Peter K. Morse, Paul J. Steinhardt, Salvatore Torquato
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引用次数: 0
摘要
先前的工作[Phys. Rev. X 5, 021020 (2015)]表明,隐身超均匀系统可被视为傅里叶空间的硬球,即在原点周围的球形区域中,结构因子恰好为零,这与现实空间硬球的对相关函数类似。早先的研究集中于空间维度 d=1-4,而在这里我们将分析扩展到更高的维度,以便与高维球体堆积和玻璃均场理论建立联系。我们利用这种对应关系证实了最致密的傅立叶空间硬球系统是布拉维晶格系统,而不是实空间硬球,后者的最致密构型被猜测为无序的。我们顺便给出了第一个布拉格峰位置的简明形式。我们还将之前提出的无序隐形超均匀系统的病毒序列扩展到更高维度,以预测空间不相关性是维度的函数。这一预测随后被维数为 d=2-8 的无序隐身超均匀基态的数值模拟所证实,由于采用了高度并行化的算法,这一模拟最近才得以实现。
Ordered and disordered stealthy hyperuniform point patterns across spatial dimensions
In previous work [Phys. Rev. X5, 021020 (2015)] it was shown that stealthy hyperuniform systems can be regarded as hard spheres in Fourier space in the sense that the structure factor is exactly zero in a spherical region around the origin in analogy with the pair-correlation function of real-space hard spheres. While this earlier work focused on spatial dimensions , here we extend the analysis to higher dimensions in order to make connections to high-dimensional sphere packings and the mean-field theory of glasses. We exploit this correspondence to confirm that the densest Fourier-space hard-sphere system is that of a Bravais lattice in contrast to real-space hard spheres, whose densest configuration is conjectured to be disordered. In passing, we give a concise form for the position of the first Bragg peak. We also extend the virial series previously suggested for disordered stealthy hyperuniform systems to higher dimensions in order to predict spatial decorrelation as a function of dimension. This prediction is then borne out by numerical simulations of disordered stealthy hyperuniform ground states in dimensions , which have only recently been made possible due to a highly parallelized algorithm.