发光
材料科学
钙钛矿(结构)
纳米晶
激发
自旋(空气动力学)
异质结
吸收(声学)
光电子学
超快激光光谱学
圆极化
光谱学
人口
自旋态
分子物理学
受激发射
飞秒
化学物理
自旋电子学
光抽运
吸收光谱法
凝聚态物理
发射光谱
光化学
结晶学
自旋扩散
纳米技术
作者
Xingyu Zhang,Honghan Ji,Jieyu Tang,Houchao Jing,Tianyong Zhang,Pengfei Duan,Shuang Jiang,Xue Jin
摘要
ABSTRACT Chiral perovskites enable spin‐polarized light emission through the chiral‐induced spin selectivity (CISS) effect, offering a pathway toward magnet‐free spin‐optoelectronic devices. However, in most CISS‐based luminescent systems, the spin‐filtering and light‐emitting functions are intrinsically coupled, which obscures the independent role of spin injection in modulating emission and precludes a clear mechanistic understanding. Here, a core–shell chiral perovskite nanocrystal system consisting of an achiral MAPbI 3 core and a two‐dimensional chiral perovskite shell based on R / S ‐1‐(2‐naphthyl)ethylamine (NEA) is reported. This heterostructure enables excitation‐wavelength‐controlled spin injection. Owing to the strong absorption of the chiral shell at 375 nm and its transparency at 532 nm, 375 nm excitation activates a CISS‐mediated shell‐to‐core spin‐polarized carrier injection pathway, whereas 532 nm excitation mainly populates the MAPbI 3 core directly. This optical switching of the injection pathway boosts the circularly polarized luminescence (CPL) dissymmetry factor ( g lum ) from 1.5 × 10 −3 (532 nm excitation) to 3.8 × 10 −3 (375 nm excitation). In parallel, the magnetic conductive‐probe atomic force microscopy (mCP‐AFM) measurements reveal up to 85% spin polarization, and transient absorption spectroscopy shows a distinct 48 ps shell‐mediated population transfer component. These findings establish that CISS‐mediated spin injection can be optically controlled by excitation wavelength, enabling wavelength‐addressable spin manipulation in chiral heterostructures.
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