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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- 94 -<br />
aluminium nuclei in the metal and reference compound. A consider-<br />
able improvement in the accuracy of Knight shift calculations will<br />
be necessary to enable a precise comparison between theory and<br />
experiment to be made. However the value reported here of<br />
1.640 x 10 3 does show a small but significant departure from the<br />
previously accepted estimate of 1.61 x<br />
10 3.<br />
7.3 RECORDED L<strong>IN</strong>ESHAPES AND SECOND MOMENT VALUES<br />
7.3.1 <strong>IN</strong>TRODUCTION<br />
Although theory is unable to predict the exact form of<br />
the absorption spectrum, a comparison between the theoretical and<br />
experimental second moments can be made.<br />
27A1<br />
is the only natur-<br />
ally occurring aluminium isotope. It occupies a FCC lattice, the<br />
lattice constant being 4.0496 X.<br />
moment predicted by Van Vleck's calculation<br />
From this the dipolar second<br />
(16)<br />
is 9.18 kU1z2<br />
(7.44 G2). (It has also been quoted as 9.42 kHz2 (7.63 G2). )<br />
Previous experimental determinations on pure annealed specimens<br />
have consistently yielded values above this in the range 11.8 to<br />
15.4 kHz2 (9.5-12.5 G2)(72,103-110). The discrepancy between theory<br />
and experiment is well known. In the main it has been attribut-<br />
ed to a nuclear quadrupole interaction, but the mechanism for such<br />
an interaction has never been demonstrated conclusively.<br />
7.3.2 MEASUREMENTS<br />
The resonance spectra of the static aluminium powders<br />
were obtained by Fourier transformation of the detected FIDs as<br />
detailed in Section 5.6. In each case about 1 cm3 of the loose