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

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- 110 -<br />

figures may arise partly from a bulk susceptibility correction due<br />

to the geometry of the samples used in each case. However a calc-<br />

ulation similar to that performed for aluminium in Section 7.2.3(c)<br />

puts the possible contribution to the experimental Knight shift<br />

measured here of no more than 5 ppm. Certainly there was no measur-<br />

able difference in the resonance frequencies of 51V<br />

powder specimens and the solid araldite slugs.<br />

8.3 NIOBIUM<br />

in the loose<br />

99.9% pure niobium powder with a particle size of less than<br />

40 dun was obtained from Metals Research Limited. The static measure-<br />

ments were recorded on specimens of the loosely packed unannealed<br />

powder at room temperature using a resonant frequency of 15 MHz.<br />

The spin-lattice relaxation time was measured using a 90-T-90<br />

pulse sequence, but the recovery envelope was not found to obey a<br />

simple exponential relationship. A large proportion of the magnet-<br />

ization recovered in a few microseconds, but a slow component had a<br />

time constant of about 1.1 ms. This form of recovery indicates<br />

that there was a significant second-order quadrupole broadening<br />

present in the powder specimens, a result which is in agreement with<br />

that recorded by y Butterworth in similar powdered metal samples.<br />

The FIDs recorded from these samples were found to be almost<br />

exponential with a time constant of 11.5 ± 1.5 is. This value is<br />

considerably shorter than that found by Butterworth from a pure foil<br />

sample, but is consistent with his measured T2 values from powdered<br />

specimens and the large variation in linewidths reported elsewhere.<br />

The width of the Lorentzian lineshape defined by the exponential decay<br />

of the transverse magnetization is given by<br />

(127)

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