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Broadband inversion for MAS NMR with single-sideband-selective adiabatic pulses

Authors :
Gwendal Kervern
Lyndon Emsley
Guido Pintacuda
Andrew J. Pell
Philip J. Grandinetti
Dominique Massiot
Michaël Deschamps
Institut des Sciences Analytiques (ISA)
Institut de Chimie du CNRS (INC)-Université Claude Bernard Lyon 1 (UCBL)
Université de Lyon-Université de Lyon-Centre National de la Recherche Scientifique (CNRS)
ISA - Centre de RMN à très hauts champs
Université de Lyon-Université de Lyon-Centre National de la Recherche Scientifique (CNRS)-Institut de Chimie du CNRS (INC)-Université Claude Bernard Lyon 1 (UCBL)
Conditions Extrêmes et Matériaux : Haute Température et Irradiation (CEMHTI)
Université d'Orléans (UO)-Institut de Chimie du CNRS (INC)-Centre National de la Recherche Scientifique (CNRS)
Université d'Orléans (UO)
Fédération RMN du Solide à Hauts Champs (FRMN-SHC)
Source :
Journal of Chemical Physics, Journal of Chemical Physics, American Institute of Physics, 2011, 134, pp.024117. ⟨10.1063/1.3521491⟩
Publication Year :
2011

Abstract

We explain how and under which conditions it is possible to obtain an efficient inversion of an entire sideband family of several hundred kHz using low-power, sideband-selective adiabatic pulses, and we illustrate with some experimental results how this framework opens new avenues in solid-state NMR for manipulating spin systems with wide spinning-sideband (SSB) manifolds. This is achieved through the definition of the criteria of phase and amplitude modulation for designing an adiabatic inversion pulse for rotating solids. In turn, this is based on a framework for representing the Hamiltonian of the spin system in an NMR experiment under magic angle spinning (MAS). Following earlier ideas from Caravatti et al. [J. Magn. Reson. 55, 88 (1983)], the so-called ``jolting frame'' is used, which is the interaction frame of the anisotropic interaction giving rise to the SSB manifold. In the jolting frame, the shift modulation affecting the nuclear spin is removed, while the Hamiltonian corresponding to the RF field is frequency modulated and acquires a spinning-sideband pattern, specific for each crystallite orientation. (C) 2011 American Institute of Physics. [doi: 10.1063/1.3521491]

Details

ISSN :
10897690 and 00219606
Volume :
134
Issue :
2
Database :
OpenAIRE
Journal :
The Journal of chemical physics
Accession number :
edsair.doi.dedup.....582fdcb91ade1585c8d8a385492cddf5