Adiabatic sweep pulses for earth’s field NMR with a surface coil

[Display omitted] •Adiabatic sweep pulses that function well in low fields.•Means to avoid coming close to zero frequency.•Method of avoiding the ill-effects of the counter-rotating component of RF field. Adiabatic NMR sweep pulses are described for inversion and excitation in very low magnetic fiel...

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Veröffentlicht in:Journal of magnetic resonance (1997) 2018-03, Vol.288, p.23-27
Hauptverfasser: Conradi, Mark S., Altobelli, Stephen A., Sowko, Nicholas J., Conradi, Susan H., Fukushima, Eiichi
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Sprache:eng
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Zusammenfassung:[Display omitted] •Adiabatic sweep pulses that function well in low fields.•Means to avoid coming close to zero frequency.•Method of avoiding the ill-effects of the counter-rotating component of RF field. Adiabatic NMR sweep pulses are described for inversion and excitation in very low magnetic fields B0 and with broad distribution of excitation field amplitude B1. Two aspects distinguish the low field case: (1) when B1 is comparable to or greater than B0, the rotating field approximation fails and (2) inversion sweeps cannot extend to values well below the Larmor frequency because they would approach or pass through zero frequency. Three approaches to inversion are described. The first is a conventional tangent frequency sweep down to the Larmor frequency, a 180° phase shift, and a sweep back up to the starting frequency. The other two are combined frequency and amplitude sweeps covering a narrower frequency range; one is a symmetric sweep from above to below the Larmor frequency and the other uses a smooth decrease of B1 immediately before and after the 180° phase shift. These two AM/FM sweeps show excellent inversion efficiencies over a wide range of B1, a factor of 30 or more. We also demonstrate an excitation sweep that works well in the presence of the same wide range of B1. We show that the primary effect of the counter-rotating field (i.e., at low B0) is that the magnetization suffers large, periodic deviations from where it would be at large B0. Thus, successful sweep pulses must avoid any sharp features in the amplitude, phase, or frequency.
ISSN:1090-7807
1096-0856
DOI:10.1016/j.jmr.2017.11.018