发光
光致发光
晶体结构
结晶学
化学
量子产额
手性(物理)
材料科学
光化学
对称性破坏
光电子学
物理
光学
手征对称破缺
量子力学
Nambu–Jona Lasinio模型
荧光
作者
Tao Song,Qiang Wang,Haolin Lu,Xijiao Mu,Bolong Wang,Jizhong Liu,Bo Ma,Jing Cao,Chuanxiang Sheng,Guankui Long,Qiang Wang,Shouxin Zhang
标识
DOI:10.1002/anie.202400769
摘要
Abstract Generating circularly polarized luminescence (CPL) with simultaneous high photoluminescence quantum yield (PLQY) and dissymmetry factor ( g lum ) is difficult due to usually unmatched electric transition dipole moment ( μ ) and magnetic transition dipole moment ( m ) of materials. Herein we tackle this issue by playing a “cascade cationic insertion” trick to achieve strong CPL (with PLQY of ~100 %) in lead‐free metal halides with high g lum values reaching −2.3×10 −2 without using any chiral inducers. Achiral solvents of hydrochloric acid (HCl) and N, N ‐dimethylformamide (DMF) infiltrate the crystal lattice via asymmetric hydrogen bonding, distorting the perovskite structure to induce the “intrinsic” chirality. Surprisingly, additional insertion of Cs + cation to substitute partial (CH 3 ) 2 NH 2 + transforms the chiral space group to achiral but the crystal maintains chiroptical activity. Further doping of Sb 3+ stimulates strong photoluminescence as a result of self‐trapped excitons (STEs) formation without disturbing the crystal framework. The chiral perovskites of indium‐antimony chlorides embedded on LEDs chips demonstrate promising potential as CPL emitters. Our work presents rare cases of chiroptical activity of highly luminescent perovskites from only achiral building blocks via spontaneous resolution as a result of symmetry breaking.
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