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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- 118 -<br />
Lifetime broadening alone gives rise to a Lorentzian line-<br />
shape in the frequency domain with a width at half-height of 1/'nT1.<br />
Assuming that the lifetime contribution to the total width of the<br />
residual spectrum can be separated by a simple subtraction, then<br />
upon substituting the values for T1 recorded previously the secular<br />
broadening of the central line becomes about 560 Hz for both iso-<br />
topes. The above value includes a contribution from the inhomo-<br />
geneity of the magnetic field but this was estimated to be negigible<br />
(< 20 Hz) in comparison. Consequently the figure quoted represents<br />
a measure of the electron coupled scalar interaction between the<br />
cadmium nuclei. The equivalence of the linewidth for the two iso-<br />
topes simply reflects their almost equal natural abundancies.<br />
At room temperature the relaxation times of both isotopes are of<br />
approximately the same magnitude as the inverse of the first and<br />
second nearest neighbour exchange coupled constants as determined<br />
(139)<br />
by Alloul and Deltour. This leads to the possibility that<br />
the isotropic magnetic exchange interaction may be time averaged by<br />
lifetime fluctuations in the nuclear spin states. Any detailed<br />
calculation of the Rudermann-Kittel(14) indirect exchange interact-<br />
ion is precluded by an incomplete knowledge of the effect of these<br />
fluctuations as well as by the preliminary nature of the results.<br />
Consequently we content ourselves with making a simple comparison<br />
of our results to those obtained by Alloul and Deltour from observat-<br />
ion of the modulated structure of the spin echoes of the 113Cd reson-<br />
ance in cadmium based alloys. Their experiment was undertaken at<br />
liquid helium temperatures, in which region T1 contributions to the<br />
lineshapes are negligible. The exchange coupling constants, J1<br />
and J2, between the first and second nearest neighbours in the hexagonal