The effect of temperature, interaction range, and pair potential on the formation of dodecagonal quasicrystals in core-corona systems
H Pattabhiraman, M Dijkstra - Journal of Physics: Condensed …, 2017 - iopscience.iop.org
Journal of Physics: Condensed Matter, 2017•iopscience.iop.org
A two-dimensional dodecagonal quasicrystal was previously reported by Dotera et al (2014
Nature 506 208) in a system of particles interacting with a hard core of diameter σ and a
repulsive square shoulder of diameter $\delta= 1.40\sigma $. In the current work, we
examine the formation of this quasicrystal using bond orientational order parameters,
correlation functions and tiling distributions. We find that this dodecagonal quasicrystal forms
from a fluid phase. We further study the effect of the width of the repulsive shoulder by …
Nature 506 208) in a system of particles interacting with a hard core of diameter σ and a
repulsive square shoulder of diameter $\delta= 1.40\sigma $. In the current work, we
examine the formation of this quasicrystal using bond orientational order parameters,
correlation functions and tiling distributions. We find that this dodecagonal quasicrystal forms
from a fluid phase. We further study the effect of the width of the repulsive shoulder by …
Abstract
A two-dimensional dodecagonal quasicrystal was previously reported by Dotera et al (2014 Nature 506 208) in a system of particles interacting with a hard core of diameter σ and a repulsive square shoulder of diameter . In the current work, we examine the formation of this quasicrystal using bond orientational order parameters, correlation functions and tiling distributions. We find that this dodecagonal quasicrystal forms from a fluid phase. We further study the effect of the width of the repulsive shoulder by simulating the system over a range of values of δ. For the range of densities and temperatures considered, we observe the formation of the dodecagonal quasicrystal between and . We also study the effect of shape of the interaction potential by simulating the system using three other interaction potentials with two length scales, namely hard-core plus a linear ramp, modified exponential, or Buckingham (exp-6) potential. We observe the presence of the quasicrystal in all three systems. However, depending on the shape of the potential, the formation of the quasicrystal takes place at lower temperatures (or higher interaction strengths). Using free-energy calculations, we demonstrate that the quasicrystal is thermodynamically stable in the square-shoulder and linear-ramp system.
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