发光
单体
中胚层
聚合物
材料科学
液晶
聚合
三元运算
圆二色性
手性(物理)
结晶学
液晶
化学
光电子学
物理
量子力学
手征对称破缺
复合材料
计算机科学
Nambu–Jona Lasinio模型
程序设计语言
夸克
作者
Hang Li,Jiaxin Luo,Chao Liu,Wenting Yu,Yixiang Cheng
标识
DOI:10.1002/chem.202303852
摘要
Abstract Recently, extensive works have focused on increasing the dissymmetry factors ( g lum ) of various circularly polarized luminescence (CPL) materials, which is one of the most important factors for future applications of CPL. Herein, we designed a chiral co‐assembled liquid crystal polymer (LCP) PTZ@ R/S ‐PB2 , which was prepared by chiral binary co‐polymer ( R/S ‐PB2 ) doped with achiral phenothiazine derivation dye ( PTZ ). For comparison, ternary co‐polymerized LCP ( R/S ‐PT ) was synthesized by co‐polymerizing with mesogenic monomer, chiral monomer and emissive monomer. Both PTZ@ R/S ‐PB2 and R/S ‐PT showed aggregation‐induced emission (AIE) properties. Interestingly, the CPL signals of both PTZ@ R/S ‐PB2 and R/S ‐PT were reversed and amplified after thermal annealing treatment. The | g lum | values of the co‐assembled PTZ@ R/S ‐PB2 were up to 0.13 at a 32 nm thickness, which was 5.4 times that of R/S ‐PT (| g lum |=0.024). This is due to PTZ@ R/S ‐PB2 could form more orderly chiral co‐assembly structures. Noticeably, increasing the LCP film thickness could further improve the g lum value, and the maximum g lum of PTZ@ R/S ‐PB2 could be enhanced to +0.91/−0.82 at a 220 nm thickness.
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