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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-66-<br />
The transient nuclear signals were recorded by using the<br />
DL 102 signal averager. In the experimental arrangement used<br />
each scan through the 200 memory channels was triggered off the<br />
leading edge of the gating pulse to the transmitter and the det-<br />
ected FID following the rf pulse was DC coupled into the averager.<br />
No on-line Fourier transform capability was available, so the cont-<br />
ents of the averager's memory were output to the teletype and<br />
recorded onto paper tape. Fourier transformation of the recorded<br />
data was undertaken with the University's ICL 1906A computer. The<br />
program used for this purpose basically operated from the numeri-<br />
cal summation<br />
(w) _1<br />
I G(t) cos wt St<br />
Second moment values were determined from the transformed spectra<br />
by a simple summation procedure written into the computer program.<br />
Asymmetric nuclear lineshapes such as those arising from aniso-<br />
tropic Knight shift interactions were obtained by setting the ref-<br />
erence frequency to the phase sensitive detector well outside the<br />
resonance spectrum. The transient response to the if pulse was<br />
then recorded along a single detection axis in the rotating refer-<br />
ence frame. After a correction for the reference phase the decay<br />
signals were transformed using the same summation procedure as<br />
above. This results in a symmetric frequency distribution with<br />
the asymmetric absorption lineshape mirrored about vref'<br />
The time origin of the recorded decay shapes was taken as the<br />
centre of the -rf pulse for all measurements. This position has<br />
been determined theoretically(68) and was confirmed for the rotating