AI Article Synopsis

  • Solid-state Mo NMR studies were conducted on various MoS materials using high-field magnets (19.6 T and 35.2 T), highlighting Mo's spin relaxation properties related to chemial shift anisotropy (CSA).
  • Research showed that the relaxation rates increased with certain parameters, indicating that electronic delocalization within the MoS structure influences Mo CSA, allowing for better analytical insights.
  • The findings addressed previous challenges in retrieving spectral parameters by demonstrating shorter relaxation times in newer samples, enabling successful observation of detailed NMR spectra for multilayer MoS materials, including the first observation of MAS NMR for a specific configuration.

Article Abstract

Solid-state, natural-abundance Mo NMR experiments of four different MoS materials have been performed on a magnet = 19.6 T and on a new Series Connected Hybrid (SCH) magnet at 35.2 T. Employing two different 2H-MoS (2H phase) materials, a "pseudo-amorphous" MoS nano-material, and a MoS layer on the AlO support of a hydrodesulphurization (HDS) catalyst have enabled introduction of solid-state Mo NMR as an important analytical tool in studies of MoS nano-materials. Mo spin-lattice relaxation time ( ) studies of 160- and 4-layer 2H-MoS samples at 19.6 and 35.2 T show their relaxation rates (1/ ) increase in proportion to . This is in accord with chemical shift anisotropy (CSA) relaxation being the dominant (Mo) mechanism, with a large Mo CSA = 1025 ppm determined for all four MoS nano-materials. The dominant CSA mechanism suggests the MoS band-gap electrons are delocalized throughout the lattice-layer structures, thereby acting as a fast modulation source ( τ << 1) for Mo CSA in 2H-MoS. A decrease in (Mo) is observed for an increase in field and for a decrease in the number of 2H-MoS layers. All four nano-materials exhibit identical Mo electric field gradient (EFG) parameters. The results account for the several failures to retrieve Mo spectral EFG and CSA parameters for multilayer 2H-MoS samples in the pioneering solid-state Mo NMR studies performed during the past two decades (1990-2010), because of the extremely long (Mo) = ~200-250 s observed at low (~9.4 T) used at that time. Much shorter (Mo) values are observed even at 19.6 T for the "pseudo-amorphous" and the HDS catalyst (MoS-AlO support) MoS nano-materials. These allowed useful solid-state Mo NMR spectra for these two samples to be obtained at 19.6 T in a few to < 24 h. Most importantly, this research led to observation of an impressive Mo MAS spectrum for an average of 1-4 thick MoS-layers on a AlO support, i.e., the first MAS NMR spectrum of a low natural-abundance, low-γ quadrupole-nucleus species layered on a catalyst support. While a huge gain in NMR sensitivity, factor ~ 60, is observed for the Mo MAS spectrum of the 160-layer sample at 35.2 T compared to 14.1 T, the MAS spectrum for the 4-layer sample is almost completely wiped out at 35.2 T. This unusual observation for the 4-layer sample (crumpled, rose-like and defective Mo-edge structures) is due to an increased distribution of the isotropic Mo shifts in the Mo MAS spectra at up to 35.2 T upon reduction of the number of sample layers.

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Source
http://www.ncbi.nlm.nih.gov/pmc/articles/PMC8276973PMC
http://dx.doi.org/10.1021/acs.jpcc.0c10522DOI Listing

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