TY - JOUR
T1 - Stimulating and Manipulating Robust Circularly Polarized Photoluminescence in Achiral Hybrid Perovskites
AU - Zhan, Guixiang
AU - Zhang, Junran
AU - Zhang, Linghai
AU - Ou, Zhenwei
AU - Yang, Hongyu
AU - Qian, Yuchi
AU - Zhang, Xu
AU - Xing, Ziyue
AU - Zhang, Le
AU - Li, Congzhou
AU - Zhong, Jingxian
AU - Yuan, Jiaxiao
AU - Cao, Yang
AU - Zhou, Dawei
AU - Chen, Xiaolong
AU - Ma, Huifang
AU - Song, Xuefen
AU - Zha, Chenyang
AU - Huang, Xiao
AU - Wang, Jianpu
AU - Wang, Ti
AU - Huang, Wei
AU - Wang, Lin
N1 - Publisher Copyright:
© 2022 American Chemical Society. All rights reserved.
PY - 2022/5/25
Y1 - 2022/5/25
N2 - Circularly polarized light (CPL) is essential for optoelectronic and chiro-spintronic applications. Hybrid perovskites, as star optoelectronic materials, have demonstrated CPL activity, which is, however, mostly limited to chiral perovskites. Here, we develop a simple, general, and efficient strategy to stimulate CPL activity in achiral perovskites, which possess rich species, efficient luminescence, and tunable bandgaps. With the formation of van der Waals heterojunctions between chiral and achiral perovskites, a nonequilibrium spin population and thus CPL activity are realized in achiral perovskites by receiving spin-polarized electrons from chiral perovskites. The polarization degree of room-temperature CPL in achiral perovskites is at least one order of magnitude higher than in chiral ones. The CPL polarization degree and emission wavelengths of achiral perovskites can be flexibly designed by tuning chemical compositions, operating temperature, or excitation wavelengths. We anticipate that unlimited types of achiral perovskites can be endowed with CPL activity, benefiting their applications in integrated CPL sources and detectors.
AB - Circularly polarized light (CPL) is essential for optoelectronic and chiro-spintronic applications. Hybrid perovskites, as star optoelectronic materials, have demonstrated CPL activity, which is, however, mostly limited to chiral perovskites. Here, we develop a simple, general, and efficient strategy to stimulate CPL activity in achiral perovskites, which possess rich species, efficient luminescence, and tunable bandgaps. With the formation of van der Waals heterojunctions between chiral and achiral perovskites, a nonequilibrium spin population and thus CPL activity are realized in achiral perovskites by receiving spin-polarized electrons from chiral perovskites. The polarization degree of room-temperature CPL in achiral perovskites is at least one order of magnitude higher than in chiral ones. The CPL polarization degree and emission wavelengths of achiral perovskites can be flexibly designed by tuning chemical compositions, operating temperature, or excitation wavelengths. We anticipate that unlimited types of achiral perovskites can be endowed with CPL activity, benefiting their applications in integrated CPL sources and detectors.
KW - chiral/achiral perovskite
KW - circularly polarized light
KW - heterostructure
KW - spin-polarization
UR - http://www.scopus.com/inward/record.url?scp=85130006483&partnerID=8YFLogxK
U2 - 10.1021/acs.nanolett.2c00482
DO - 10.1021/acs.nanolett.2c00482
M3 - 文章
C2 - 35507685
AN - SCOPUS:85130006483
SN - 1530-6984
VL - 22
SP - 3961
EP - 3968
JO - Nano Letters
JF - Nano Letters
IS - 10
ER -