Strong Second- and Third-Harmonic Generation in 1D Chiral Hybrid Bismuth Halides

Breaking the symmetry of a crystal structure can enable even-order nonlinear activities, including second-harmonic generation (SHG). The emerging chiral hybrid organic–inorganic metal halides feature unique optical and electronic properties and flexible crystal structures, making them a class of pro...

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Veröffentlicht in:Journal of the American Chemical Society 2021-10, Vol.143 (39), p.16095-16104
Hauptverfasser: Yao, Li, Zeng, Zhouxiaosong, Cai, Chengkun, Xu, Peng, Gu, Honggang, Gao, Liang, Han, Junbo, Zhang, Xiaowei, Wang, Xi, Wang, Xiao, Pan, Anlian, Wang, Jian, Liang, Wenxi, Liu, Shiyuan, Chen, Chao, Tang, Jiang
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container_end_page 16104
container_issue 39
container_start_page 16095
container_title Journal of the American Chemical Society
container_volume 143
creator Yao, Li
Zeng, Zhouxiaosong
Cai, Chengkun
Xu, Peng
Gu, Honggang
Gao, Liang
Han, Junbo
Zhang, Xiaowei
Wang, Xi
Wang, Xiao
Pan, Anlian
Wang, Jian
Liang, Wenxi
Liu, Shiyuan
Chen, Chao
Tang, Jiang
description Breaking the symmetry of a crystal structure can enable even-order nonlinear activities, including second-harmonic generation (SHG). The emerging chiral hybrid organic–inorganic metal halides feature unique optical and electronic properties and flexible crystal structures, making them a class of promising nonlinear optical materials. However, their nonlinear response performances are currently inferior to traditional nonlinear crystals, because of the lack of research on resonant enhancement and third-harmonic generation (THG). Herein, we designed chiral hybrid bismuth halides with naturally nonsymmetrical structure to enable SHG. Simultaneously, these chiral compounds preserve 1D crystal structures to create strong free exciton, broad self-trapped exciton (STE), and discrete band energy levels, which facilitate the resonant enhancement of SHG and THG susceptibilities. These new chiral films showcase superior effective SHG susceptibility (χ(2) ∼ 130.5 pm V–1 at an interesting wavelength of 1550 nm), exceeding that of the reference, a commercial LiNbO3 (χ(2) ∼ 83.4 pm V–1) single-crystal film. Furthermore, their THG intensities are even higher than their SHG intensities, with effective THG susceptibility (χ(3)) being ∼9.0 × 106 pm2 V–2 at 1550 nm (37 times that of the reference monolayer WS2). Their high SHG and THG performances indicate the promising future of these 1D chiral hybrid bismuth halides toward nonlinear optical applications.
doi_str_mv 10.1021/jacs.1c06567
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The emerging chiral hybrid organic–inorganic metal halides feature unique optical and electronic properties and flexible crystal structures, making them a class of promising nonlinear optical materials. However, their nonlinear response performances are currently inferior to traditional nonlinear crystals, because of the lack of research on resonant enhancement and third-harmonic generation (THG). Herein, we designed chiral hybrid bismuth halides with naturally nonsymmetrical structure to enable SHG. Simultaneously, these chiral compounds preserve 1D crystal structures to create strong free exciton, broad self-trapped exciton (STE), and discrete band energy levels, which facilitate the resonant enhancement of SHG and THG susceptibilities. These new chiral films showcase superior effective SHG susceptibility (χ(2) ∼ 130.5 pm V–1 at an interesting wavelength of 1550 nm), exceeding that of the reference, a commercial LiNbO3 (χ(2) ∼ 83.4 pm V–1) single-crystal film. Furthermore, their THG intensities are even higher than their SHG intensities, with effective THG susceptibility (χ(3)) being ∼9.0 × 106 pm2 V–2 at 1550 nm (37 times that of the reference monolayer WS2). 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