Homochirality to design high-Tc lead-free ferroelastic semiconductors

Ferroelastic semiconductor materials have garnered significant research interest due to their promising applications in the fields of shape memory, superelasticity, templated electronic nanostructures, mechanical switching, and optoelectronic transmission. However, the toxicity of lead-based structu...

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Veröffentlicht in:Journal of materials chemistry. C, Materials for optical and electronic devices Materials for optical and electronic devices, 2024-05, Vol.12 (17), p.6098-6105
Hauptverfasser: Bo-Wen, Deng, Zhi-Peng, Rao, Ming-Jing, Shen, Ke-Wei, Liang, Zhu, Yang, Wang, Zhi-Jie, Ding, Kun, Chang-Yuan, Su, Meng-Meng Lun, Zhi-Xu, Zhang, Zhang, Yi, Da-Wei, Fu
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container_issue 17
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container_title Journal of materials chemistry. C, Materials for optical and electronic devices
container_volume 12
creator Bo-Wen, Deng
Zhi-Peng, Rao
Ming-Jing, Shen
Ke-Wei, Liang
Zhu, Yang
Wang, Zhi-Jie
Ding, Kun
Chang-Yuan, Su
Meng-Meng Lun
Zhi-Xu, Zhang
Zhang, Yi
Da-Wei, Fu
description Ferroelastic semiconductor materials have garnered significant research interest due to their promising applications in the fields of shape memory, superelasticity, templated electronic nanostructures, mechanical switching, and optoelectronic transmission. However, the toxicity of lead-based structures and low phase-transition temperature (Tc) greatly constrain the application scenarios of ferroelastic semiconductors. Here, using an H/OH-substitution-induced homochiral strategy, we synthesize a pair of lead-free ferroelastic semiconductors (R/S-CTA)2SbCl5 (CTA = 3-chloro-2-hydroxypropyltrimethyllammonium) having semiconductor properties with an indirect bandgap of 3.41 eV. They crystallized in the chiral space group P212121 at room temperature, and both undergo 422F222 type ferroelastic phase transitions with Tc up to 410 K, accompanied by a large entropy change of 68.75 and 66.09 J mol−1 K−1, respectively. Owing to the introduction of chirality, they exhibited temperature-dependent nonlinear second-harmonic generation (SHG) properties. Relatively, the achiral TMCP (TMCP = N,N,N-trimethylchloropropylamine) makes the phase transition properties of centrosymmetric TMCP2SbCl5 ordinary compared to chiral R/S-pair. This is precisely the main starting point of homochiral strategies in phase transition and optical structure research, while arousing research interest. This work, which provides a new avenue for the design of high-Tc lead-free ferroelastic semiconductor compounds, is a powerful motivation for the realization of multifunctional materials related to chirality.
doi_str_mv 10.1039/d4tc00428k
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source Royal Society Of Chemistry Journals 2008-
subjects Chirality
Crystallization
Lead free
Multifunctional materials
Optoelectronics
Phase transitions
Room temperature
Second harmonic generation
Semiconductor materials
Semiconductors
Shape memory
Superelasticity
Temperature dependence
Transition temperature
title Homochirality to design high-Tc lead-free ferroelastic semiconductors
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