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The use of symmetrized valence and relative motion coordinates for crystal potentials

机译:使用对称化合价和相对运动坐标的晶体电位

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摘要

Symmetrized valence coordinates are linear combinations of conventional valence coordinates which display the symmetry of a set of atoms bound by the valence bonds. Relative motion coordinates are relative translations, or relative rotations, of two or more strongly bonded groups of atoms among which relatively weak forces act. They are useful for expressing interactions between molecules in molecular crystals and should be chosen, also, to reflect the symmetry of the interacting groups. Since coordinates defined by these procedures possess elements of symmetry in common with the bonding electron distributions, the force constants in the potential should be more amenable to calculation in terms of energy changes in the electronic ground state which accompany displacements of the atoms from equilibrium. It is easier to determine force constants for fitting experimental data because interaction constants coupling coordinates of unlike symmetry with regard to the crystal point group are necessarily zero. They may be small, also, for coordinates which belong to different representations of the local symmetry when this is not the same as for the crystal. Procedures are given for defining the coordinates, and for assuring that the potential energy is invariant to crystal translations and rotations. The secular equation is derived by expressing the kinetic and potential energies in terms of components of mass adjusted basis vectors which are chosen so that high and low frequency modes can be separated approximately. The necessity to remove redundancies among the coordinates in the potential is avoided. The Journal of Chemical Physics is copyrighted by The American Institute of Physics.
机译:对称的化合价坐标是常规化合价坐标的线性组合,显示了由化合价键结合的一组原子的对称性。相对运动坐标是两个或更多个强键原子组的相对平移或相对旋转,其中相对弱的力起作用。它们可用于表达分子晶体中分子之间的相互作用,因此也应选择它们以反映相互作用基团的对称性。由于由这些过程定义的坐标具有与键合电子分布相同的对称元素,因此电势中的力常数应更适合根据电子基态中的能量变化(伴随着原子从平衡中的位移)进行计算。确定适合实验数据的力常数更容易,因为相互作用常数耦合相对于晶点组的对称性不同的坐标必须为零。当与晶体不同时,对于属于局部对称性的不同表示的坐标,它们也可能很小。给出了定义坐标的程序,并确保了势能对于晶体平移和旋转是不变的。通过用质量调整后的基矢量的分量表示动能和势能,可以推导出长期方程。避免了去除电位中的坐标之间的冗余的必要性。 《化学物理学杂志》的版权归美国物理学会所有。

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