“…Meanwhile, many diverse factors, such as tersolvent composition, solvent polarity, polymer molecular weight, alkyl chain length, limonene enantiopurity, solution temperature, clockwise and counter-clockwise stirring, and aggregate size are confirmed to influence the magnitude of the induced CD and/or CPL amplitude. Through theoretical calculation, they assume that the inherent twisting ability (H-H repulsion) between the near- Zhang et al demonstrated that solvent chirality can be transferred to the aggregates of many optically inactive π-conjugated polymers with different backbone structures, such as main chain azo-containing polyfluorene (F8AZO), poly(9,9-di-n-octylfluorenyl-2,7-diyl) (PF8), poly(9,9-di-noctylsila-fluorenyl-2,7-diyl) (PSi8), poly(9-(1-octylnonyl)-9H-carbazole-2,7-diyl) (PCz8), P(F8-alt-Si8), P(F8-alt-Cz8), and P(Si8-alt-Cz8), hyperbranched PF8s, side chain azo-containing polymers PAzoMA, P(AzoMA-rans-MMA), and star side-chain Azo polymers (star PAzoMAs) as shown in Figure 6 [69,[72][73][74][75][76]. Optically active F8AZO aggregates were successfully generated by the chirality transfer from (S)-and (R)-limonene, demonstrated by the intense ICD signals corresponding to F8AZO in the visible region [69].…”