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Cation dynamics by (1)H and (13)C MAS NMR in hybrid organic–inorganic (CH(3)CH(2)NH(3))(2)CuCl(4)

To understand the dynamics of the cation in layered perovskite-type (CH(3)CH(2)NH(3))(2)CuCl(4), the temperature-dependent chemical shifts and spin–lattice relaxation times T(1ρ) in the rotating frame have been measured using (1)H magic angle spinning nuclear magnetic resonance (MAS NMR) and (13)C c...

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Autores principales: Lim, Ae Ran, Joo, Yong Lak
Formato: Online Artículo Texto
Lenguaje:English
Publicado: The Royal Society of Chemistry 2018
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9086738/
https://www.ncbi.nlm.nih.gov/pubmed/35548822
http://dx.doi.org/10.1039/c8ra06268d
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author Lim, Ae Ran
Joo, Yong Lak
author_facet Lim, Ae Ran
Joo, Yong Lak
author_sort Lim, Ae Ran
collection PubMed
description To understand the dynamics of the cation in layered perovskite-type (CH(3)CH(2)NH(3))(2)CuCl(4), the temperature-dependent chemical shifts and spin–lattice relaxation times T(1ρ) in the rotating frame have been measured using (1)H magic angle spinning nuclear magnetic resonance (MAS NMR) and (13)C cross-polarization (CP)/MAS NMR techniques. Each proton and carbon in the (CH(3)CH(2)NH(3))(+) cation is distinguished in MAS NMR spectra. The Bloembergen–Purcell–Pound (BPP) curves for (1)H T(1ρ) in CH(3)CH(2) and NH(3), and for the (13)C T(1ρ) in CH(3) and CH(2) are revealed to have minima at low temperatures. This implies that the curves represent the CH(3) and NH(3)(+) rotational motions. The amplitude of the cationic motion is enhanced at the C-end, that is, the N-end of the organic cation is fixed to the inorganic layer through N–H⋯Cl hydrogen bonds, and T(1ρ) becomes short with larger-amplitude molecular motions.
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spelling pubmed-90867382022-05-10 Cation dynamics by (1)H and (13)C MAS NMR in hybrid organic–inorganic (CH(3)CH(2)NH(3))(2)CuCl(4) Lim, Ae Ran Joo, Yong Lak RSC Adv Chemistry To understand the dynamics of the cation in layered perovskite-type (CH(3)CH(2)NH(3))(2)CuCl(4), the temperature-dependent chemical shifts and spin–lattice relaxation times T(1ρ) in the rotating frame have been measured using (1)H magic angle spinning nuclear magnetic resonance (MAS NMR) and (13)C cross-polarization (CP)/MAS NMR techniques. Each proton and carbon in the (CH(3)CH(2)NH(3))(+) cation is distinguished in MAS NMR spectra. The Bloembergen–Purcell–Pound (BPP) curves for (1)H T(1ρ) in CH(3)CH(2) and NH(3), and for the (13)C T(1ρ) in CH(3) and CH(2) are revealed to have minima at low temperatures. This implies that the curves represent the CH(3) and NH(3)(+) rotational motions. The amplitude of the cationic motion is enhanced at the C-end, that is, the N-end of the organic cation is fixed to the inorganic layer through N–H⋯Cl hydrogen bonds, and T(1ρ) becomes short with larger-amplitude molecular motions. The Royal Society of Chemistry 2018-10-04 /pmc/articles/PMC9086738/ /pubmed/35548822 http://dx.doi.org/10.1039/c8ra06268d Text en This journal is © The Royal Society of Chemistry https://creativecommons.org/licenses/by/3.0/
spellingShingle Chemistry
Lim, Ae Ran
Joo, Yong Lak
Cation dynamics by (1)H and (13)C MAS NMR in hybrid organic–inorganic (CH(3)CH(2)NH(3))(2)CuCl(4)
title Cation dynamics by (1)H and (13)C MAS NMR in hybrid organic–inorganic (CH(3)CH(2)NH(3))(2)CuCl(4)
title_full Cation dynamics by (1)H and (13)C MAS NMR in hybrid organic–inorganic (CH(3)CH(2)NH(3))(2)CuCl(4)
title_fullStr Cation dynamics by (1)H and (13)C MAS NMR in hybrid organic–inorganic (CH(3)CH(2)NH(3))(2)CuCl(4)
title_full_unstemmed Cation dynamics by (1)H and (13)C MAS NMR in hybrid organic–inorganic (CH(3)CH(2)NH(3))(2)CuCl(4)
title_short Cation dynamics by (1)H and (13)C MAS NMR in hybrid organic–inorganic (CH(3)CH(2)NH(3))(2)CuCl(4)
title_sort cation dynamics by (1)h and (13)c mas nmr in hybrid organic–inorganic (ch(3)ch(2)nh(3))(2)cucl(4)
topic Chemistry
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9086738/
https://www.ncbi.nlm.nih.gov/pubmed/35548822
http://dx.doi.org/10.1039/c8ra06268d
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