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NNR IN RAPIDLY ROTATED METALS By - Nottingham eTheses ...

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- 27 -<br />

quadrupole moments to produce transitions within the spin levels<br />

of the nuclei. The vibrational modes in a solid may be assumed<br />

to occupy a Debye spectrum, the Debye frequency being defined by<br />

hvD - keD. There are three suggested phonon relaxation processes,<br />

(i) Single Phonon. Transitions induced between the nuclear<br />

spin states correspond to the creation or destruction of a single<br />

phonon. Only these phonons with energy hvp = hV0 can participate.<br />

However V0 « VD, so there are very few phonons which fulfil this<br />

condition and such a process is not an efficient relaxation<br />

mechanism. As phonons obey Bose-Einstein statistics and hv0 « kT<br />

the number of phonons with energy hV0 is proportional to the absolute<br />

temperature. The relaxation probability depends upon the number<br />

2<br />

of vibrational modes with frequency V0. Hence l/T1 a v0T.<br />

(ii) Four Phonon. A second order process has been suggested (20)<br />

by which two phonons are created and two destroyed, the energy<br />

difference being made up by the lattice transition. This mechanism<br />

predicts aT4 dependence of T1 but although it was expected to<br />

dominate at high temperatures it has never been observed experi-<br />

mentally. Indeed, a more recent calculation<br />

(21) has shown that<br />

such a process does not in fact give rise to any net transition<br />

between nuclear spin levels, and consequently does not contribute<br />

to the overall<br />

Tl.<br />

(iii) Two Phonon (Raman). This process is far more efficient<br />

than the single phonon because any phonon in the Debye spectrum<br />

can participate. A phonon is scattered inelastically<br />

at a nucleus<br />

so an induced transition between spin states is accompanied by a<br />

corresponding change in the phonon energy. Although the relaxation

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