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Analysis of the Structure, Thermal, and Molecular Dynamics of Organic–Inorganic Hybrid Crystal at Phases IV, III, II, and I: [NH(2)(CH(3))(2)](2)CdBr(4)

[Image: see text] A comprehensive understanding of the physicochemical properties of organic–inorganic hybrids is essential for their solid-state lighting applications. Therefore, a single crystal of [NH(2)(CH(3))(2)](2)CdBr(4) was grown; the crystal structure was monoclinic, and the phase transitio...

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Autores principales: Kim, Sun Ha, Joo, Yong Lak, Lim, Ae Ran
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2023
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10515402/
https://www.ncbi.nlm.nih.gov/pubmed/37744861
http://dx.doi.org/10.1021/acsomega.3c05963
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author Kim, Sun Ha
Joo, Yong Lak
Lim, Ae Ran
author_facet Kim, Sun Ha
Joo, Yong Lak
Lim, Ae Ran
author_sort Kim, Sun Ha
collection PubMed
description [Image: see text] A comprehensive understanding of the physicochemical properties of organic–inorganic hybrids is essential for their solid-state lighting applications. Therefore, a single crystal of [NH(2)(CH(3))(2)](2)CdBr(4) was grown; the crystal structure was monoclinic, and the phase transition temperatures for the four phases IV, III, II, and I were 383 K (T(C1)), 417 K (T(C2)), and 427 K (T(C3)). Furthermore, the chemical shifts caused by the local field around (1)H, (13)C, (14)N, and (113)Cd changed continuously with temperature, especially near T(C1), indicating that the local environment changes with temperature. Owing to the large change in (113)Cd chemical shifts, the coordination geometry of Br around Cd in the CdBr(4) tetrahedra changes near T(C1). Therefore, it is proposed that Br plays a significant role in the N–H···Br hydrogen bond. Finally, the spin-lattice relaxation time T(1ρ), representing the energy transfer around the (1)H and (13)C atoms of the cation, changed significantly with temperature. The activation energies obtained from the T(1ρ) results were two times larger at high temperatures than at low temperatures. This study provides an understanding of the fundamental properties of organic–inorganic hybrid compounds to broaden their applications.
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spelling pubmed-105154022023-09-23 Analysis of the Structure, Thermal, and Molecular Dynamics of Organic–Inorganic Hybrid Crystal at Phases IV, III, II, and I: [NH(2)(CH(3))(2)](2)CdBr(4) Kim, Sun Ha Joo, Yong Lak Lim, Ae Ran ACS Omega [Image: see text] A comprehensive understanding of the physicochemical properties of organic–inorganic hybrids is essential for their solid-state lighting applications. Therefore, a single crystal of [NH(2)(CH(3))(2)](2)CdBr(4) was grown; the crystal structure was monoclinic, and the phase transition temperatures for the four phases IV, III, II, and I were 383 K (T(C1)), 417 K (T(C2)), and 427 K (T(C3)). Furthermore, the chemical shifts caused by the local field around (1)H, (13)C, (14)N, and (113)Cd changed continuously with temperature, especially near T(C1), indicating that the local environment changes with temperature. Owing to the large change in (113)Cd chemical shifts, the coordination geometry of Br around Cd in the CdBr(4) tetrahedra changes near T(C1). Therefore, it is proposed that Br plays a significant role in the N–H···Br hydrogen bond. Finally, the spin-lattice relaxation time T(1ρ), representing the energy transfer around the (1)H and (13)C atoms of the cation, changed significantly with temperature. The activation energies obtained from the T(1ρ) results were two times larger at high temperatures than at low temperatures. This study provides an understanding of the fundamental properties of organic–inorganic hybrid compounds to broaden their applications. American Chemical Society 2023-09-08 /pmc/articles/PMC10515402/ /pubmed/37744861 http://dx.doi.org/10.1021/acsomega.3c05963 Text en © 2023 The Authors. Published by American Chemical Society https://creativecommons.org/licenses/by-nc-nd/4.0/Permits non-commercial access and re-use, provided that author attribution and integrity are maintained; but does not permit creation of adaptations or other derivative works (https://creativecommons.org/licenses/by-nc-nd/4.0/).
spellingShingle Kim, Sun Ha
Joo, Yong Lak
Lim, Ae Ran
Analysis of the Structure, Thermal, and Molecular Dynamics of Organic–Inorganic Hybrid Crystal at Phases IV, III, II, and I: [NH(2)(CH(3))(2)](2)CdBr(4)
title Analysis of the Structure, Thermal, and Molecular Dynamics of Organic–Inorganic Hybrid Crystal at Phases IV, III, II, and I: [NH(2)(CH(3))(2)](2)CdBr(4)
title_full Analysis of the Structure, Thermal, and Molecular Dynamics of Organic–Inorganic Hybrid Crystal at Phases IV, III, II, and I: [NH(2)(CH(3))(2)](2)CdBr(4)
title_fullStr Analysis of the Structure, Thermal, and Molecular Dynamics of Organic–Inorganic Hybrid Crystal at Phases IV, III, II, and I: [NH(2)(CH(3))(2)](2)CdBr(4)
title_full_unstemmed Analysis of the Structure, Thermal, and Molecular Dynamics of Organic–Inorganic Hybrid Crystal at Phases IV, III, II, and I: [NH(2)(CH(3))(2)](2)CdBr(4)
title_short Analysis of the Structure, Thermal, and Molecular Dynamics of Organic–Inorganic Hybrid Crystal at Phases IV, III, II, and I: [NH(2)(CH(3))(2)](2)CdBr(4)
title_sort analysis of the structure, thermal, and molecular dynamics of organic–inorganic hybrid crystal at phases iv, iii, ii, and i: [nh(2)(ch(3))(2)](2)cdbr(4)
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10515402/
https://www.ncbi.nlm.nih.gov/pubmed/37744861
http://dx.doi.org/10.1021/acsomega.3c05963
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