Chiral symmetry breaking by spatial confinement in tactoidal droplets of lyotropic chromonic liquid crystals

被引:149
|
作者
Tortora, Luana [1 ]
Lavrentovich, Oleg D. [1 ,2 ]
机构
[1] Kent State Univ, Inst Liquid Crystal, Kent, OH 44242 USA
[2] Kent State Univ, Chem Phys Interdisciplinary Program, Kent, OH 44242 USA
基金
美国国家科学基金会;
关键词
parity breaking; twisted tactoids; geometrical anchoring; nematic-isotropic coexistence; NEMATIC TACTOIDS; LIGHT-SCATTERING; PHASE-SEPARATION; PARITY-BREAKING; DEFECTS; MODEL; CONDENSATION; TRANSITION; MESOPHASES; MOLECULES;
D O I
10.1073/pnas.1100087108
中图分类号
O [数理科学和化学]; P [天文学、地球科学]; Q [生物科学]; N [自然科学总论];
学科分类号
07 ; 0710 ; 09 ;
摘要
In many colloidal systems, an orientationally ordered nematic (N) phase emerges fromthe isotropic (I) melt in the form of spindle-like birefringent tactoids. In cases studied so far, the tactoids always reveal a mirror-symmetric nonchiral structure, sometimes even when the building units are chiral. We report on chiral symmetry breaking in the nematic tactoids formed in molecularly nonchiral polymer-crowded aqueous solutions of low-molecular weight disodium cromoglycate. The parity is broken by twisted packing of self-assembled molecular aggregates within the tactoids as manifested by the observed optical activity. Fluorescent confocal microscopy reveals that the chiral N tactoids are located at the boundaries of cells. We explain the chirality induction as a replacement of energetically costly splay packing of the aggregates within the curved bipolar tactoidal shape with twisted packing. The effect represents a simple pathway of macroscopic chirality induction in an organic system with no molecular chirality, as the only requirements are orientational order and curved shape of confinement.
引用
收藏
页码:5163 / 5168
页数:6
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