Abstract
Six-dimensional hard hypersphere systems in the A6, D6, and E6 crystalline phases have been studied using event-driven molecular dynamics simulations in periodic, skew cells that reflect the underlying lattices. In all the simulations, the systems had sufficient numbers of hyperspheres to capture the first coordination shells, and the larger simulations also included the complete second coordination shell. The equations of state, for densities spanning the fluid, metastable fluid, and solid regimes, were determined. Using molecular dynamics simulations with the hyperspheres tethered to lattice sites allowed the computation of the free energy for each of the crystal lattices relative to the fluid phase. From these free energies, the fluid-crystal coexistence region was determined for the E6, D6, and A6 lattices. Pair correlation functions for all the examined states were computed. Interestingly, for all the states examined, the pair correlation functions displayed neither a split second peak nor a shoulder in the second peak. These behaviors have been previously used as a signature of the freezing of the fluid phase for hard hyperspheres in two to five dimensions.
Highlights
Research into systems in arbitrary spatial dimensions is an active area of inquiry in a variety of fields
This paper extends earlier work that reported on six dimensional Monte Carlo (MC) and molecular dynamics (MD) calculations in the fluid and high density metastable regimes25,26
The simulations were performed in skew boxes, with the edges aligned with basis vectors of the lattice under examination; this allows for a much wider range of system sizes to be explored compared to restricting the box to be hypercubic or hyperrectagular
Summary
Research into systems in arbitrary spatial dimensions is an active area of inquiry in a variety of fields. In most previous work on higher dimension hard hypersphere systems, the simulations are performed in periodic boxes where the sides of the primary simulation cell are orthogonal This severely restricts the system sizes (i.e. the number of hyperspheres in the system) for a particular lattice type. We perform simulations for different six dimensional hard hypersphere crystals in skew periodic boxes, where the edges are aligned with the basis vectors of the lattice. This allows the analysis of a wider range of distinct system sizes for a given lattice.
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