In many colloidal systems, an orientationally ordered nematic (N) phase emerges from the 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.parity breaking | twisted tactoids | geometrical anchoring | nematic-isotropic coexistence I n 1949, Onsager demonstrated theoretically that a dispersion of long rigid rods develops an organized state, a so-called nematic (N) with rods being parallel to each, once their concentration exceeds some critical value (1). This remarkable collective behavior with an establishment of nonpolar axis of alignmentn ¼ −n, called the director, stems from the molecular symmetry alone, as the only requirement of the Onsager model is that the rods do not overlap. The theory was inspired by Bernal and Fankuchen's experiments (2) on aqueous suspensions of tobacco mosaic viruses (TMV) that phase separated into an isotropic (I) phase with a relatively low concentration of TMV rods and an N phase with a high concentration of TMV. The N domains emerged as spindle-like "tactoids" (3, 4) with the axes of rods following the meridians of the spindles. Besides TMV dispersions (2, 5), the N tactoids have been experimentally documented in water dispersions of many other materials, such as vanadium pentoxide (3, 4, 6, 7), bohemite rods (8), fd viruses (9, 10), f-actin (11), carbon nanotubes (12), as well as in lyotropic chromonic liquid crystals (LCLCs) (13,14).Reversible chromonic assembly and ensuing LCLC mesomorphism is displayed broadly by dyes, drugs (15-18), nucleotides (19,20), and DNA oligomers (21,22). Typically, the LCLC molecule is plank-like with aromatic cores and peripheral polar groups. In water, the polyaromatic cores stack face-to-face, forming elongated charged aggregates. The aggregates, self-assembled through weak noncovalent interactions, are polydisperse, with the length distribution that depends on concentration, temperature, ionic strength, and presence of crowding agents. At low concentrations, the aggregates are short and orient randomly. As the volume fraction increases, the aggregates elongate, multiply, and eventually some frac...