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A Novel Chiral Phase of Achiral Hard Triangles and an Entropy-Driven Demixing of Enantiomers

机译:一种新的非手性硬三角形手性相和熵驱动的三角形   对映体的分层

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摘要

We investigate the phase behavior of a system of hard equilateral andright-angled triangles in two dimensions using Monte Carlo simulations. Hardequilateral triangles undergo a continuous isotropic-triatic liquid crystalphase transition at packing fraction $\phi=0.7$. Similarly, hard right-angledisosceles triangles exhibit a first-order phase transition from an isotropicfluid phase to a rhombic liquid crystal phase with a coexistence region $\phi\in \left[0.733,0.782\right]$. Both these liquid crystal phases undergo acontinuous phase transition to their respective close-packed crystal structuresat high pressures. Although the particles and their close-packed crystals areboth achiral, the solid phases of equilateral and right-angled trianglesexhibit spontaneous chiral symmetry breaking at sufficiently high packingfractions. The colloidal triangles rotate either in clockwise or anti-clockwisedirection with respect to one of the lattice vectors for packing fractionshigher than $\phi_\chi$. As a consequence, these triangles spontaneously form aregular lattice of left- or right-handed chiral holes which are surrounded bysix triangles in the case of equilateral triangles and four or eight trianglesfor right-angled triangles. Moreover, our simulations show a spontaneousentropy-driven demixing transition of the right- and left-handed "enantiomers".
机译:我们使用蒙特卡洛模拟研究二维的硬等边和直角三角形系统的相行为。硬等边三角形在填充分数$ \ phi = 0.7 $下经历连续的各向同性-三相液晶相变。类似地,坚硬的直角等腰三角形表现出从各向同性流体相到菱形液晶相的一阶相变,并在\ left [0.733,0.782 \ right] $中共存区域。在高压下,这两个液晶相都经历了连续的相变,过渡到它们各自的密堆积晶体结构。尽管颗粒及其紧密堆积的晶体都是非手性的,但等边三角形和直角三角形的固相在足够高的堆积分数下表现出自发的手性对称性。胶体三角形相对于用于填充高于$ \ phi_ \ chi $的分数的晶格矢量之一沿顺时针方向或逆时针方向旋转。结果,这些三角形自发地形成左旋或右旋手性孔的规则晶格,在等边三角形的情况下,它们被六个三角形包围,而对于直角三角形,则被四个或八个三角形包围。而且,我们的模拟显示了右手和左手“对映体”的自发熵驱动的混合转变。

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