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Atomic displacement parameters, vibrational spectra and thermodynamic functions for crystals: a strong connection

机译:晶体的原子位移参数,振动光谱和热力学功能:强大的连接

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In crystallography, atomic motion is usually accounted for by considering the Fourier transform of the probability density function (pdf) of an atom around its mean position, which is often called a "temperature factor". For "anisotropic" displacement, such "temperature factors" T_i(hkl) can be written as. T_i(h) chemical bounds exp(-2 #pi# ~2H~TUH) where the U's (chemical bounds u_iu_j>) are second-rank tensors and are called anisotropic atomic displacement parameters or ADP's and H is the reciprocal-lattice vector referred to a set of Cartesian axes, or (more frequently) to a set of reference axes of unit length cinciding in direction with the reciprocal axes. There are also more complex forulations, involving higher temrs in the cumulant expansion, leading to higher-rank tensors (see, for instance, Johnson [22-24]).
机译:在晶体中,通常考虑其围绕其平均位置周围的原子的概率密度函数(PDF)的傅里叶变换来占原子动作,这通常被称为“温度因数”。对于“各向异性”位移,可以写入这样的“温度因子”T_I(HKL)。 T_I(h)化学界限Exp(-2#pi#〜2h〜tuh),其中U's(化学界限U_IU_J>)是第二级张量,称为各向异性原子位移参数或ADP和H是所提到的互核 - 晶格矢量到一组笛卡尔轴,或(更频繁地)到与互易轴线的方向沿着沿着往复轴的一组单元长度的参考轴。还有更复杂的缩写,涉及累积膨胀中的更高温度,导致较高级别的张量(例如,参见,例如,约翰逊[22-24])。

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