面心立方晶格

相同条件下体心立方金属的塑性高于面心立方金属，其屈服强度和初始弹性模量均低于面心立方晶格金属，但屈服阶段早于面心立方晶格金属出现，持续时间更长。

The plasticity of nano BCC metals is stronger than that of FCC metals , but yielding strength and modulus of elasticity are lower than that of FCC metals .

面心立方晶格第一布里渊区的三维动画模拟

Simulation of face-centered cubic lattice 's First Brillouin zone with 3-dimensional animation

Fe在Pt层中扩散形成Fe3PtC相，Cu在Pt中扩散形成的新相为面心立方晶格，晶格常数为3.8278×10~（-10）m，可能为Cu3Pt相。

Fe_3PtC phase is formed in Fe after diffusing in Pt layer , which a new phase is formed in Cu , that is Cu_3Pt phase with fee and the lattice constant 3.8278 × 10 ~ ( - 10 ) m after diffusing in Pt layer .

面心立方晶格的非简谐效应

The anharmonic effect of the face-centred cubic lattice

D晶格证明是面心立方晶格，并揭示了D格点的空间分布规律。

A face-centered cubic lattice . The space distribution law of D lattice point is revealed .

计算结果表明，在简单立方晶格和面心立方晶格中都能够实现全光子带隙，这在各向同性介质球时是不存在的。

Our results demonstrate that complete PBGs can be found in both fcc and sc lattice structures which are absent in PCs composed of isotropic dielectric spheres .

In熔体黏度的异常转变可能是因为在熔点以上的低温区液态In的结构类似面心立方晶格，随着温度升高转变为无规密堆结构所致。

It is considered that the abnormal change of In melt is possibly due to the transition from resembling face centered cubic lattice at low temperature to random close-packed structure at high temperature .

用简单数学方法就体心立方晶格和面心立方晶格证明了三维情况下布里渊区体积等于倒格子原胞体积。

It is proved that the volume of Brillouin zone and that of the reciprocal lattice primitive cell are equal for bcc lattice and fcc lattice in three dimensions by a simple mathematical method .

用该表达式计算了C（60）分别为面心立方和六方晶格时晶体的结合能，讨论了不同晶格的稳定性问题，解释了C（60）晶体一般是面心立方的原因。

The binding energy of face-centered cubic lattice and hexagonal lattice for C_ ( 60 ) crystal was calculated by using the analytic interaction potential , the stability of different lattice was discussed and the reason why C_ ( 60 ) is general face-centered cubic lattice was explained .