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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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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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.</description><identifier>ISSN: 2050-7526</identifier><identifier>EISSN: 2050-7534</identifier><identifier>DOI: 10.1039/d4tc00428k</identifier><language>eng</language><publisher>Cambridge: Royal Society of Chemistry</publisher><subject>Chirality ; Crystallization ; Lead free ; Multifunctional materials ; Optoelectronics ; Phase transitions ; Room temperature ; Second harmonic generation ; Semiconductor materials ; Semiconductors ; Shape memory ; Superelasticity ; Temperature dependence ; Transition temperature</subject><ispartof>Journal of materials chemistry. C, Materials for optical and electronic devices, 2024-05, Vol.12 (17), p.6098-6105</ispartof><rights>Copyright Royal Society of Chemistry 2024</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27923,27924</link.rule.ids></links><search><creatorcontrib>Bo-Wen, Deng</creatorcontrib><creatorcontrib>Zhi-Peng, Rao</creatorcontrib><creatorcontrib>Ming-Jing, Shen</creatorcontrib><creatorcontrib>Ke-Wei, Liang</creatorcontrib><creatorcontrib>Zhu, Yang</creatorcontrib><creatorcontrib>Wang, Zhi-Jie</creatorcontrib><creatorcontrib>Ding, Kun</creatorcontrib><creatorcontrib>Chang-Yuan, Su</creatorcontrib><creatorcontrib>Meng-Meng Lun</creatorcontrib><creatorcontrib>Zhi-Xu, Zhang</creatorcontrib><creatorcontrib>Zhang, Yi</creatorcontrib><creatorcontrib>Da-Wei, Fu</creatorcontrib><title>Homochirality to design high-Tc lead-free ferroelastic semiconductors</title><title>Journal of materials chemistry. C, Materials for optical and electronic devices</title><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.</description><subject>Chirality</subject><subject>Crystallization</subject><subject>Lead free</subject><subject>Multifunctional materials</subject><subject>Optoelectronics</subject><subject>Phase transitions</subject><subject>Room temperature</subject><subject>Second harmonic generation</subject><subject>Semiconductor materials</subject><subject>Semiconductors</subject><subject>Shape memory</subject><subject>Superelasticity</subject><subject>Temperature dependence</subject><subject>Transition temperature</subject><issn>2050-7526</issn><issn>2050-7534</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2024</creationdate><recordtype>article</recordtype><recordid>eNo9jc1KAzEURoMoWGo3PsGA62h-Z5KllGqFgpu6Lpmbm07qtKlJZuHbW1D8NueszkfIPWePnEn75FUFxpQwn1dkJphmtNNSXf-7aG_JopQDu8zw1rR2RlbrdEwwxOzGWL-bmhqPJe5PzRD3A91CM6LzNGTEJmDOCUdXaoSm4DFCOvkJasrljtwENxZc_HFOPl5W2-Wabt5f35bPG3rmRlaqVc8hGAeCWx_6FjoRRIeW6V4IzaFXAh1T2qAXPRgbpEH0nXUGeNu6Xs7Jw2_3nNPXhKXuDmnKp8vlTjJlO91xKeQPNFBOXA</recordid><startdate>20240502</startdate><enddate>20240502</enddate><creator>Bo-Wen, Deng</creator><creator>Zhi-Peng, Rao</creator><creator>Ming-Jing, Shen</creator><creator>Ke-Wei, Liang</creator><creator>Zhu, Yang</creator><creator>Wang, Zhi-Jie</creator><creator>Ding, Kun</creator><creator>Chang-Yuan, Su</creator><creator>Meng-Meng Lun</creator><creator>Zhi-Xu, Zhang</creator><creator>Zhang, Yi</creator><creator>Da-Wei, Fu</creator><general>Royal Society of Chemistry</general><scope>7SP</scope><scope>7U5</scope><scope>8FD</scope><scope>L7M</scope></search><sort><creationdate>20240502</creationdate><title>Homochirality to design high-Tc lead-free ferroelastic semiconductors</title><author>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</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-p183t-54b1cf8ac219dfb6c72f27e905b2251cb42ea0458ed2bc89f38eed79a8c166ab3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2024</creationdate><topic>Chirality</topic><topic>Crystallization</topic><topic>Lead free</topic><topic>Multifunctional materials</topic><topic>Optoelectronics</topic><topic>Phase transitions</topic><topic>Room temperature</topic><topic>Second harmonic generation</topic><topic>Semiconductor materials</topic><topic>Semiconductors</topic><topic>Shape memory</topic><topic>Superelasticity</topic><topic>Temperature dependence</topic><topic>Transition temperature</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Bo-Wen, Deng</creatorcontrib><creatorcontrib>Zhi-Peng, Rao</creatorcontrib><creatorcontrib>Ming-Jing, Shen</creatorcontrib><creatorcontrib>Ke-Wei, Liang</creatorcontrib><creatorcontrib>Zhu, Yang</creatorcontrib><creatorcontrib>Wang, Zhi-Jie</creatorcontrib><creatorcontrib>Ding, Kun</creatorcontrib><creatorcontrib>Chang-Yuan, Su</creatorcontrib><creatorcontrib>Meng-Meng Lun</creatorcontrib><creatorcontrib>Zhi-Xu, Zhang</creatorcontrib><creatorcontrib>Zhang, Yi</creatorcontrib><creatorcontrib>Da-Wei, Fu</creatorcontrib><collection>Electronics & Communications Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of materials chemistry. C, Materials for optical and electronic devices</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Bo-Wen, Deng</au><au>Zhi-Peng, Rao</au><au>Ming-Jing, Shen</au><au>Ke-Wei, Liang</au><au>Zhu, Yang</au><au>Wang, Zhi-Jie</au><au>Ding, Kun</au><au>Chang-Yuan, Su</au><au>Meng-Meng Lun</au><au>Zhi-Xu, Zhang</au><au>Zhang, Yi</au><au>Da-Wei, Fu</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Homochirality to design high-Tc lead-free ferroelastic semiconductors</atitle><jtitle>Journal of materials chemistry. C, Materials for optical and electronic devices</jtitle><date>2024-05-02</date><risdate>2024</risdate><volume>12</volume><issue>17</issue><spage>6098</spage><epage>6105</epage><pages>6098-6105</pages><issn>2050-7526</issn><eissn>2050-7534</eissn><abstract>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.</abstract><cop>Cambridge</cop><pub>Royal Society of Chemistry</pub><doi>10.1039/d4tc00428k</doi><tpages>8</tpages><oa>free_for_read</oa></addata></record> |
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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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