观结构产生了影响,但所有样品均为层状钙钛矿结构;BPFCT-x样品的剩余极化强度(2Pr)随着掺杂量的增加呈现出先增大后减小的变化趋势,当Pr含量为0.75时,样品的2Pr达到最大值,为6.43μC/cm2.样品的磁性与铁电性能具有相同的变化规律,室温下样品的剩余磁化强度(2Mr)也呈现出先增大后减小的趋势,并且也在x=0.75时达到最大为0.097 emu/g.随着Pr掺杂量增大,样品的室温下铁电和铁磁性能得到明显改善,并且当掺杂量为0.75时,样品室温多铁性最好.Pr掺杂降低了样品中的缺陷浓度,从而提高了样品铁电畴动性,这有助于提高样品铁电性能.而样品铁磁性能的改善可能与Pr对样品晶格畸变产生的影响有关. 相似文献
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The anisotropic properties of 1T- and 2H-TaS2 axe investigated by the density functional theory within the framework of full-potential linearized augmented plane wave method. The band structures of 1T- and 2H-TaS2 exhibit anisotropic properties and the calculated electronic specific-heat coefficient γ of 2H-TaS2 accords well with the existing experimental value. The anisotropic frequency-dependent dielectric functions including the effect of the Drude term are analysed, where the ε^xx(ω) spectra corresponding to the electric field E perpendicular to the z axis show excellent agreement with the measured results except for the ε1^xx(ω) of 1T-TaS2 below the energy level of 2.6 eV which is due to the lack of the enough CDW information for reference in our calculation. Furthermore, based on the values of optical effective mass ratio P of 1T and 2H phases it is found that the anisotropy in 2H-TaS2 is stronger than that in 1T-TaS2. 相似文献
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A set of two-dimensional nonlinear equations for thin electroelastic shells in vibrations with moderately large thickness-shear
deformations are obtained from the variational formulation of the three-dimensional equations of nonlinear electroelasticity
by expanding the mechanical displacement vector and the electric potential into power series in the shell thickness coordinate
and retaining lower order terms. As an example, the equations are used to study nonlinear thickness-shear vibrations of a
circular cylindrical shell driven by an electric voltage. Nonlinear amplitude-frequency behavior of electric current near
strong resonance is obtained. 相似文献