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Structural Disorder in Li(6)PS(5)I Speeds (7)Li Nuclear Spin Recovery and Slows Down (31)P Relaxation–Implications for Translational and Rotational Jumps as Seen by Nuclear Magnetic Resonance

[Image: see text] Lithium-thiophosphates have attracted great attention as they offer a rich playground to develop tailor-made solid electrolytes for clean energy storage systems. Here, we used poorly conducting Li(6)PS(5)I, which can be converted into a fast ion conductor by high-energy ball-millin...

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Autores principales: Brinek, M., Hiebl, C., Hogrefe, K., Hanghofer, I., Wilkening, H. M. R.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2020
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7662756/
https://www.ncbi.nlm.nih.gov/pubmed/33193940
http://dx.doi.org/10.1021/acs.jpcc.0c06090
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author Brinek, M.
Hiebl, C.
Hogrefe, K.
Hanghofer, I.
Wilkening, H. M. R.
author_facet Brinek, M.
Hiebl, C.
Hogrefe, K.
Hanghofer, I.
Wilkening, H. M. R.
author_sort Brinek, M.
collection PubMed
description [Image: see text] Lithium-thiophosphates have attracted great attention as they offer a rich playground to develop tailor-made solid electrolytes for clean energy storage systems. Here, we used poorly conducting Li(6)PS(5)I, which can be converted into a fast ion conductor by high-energy ball-milling to understand the fundamental guidelines that enable the Li(+) ions to quickly diffuse through a polarizable but distorted matrix. In stark contrast to well-crystalline Li(6)PS(5)I (10(–6) S cm(–1)), the ionic conductivity of its defect-rich nanostructured analog touches almost the mS cm(–1) regime. Most likely, this immense enhancement originates from site disorder and polyhedral distortions introduced during mechanical treatment. We used the spin probes (7)Li and (31)P to monitor nuclear spin relaxation that is directly induced by Li(+) translational and/or PS(4)(3–) rotational motions. Compared to the ordered form, (7)Li spin–lattice relaxation (SLR) in nano-Li(6)PS(5)I reveals an additional ultrafast process that is governed by activation energy as low as 160 meV. Presumably, this new relaxation peak, appearing at T(max) = 281 K, reflects extremely rapid Li hopping processes with a jump rate in the order of 10(9) s(–1) at T(max). Thus, the thiophosphate transforms from a poor electrolyte with island-like local diffusivity to a fast ion conductor with 3D cross-linked diffusion routes enabling long-range transport. On the other hand, the original (31)P nuclear magnetic resonance (NMR) SLR rate peak, pointing to an effective (31)P-(31)P spin relaxation source in ordered Li(6)PS(5)I, is either absent for the distorted form or shifts toward much higher temperatures. Assuming the (31)P NMR peak as being a result of PS(4)(3–) rotational jump processes, NMR unveils that disorder significantly slows down anion dynamics. The latter finding might also have broader implications and sheds light on the vital question how rotational dynamics are to be manipulated to effectively enhance Li(+) cation transport.
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spelling pubmed-76627562020-11-13 Structural Disorder in Li(6)PS(5)I Speeds (7)Li Nuclear Spin Recovery and Slows Down (31)P Relaxation–Implications for Translational and Rotational Jumps as Seen by Nuclear Magnetic Resonance Brinek, M. Hiebl, C. Hogrefe, K. Hanghofer, I. Wilkening, H. M. R. J Phys Chem C Nanomater Interfaces [Image: see text] Lithium-thiophosphates have attracted great attention as they offer a rich playground to develop tailor-made solid electrolytes for clean energy storage systems. Here, we used poorly conducting Li(6)PS(5)I, which can be converted into a fast ion conductor by high-energy ball-milling to understand the fundamental guidelines that enable the Li(+) ions to quickly diffuse through a polarizable but distorted matrix. In stark contrast to well-crystalline Li(6)PS(5)I (10(–6) S cm(–1)), the ionic conductivity of its defect-rich nanostructured analog touches almost the mS cm(–1) regime. Most likely, this immense enhancement originates from site disorder and polyhedral distortions introduced during mechanical treatment. We used the spin probes (7)Li and (31)P to monitor nuclear spin relaxation that is directly induced by Li(+) translational and/or PS(4)(3–) rotational motions. Compared to the ordered form, (7)Li spin–lattice relaxation (SLR) in nano-Li(6)PS(5)I reveals an additional ultrafast process that is governed by activation energy as low as 160 meV. Presumably, this new relaxation peak, appearing at T(max) = 281 K, reflects extremely rapid Li hopping processes with a jump rate in the order of 10(9) s(–1) at T(max). Thus, the thiophosphate transforms from a poor electrolyte with island-like local diffusivity to a fast ion conductor with 3D cross-linked diffusion routes enabling long-range transport. On the other hand, the original (31)P nuclear magnetic resonance (NMR) SLR rate peak, pointing to an effective (31)P-(31)P spin relaxation source in ordered Li(6)PS(5)I, is either absent for the distorted form or shifts toward much higher temperatures. Assuming the (31)P NMR peak as being a result of PS(4)(3–) rotational jump processes, NMR unveils that disorder significantly slows down anion dynamics. The latter finding might also have broader implications and sheds light on the vital question how rotational dynamics are to be manipulated to effectively enhance Li(+) cation transport. American Chemical Society 2020-09-29 2020-10-22 /pmc/articles/PMC7662756/ /pubmed/33193940 http://dx.doi.org/10.1021/acs.jpcc.0c06090 Text en © 2020 American Chemical Society This is an open access article published under a Creative Commons Attribution (CC-BY) License (http://pubs.acs.org/page/policy/authorchoice_ccby_termsofuse.html) , which permits unrestricted use, distribution and reproduction in any medium, provided the author and source are cited.
spellingShingle Brinek, M.
Hiebl, C.
Hogrefe, K.
Hanghofer, I.
Wilkening, H. M. R.
Structural Disorder in Li(6)PS(5)I Speeds (7)Li Nuclear Spin Recovery and Slows Down (31)P Relaxation–Implications for Translational and Rotational Jumps as Seen by Nuclear Magnetic Resonance
title Structural Disorder in Li(6)PS(5)I Speeds (7)Li Nuclear Spin Recovery and Slows Down (31)P Relaxation–Implications for Translational and Rotational Jumps as Seen by Nuclear Magnetic Resonance
title_full Structural Disorder in Li(6)PS(5)I Speeds (7)Li Nuclear Spin Recovery and Slows Down (31)P Relaxation–Implications for Translational and Rotational Jumps as Seen by Nuclear Magnetic Resonance
title_fullStr Structural Disorder in Li(6)PS(5)I Speeds (7)Li Nuclear Spin Recovery and Slows Down (31)P Relaxation–Implications for Translational and Rotational Jumps as Seen by Nuclear Magnetic Resonance
title_full_unstemmed Structural Disorder in Li(6)PS(5)I Speeds (7)Li Nuclear Spin Recovery and Slows Down (31)P Relaxation–Implications for Translational and Rotational Jumps as Seen by Nuclear Magnetic Resonance
title_short Structural Disorder in Li(6)PS(5)I Speeds (7)Li Nuclear Spin Recovery and Slows Down (31)P Relaxation–Implications for Translational and Rotational Jumps as Seen by Nuclear Magnetic Resonance
title_sort structural disorder in li(6)ps(5)i speeds (7)li nuclear spin recovery and slows down (31)p relaxation–implications for translational and rotational jumps as seen by nuclear magnetic resonance
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7662756/
https://www.ncbi.nlm.nih.gov/pubmed/33193940
http://dx.doi.org/10.1021/acs.jpcc.0c06090
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