Abstract
Consider an ensemble of systems consisting of two arbitrary spins I and S. The interaction mechanism is assumed to be dipolar interaction. Spin-lattice relaxation refers to the z components of the magnetizations. The stationary part of the Hamiltonian is given as the Zeeman expression
where ωI = γIB0 and ωs = γsB0. No assumption is yet made concerning the gyromagnetic ratios of the spin-bearing particles, γI and γs. The spin-interaction Hamiltonian Hi is identified with that for dipolar coupling Hd.
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Notes
This holds true for samples with powder geometry. Deviations are only expected with ordered systems permitting only very few orientations of the interdipole vectors.
Besides, the modulus of this term is small compared with that of the first term, because, in the period in which the correlation function retains non-vanishing values, i.e., τ ≲ τc, the sine function either remains minor if ωl(k)τC≲ 1, or oscillates
Because of the even character of the autocorrelation function, the sign of τ may be reversed in order to conform to the usual convention of the Fourier transformation (see Sect. 42.3).
Exceptions are found in cubic-or tetrahedral structure-like molecular environments where the electric-field gradient may even vanish.
In [335] an interesting NMR experiment is described that permits the direct observation of the resonance in the effective field acting as the quantization field in the rotating frame.
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© 1997 Springer-Verlag Berlin Heidelberg
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Kimmich, R. (1997). Spin-Lattice Relaxation. In: NMR. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-60582-6_12
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DOI: https://doi.org/10.1007/978-3-642-60582-6_12
Publisher Name: Springer, Berlin, Heidelberg
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