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