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th  - 1988 - 51st ENC Conference

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19 I DIPOLARAND SPIN-ROTATION POLARIZATION OF METHYL GROUP SPINS<br />

Michael Murphy and David White, Dept. of Chemistry<br />

University of Pennsylvania, Philadelphia, PA 19104<br />

We have investigated <strong>th</strong>e proton NMR of molecules such as CH3CN , CH3CmCH ,<br />

and CH3CI trapped at low concentrations in solid Kr. The me<strong>th</strong>yl groups in<br />

<strong>th</strong>ese matrices undergo nearly free quantum rotation, allowing for polarization<br />

of me<strong>th</strong>yl spins to occur via coupled spin and rotational relaxation following<br />

a temperature jump. Besides proton-proton dipolar polarization (<strong>th</strong>e 'Haupt<br />

I<br />

effect' ), we have identified additional spin polarizations, namely, <strong>th</strong>ose<br />

associated wi<strong>th</strong> secular spin-rotation and heteronuclear dipolar interactions.<br />

Due to <strong>th</strong>e magnetic isolation of <strong>th</strong>e molecules, well-resolved powder line-<br />

shapes are obtained from which <strong>th</strong>e contributions of different spin observables<br />

may be distinguished. We provide evidence <strong>th</strong>at a finite spin-rotation cou-<br />

pling exists and determine <strong>th</strong>e coupling constant for CH3CN/Kr by examining <strong>th</strong>e<br />

signal component due to polarized 'spin-rotation magnetization'. Heteronuclear<br />

2 Is<br />

dipolar polarization is demonstrated in CH3CN/Kr. Lineshape analyses are<br />

shown to provide new information regarding <strong>th</strong>e me<strong>th</strong>yl group rotational levels.<br />

I. J. Haupt, Phys. Lett. 38A, 389 (1972); Z. Naturforsch 28a, 98 (1973)<br />

2. M. Murphy and D. White, J. Chem. Phys. 86, 1640 (1987)<br />

I -- 2 0 I NMR SIGNAL PROCESSING USING PADE APPROXIMANT AND LINEAR<br />

PREDICTION Z-TRANSFORM METHOD: J. Tang*, Y. Zeng and J. R. Norris, Chemistry Division,<br />

Argonne National Laboratory, Argonne, IL 60439<br />

Linear prediction (LP) <strong>th</strong>eory has been widely applied to digital signal processing to overcome<br />

truncation and noise problems often encountered by <strong>th</strong>e fast Fourier transform me<strong>th</strong>od. Here, a new<br />

approach 1 is proposed for NMR spectral analysis wi<strong>th</strong> enhanced resolution and sensitivity using Pad6<br />

rational approximation 2-s and linear prediction z-transform. 4 In <strong>th</strong>e conventional LP me<strong>th</strong>ods 4 such as<br />

LPQRD or LPSVD, <strong>th</strong>e whole spectrum is analyzed. In order to resolve all <strong>th</strong>e spectral lines a very large<br />

LP filter leng<strong>th</strong>, usually several times <strong>th</strong>at of <strong>th</strong>e total number of spectral components, has to be used.<br />

In contrast, <strong>th</strong>is me<strong>th</strong>od can be used to zoom into a small section of <strong>th</strong>e whole spectrum for analysis if<br />

<strong>th</strong>e spectral contents in some zones are of particular interest. Thus, <strong>th</strong>is me<strong>th</strong>od uses a much shorter<br />

LP filter leng<strong>th</strong> and requires a smaller computer memory and shorter computational time. As LPQRD or<br />

LPSVD, <strong>th</strong>is me<strong>th</strong>od also yields a table of spectral parameters wi<strong>th</strong>out additional efforts required by FFT.<br />

Applications of <strong>th</strong>is me<strong>th</strong>od and <strong>th</strong>e comparisons wi<strong>th</strong> LPQRD or LPSVD will be presented. O<strong>th</strong>er LP<br />

me<strong>th</strong>ods using computationally efficient autoregression (AR) or Burg algori<strong>th</strong>m s are particularly useful for<br />

2-D NMR signal processing. By LP extrapolation of <strong>th</strong>e unobserved FID and application of line-<br />

narrowing apodization functions one can significantly improve spectral resolution while avoiding sinc-<br />

wiggling artifacts due to data truncation.<br />

.<br />

2.<br />

3.<br />

4.<br />

.<br />

J. Tang and J. R. Norris, Nature, (in press).<br />

E. Yeramian and P. Claverie, Nature 326, 169 (1987).<br />

J. Tang and J. R. Norris, J. Magn. Reson. (in press).<br />

J. Tang and J. R. Norris, in "Electronic Magnetic Resonance of <strong>th</strong>e Solid State', Vol. 1, p. I11<br />

(1987) (Ed., J. Weil), The Canadian Society for Chemistry, Ottawa, Canada.<br />

J. Tang and J. R. Norris, Chem. Phys. Lett. 131, 252 (1986).<br />

This work was supported by <strong>th</strong>e U.S. Department of Energy, Office of Basic Energy Sciences,<br />

Division of Chemical Sciences under contract W-31-109-Eng-38.<br />

107

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