首页 | 本学科首页   官方微博 | 高级检索  
文章检索
  按 检索   检索词:      
出版年份:   被引次数:   他引次数: 提示:输入*表示无穷大
  收费全文   2篇
  免费   4篇
物理学   6篇
  2014年   1篇
  2013年   2篇
  2012年   3篇
排序方式: 共有6条查询结果,搜索用时 0 毫秒
1
1.
张炜  陈文周  孙久雨  姜振益 《中国物理 B》2013,22(1):16601-016601
A theoretical prediction of ion conductivity for solid state HfO2 is carried out in analogy to ZrO2 based on the density functional calculation. Geometric and electronic structures of pure bulks exhibit similarity for the two materials. Negative formation enthalpy and negative vacancy formation energy are found for YSH (yttria-stabilized hafnia) and YSZ (yttria- stabilized zirconia), suggesting the stability of both materials. Low activation energies (below 0.7 eV) of diffusion are found in both materials, and YSH’s is a little higher than that of YSZ. In addition, for both HfO2 and ZrO2 , the supercells with native oxygen vacancies are also studied. The so-called defect states are observed in the supercells with neutral and +1 charge native vacancy but not in the +2 charge one. It can give an explanation to the relatively lower activation energies of yttria-doped oxides and +2 charge vacancy supercells. A brief discussion is presented to explain the different YSH ion conductivities in the experiment and obtained by us, and we attribute this to the different ion vibrations at different temperatures.  相似文献   
2.
3.
The structural, elastic, phonon and electronic properties of a MnPd alloy have been investigated using the first-principles calculation. The calculated lattice constants and electronic structure agree well with the experimental results. The microscopic mechanism of the diffusionless martensitic transition from the paramagnetic B2 (PM-B2) phase to the antiferromagnetic L10 (AFM-L10) phase through the intermediate paramagnetic L10 (PM-L10 ) phase has been explored theoretically. The obtained negative shear modulus C′= (C11-C12)/2 of the PM-B2 phase is closely related to the instability of the cubic B2 phase with respect to the tetragonal distortions. The calculated phonon dispersions for the PM-L10 and AFM-L10 phases indicate that they are dynamically stable. However, the AFM-L10 phase is energetically most favorable according to the calculated total energy order, so the PM-L10 →AFM-L10 transition is caused by the magnetism rather than the electron-phonon interaction. Additionally, the AFM-L10 state is stabilized through the formation of a pseudo gap located at the Fermi level. The calculated results show that the CuAu-I type structure in the collinear antiferromagnetic state is dynamically and mechanically stable, thus is the low temperature phase.  相似文献   
4.
基于密度泛函理论(Density Functional Theory,DFT),对中性硼化铝团簇AlBn(n=2~9)的几何结构、稳定性以及红外振动光谱进行了理论研究,讨论了他们的不同点及AlB4、AlB5、AlB6和AlB7的基态构型和相对稳定性.对于中性AlBn(n=2~9)基态构型,对比讨论了其失去[AlBn+(n=2~9)]和得到[AlBn-(n=2~9)]一个电子后化学键强度的变化、掺入铝原子的影响以及团簇几何结构的演化.计算结果表明:虽然掺入Al之后,团簇的稳定性差异变小,但是硼团簇和硼化铝团簇都趋向于形成平面、准平面结构以获得更大的稳定性;硼团簇的构型对硼化铝团簇的结构和稳定性起着决定性的作用;AlB3、AlB5和AlB8更稳定;红外光谱的振动模式倾向于B原子和对称性优先的趋势.  相似文献   
5.
运用基于密度泛函理论第一性原理方法研究了MnPd从立方顺磁到四方反铁磁的相变以及其弹性性质和热力学性质等.结果表明:MnPd合金顺磁立方B2结构在施加了四方应变后,结构不稳定,会发生结构相变形成四方顺磁结构.四方顺磁相弹性稳定,然而在考虑了磁性后,反铁磁四方相比四方顺磁相能量更低,而且弹性和动力学都稳定,说明反铁磁四方相是MnPd的低温结构.从而得出MnPd合金的相变路径为两步:先发生结构相变从顺磁B2立方结构转变为顺磁四方相,再由磁性诱发相变形成反铁磁四方结构.通过准谐近似得到了摩尔比热容,德拜温度等热力学性质.  相似文献   
6.
张炜  陈文周  姜振益 《物理学报》2012,61(14):148105-148105
利用密度泛函理论的平面波赝势方法研究了IrTi合金的晶格动力学行为. 声子谱计算表明四方(L10)结构动力学不稳定,通过冷冻不稳定声子模式, 发现IrTi会发生从四方(L10)到正交的结构相变.进一步分析软模对应的原子振动, 得到了具有正交对称性,空间群为Cmmm,相对于四方(L10)相能量更低、更稳定的结构. 这种正交新相(Cmmm)弹性稳定和动力学稳定,而且其结构参数与实验上观察到的低温结构有限的晶格参数相符合,表明IrTi合金的低温相是正交结构(Cmmm). 从理论上肯定了IrTi合金立方到四方再到正交的相变机制, 解决了实验上关于相变机制和低温相结构形式的争议.  相似文献   
1
设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号