1986
DOI: 10.1002/pssa.2210930156
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The “Cascade” Narrowing of the NMR Line in Solids by Radio-Frequency Fields and Slow Molecular Motions

Abstract: It is well known that moiecular motions in solids can b e monitored by their effect on the NMR linewidth or the transverse relaxation time T2 on the condition that 1) prospekt K a r h M:rrlis:~, 1 % 907 Moscow GSp-3, USSR.

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Cited by 9 publications
(7 citation statements)
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“…Note that the FID shape in Fig. 3 is similar to that observed in the RF (0, = aim) in the same sample [9] as well as in a CaF2 single crystal [4]. (Fig.…”
Section: Experimental Examplessupporting
confidence: 52%
See 1 more Smart Citation
“…Note that the FID shape in Fig. 3 is similar to that observed in the RF (0, = aim) in the same sample [9] as well as in a CaF2 single crystal [4]. (Fig.…”
Section: Experimental Examplessupporting
confidence: 52%
“…In this situation, the effective Hamiltonian of residual secular DD interactions in the RF reveals qualitatively new properties, namely it is determined by the product of spin operators of three nuclei [2] (unlike two-spin operators in the initial DD Hamiltonian [3] ). This peculiarity causes some consequences concerning spin thermodynamics [1], spin [4][5][6][7] and molecular dynamics [8,9], and so on. The next step was to record NMR and longitudinal relaxation in the effective magnetic field HH2 acting in the doubly rotating frame (DRF) [10].…”
Section: Introductionmentioning
confidence: 99%
“…The ultraslow-motion term originating from H ER 0 produces an ascending branch in the 1/T 2 dispersion curve that causes a minimum at c Ϸ 1/ L . Equation [6] has been confirmed by numerical simulation and experimental results (22).…”
Section: Theorymentioning
confidence: 60%
“…Equations ( 12)- (15) show that the degeneracy of the energy spectrum is removed, without a DC magnetic field, just by application of two RF fields with different phases and directions. The energy levels E s correspond to the eigenstates of the quantum system described by the effective Hamiltonian H ef f |ζ s = E s |ζ s , where the |ζ s are the eigenfunctions with s = 0, 1, 2, 3.…”
Section: Energy Spectrummentioning
confidence: 99%