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Lattice sums and their phase diagram implications for the classical Lennard-Jones model

机译:格点求和及其相图对经典Lennard-Jones模型的影响

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High-accuracy lattice sums have been evaluated for the Lennard-Jones 12-6 pair potential, without cutoffs, in the close-packed fcc and hcp lattices. The results confirm the small relative stability of hcp at low pressure, and locate precisely the first-order phase transition at zero temperature to the fcc structure. The reduced pressure p #sigma#~3/#epsilon# at this transition is approximately 878.476…, with both structures having been compressed to about one-half of their zero-pressure volumes. On account of its lower symmetry compared to fcc, the hcp lattice spontaneously distorts from the ideal close-packed geometry to lower its energy by a tiny amount. For low compressions, this distortion involves expansion within close-packed planes, and shrinkage in the prependicular stacking direction. However this spontaneous distortion changes sign shortly before reaching the compression required for the hcp-fcc phase transition, vanishing at a volume ratio (compared to zero pressure) of about 0.537.
机译:在紧密堆积的fcc和hcp晶格中,对Lennard-Jones 12-6对电位的高精度晶格和进行了评估,没有截断。结果证实在低压下hcp的相对稳定性较小,并且精确地确定了零温度下fcc结构的一阶相变。在该过渡处的减压p#sigma#〜3 / epsilon#大约为878.476…,两个结构都被压缩到其零压力体积的大约一半。由于与fcc相比对称性较低,hcp晶格自发地从理想的密排几何结构中变形,从而将其能量降低了极少。对于低压缩,此变形包括在密排平面内的膨胀以及在垂直堆积方向上的收缩。但是,这种自发的变形会在达到hcp-fcc相变所需的压缩之前不久发生变化,并以约0.537的体积比(与零压力相比)消失。

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