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

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- 119 -<br />

close packed crystal lattice were calculated using the expression<br />

for the second moment<br />

M2 = 0.95B2 + 0.218J2 + 0.192J2<br />

where B1 represents the total dipolar coupling between first near-<br />

est neighbours (including pseudo-dipolar coupling). Rotation at<br />

the magic angle removes the dipolar and pseudo-dipolar contribut-<br />

ions to the central spectrum. The second moment of the residual<br />

line is then given by<br />

M2 = 0.218J2 + 0.192J2<br />

The width of a Gaussian lineshape is often approximated to 2,412.<br />

Applying a similar approximation here and substituting Alloul and<br />

Deltour's values for J1 and J2 of -510 Hz and -380 Hz respectively<br />

into the above expression, we obtain a theoretical linewidth of<br />

580 Hz. The agrement with the T1 corrected value for the experi-<br />

mental linewidth quoted previously is very satisfactory. In view<br />

of the assumptions made in the calculation, the precise agreement<br />

may be fortuitous. Nevertheless, it does serve to demonstrate<br />

that any lifetime averaging effect on the scalar interaction<br />

room temperature is probably small.<br />

In conclusion we emphasize the preliminary nature of our<br />

measurements. The experimental accuracy could be improved by<br />

averaging the detected decay signals over a longer period of time<br />

and by employing a more reliable procedure for fitting the dead<br />

time data points. However, as the rotors at present available<br />

at

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