TY - JOUR
T1 - Molecular dynamics study of six-dimensional hard hypersphere crystals
AU - Lue, Leo
AU - Bishop, Marvin
AU - Whitlock, Paula A.
PY - 2021/10/11
Y1 - 2021/10/11
N2 - 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.
AB - 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.
KW - spatial dimensions
KW - cyrstal lattices
KW - hypersphere crystals
KW - molecular dynamics
UR - https://aip.scitation.org/journal/jcp
U2 - 10.1063/5.0066421
DO - 10.1063/5.0066421
M3 - Article
SN - 0021-9606
VL - 155
JO - Journal of Chemical Physics
JF - Journal of Chemical Physics
IS - 14
M1 - 144502
ER -