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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

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