Abstract

AbstractA pair of zero‐dimensional lead‐free chiral perovskites is introduced towards the detection of circularly polarized light (CPL). Although spin‐polarized carriers are generated in the perovskites under the CPL, the absorption anisotropy remained low leading to mostly similar density of photogenerated carriers under the two CPLs. Interestingly, due to the intrinsic chirality in the perovskites, they exhibited chirality‐induced spin‐selectivity (CISS) allowing the transport of only one type of spin‐half states. A high anisotropy in photocurrent along the out‐of‐plane direction has therefore appeared resulting in a spin‐dependent photovoltaic effect in vertical heterojunction devices and making them suitable for CPL detection. While a self‐powered CPL detector showed a limited (but one of the highest to date) anisotropy factor of 0.3 due to possible spin‐flips during the transport process, the factor rose to 0.6 under bias prompting extension of the effective spin‐diffusion length.

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