Inspired by the elegance and complexity of natural helical assemblies, from the nanoscopic DNA double helix and collagen triple helix to microscopic viruses and macroscopic sea shells, chemists have been trying to mimic the structure and functions of biological macromolecules in self-assembled synthetic molecules. [1][2][3][4][5][6][7] The most challenging task in these studies is the control of the overall morphology and the supramolecular chirality of the selfassembled architectures within the nanometer-to-micrometer length scale.[8] Although a few reports on reversible morphology transitions caused by external stimuli have appeared, [9] a spherical-to-helical change induced by a cation was previously unknown. However, in an interesting report Nolte and co-workers described the loss of helicity in a phthalocyanine-derived self-assembly in the presence of potassium ions.[10] Herein we report an unprecedented self-assembly of tripodal squaraine dyes, which form vesicular structures upon evaporation of the solvent from a solution of the dye and helical architectures through the expression of molecular chirality into supramolecular helicity upon a specific cation binding. [11] The supramolecular chemistry of functional dyes is at center stage in the "bottom-up" creation of nanoarchitectures.[12] Squaraines, a class of zwitterionic dyes, are well known for their tendency to form aggregates under the influence of certain solvent mixtures and cations. [13,14] Although these dyes have been studied extensively owing to their fundamental and technological significance, they are rarely exploited for the crafting of supramolecular architectures. The propensity of these dyes to aggregate to form hierarchical assemblies could be enhanced by confining the chromophores to an aromatic platform, thereby making interchromophore interaction possible. As a proof of principle of this hypothesis, we designed the three tripodal squaraines 1 a-c, which we then synthesized by the reaction of 1,3,5-tris(2-(N-methyl-N-phenylamino)ethoxy)benzene with the corresponding N,N-(dialkylaminophenyl)-4-hydroxycyclobut-3-ene-1,2-dione and characterized by spectral analysis. The UV/Vis spectra of these dyes show strong absorption but weak emission. For example, 1 c has an absorption maximum in chloroform at 647 nm (6.2 10 À7 m, e 651 nm = 8.9 10 5 m À1 cm À1 ) with a shoulder at 617 nm, whereas in acetonitrile, in addition to the l max absorption at 651 nm (8.3 10 À7 m, e 651 nm = 2.5 10 5 m À1 cm À1 ) and the shoulder at 614 nm, another band was observed at 578 nm. The emission maximum of 1 c when excited at 570 nm in chloroform or acetonitrile occurred at 662 and 663 nm with quantum yields of 0.01 and 0.004, respectively (relative to bis(4-(dimethylamino)phenyl)squaraine in chloroform as the standard). These observations support intramolecular chromophore interaction in acetonitrile and the consequent exciton coupling of the confined chromophores. [15] The absorption spectra of 1 a-c in acetonitrile-water mixtures of different compositions showed ...