th - 1988 - 51st ENC Conference
th - 1988 - 51st ENC Conference
th - 1988 - 51st ENC Conference
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198 I NUMERICAL STUDIES OF STIMULATED ESEEM WAVEFORMS: H. Jin and H.<br />
omann, Corporate Research Laboratory, EXXON Research and Engineering Company,<br />
Route 22 East, Annandale, N. J. 08801<br />
Electron spin echo envelope modulation (ESEEM) spectroscopy has proven to be a<br />
powerful me<strong>th</strong>od for studying hyperfine and quadrupolar interactions of nuclei<br />
coordinated to paramagnetic electron centers. Important areas of application<br />
include <strong>th</strong>e study of nitrogen coordination in metalloproteins; surface adsorbate<br />
interactions of supported transition metals; and <strong>th</strong>e electron density distribution<br />
on organic paramagnetic radicals important in photosyn<strong>th</strong>esis and in photoexcited<br />
triplet states. Analysis of <strong>th</strong>e ESEEM patterns for S-I/2, I -I spin systems in<br />
randomly oriented solids is usually performed using frequency spectrum analysis.<br />
ESEEM spectra are simulated by calculating <strong>th</strong>e superposition of <strong>th</strong>e two powder<br />
pattern quadrupolar spectra obtained when <strong>th</strong>e isotropic hyperfine coupling adds or<br />
subtracts to <strong>th</strong>e Zeeman field. Such simulations will accurately predict ESEEM<br />
frequencies but will usually not even give qualitatively correct modulation dep<strong>th</strong>s<br />
in <strong>th</strong>e ESEEM waveform or reproduce <strong>th</strong>e correct linewid<strong>th</strong>s in <strong>th</strong>e ESEEM spectrum.<br />
These depend on <strong>th</strong>e anisotropic hyperfine interactions and are <strong>th</strong>erefore important<br />
spectroscopic parameters which can reveal additional chemical information about <strong>th</strong>e<br />
coordination complex. This provides <strong>th</strong>e impetus for numerical studies of <strong>th</strong>e ESEEM<br />
spectrum and time domain waveforms in which <strong>th</strong>e psuedodipolar as well as <strong>th</strong>e<br />
isotropic hyperfine and quadrupolar interactions are retained. Some preliminary<br />
numerical results of <strong>th</strong>is study will be presented in <strong>th</strong>is poster. In particular, we<br />
explore <strong>th</strong>e importance of <strong>th</strong>e relative magnitudes of <strong>th</strong>e Zeeman, isotropic and<br />
psuedodipolar hyperfine, and quadrupolar interactions in determining <strong>th</strong>e modulation<br />
dep<strong>th</strong> of <strong>th</strong>e ESEEM waveform. We also explore <strong>th</strong>e ESEEM waveform and frequency<br />
spectrum in <strong>th</strong>e presence of anisotropic hyperfine interactions wi<strong>th</strong> only a partial<br />
cancellation of <strong>th</strong>e Zeeman field by <strong>th</strong>e isotropic hyperfine coupling.<br />
-- 1 99 l HIGH PRESSURE 13C CROSS-POLARIZATION AND SPIN RELAXATION STUDY OF<br />
ADAMANTANE: K.O. Prins and D. van der Putten, Van der Waals Laboratory, University<br />
of Amsterdam, Postbus 20216, 1000 HE Amsterdam, The Ne<strong>th</strong>erlands.<br />
The poster presents a description of a double resonance probe suitable for IH-I~C<br />
cross-polarization experiments at hydrostatic pressure up to 10 kbar. The probe is<br />
placed in a liquid nitrogen cryostat, constructed inside <strong>th</strong>e 13 cm bore of a 4.2 T<br />
superconducting magnet.<br />
Cross-polarization has been used in a study of <strong>th</strong>e effect of high pressure on<br />
molecular reorientation in <strong>th</strong>e orientationally disordered solid phase I and in <strong>th</strong>e<br />
ordered phase II of adamantane. It is shown <strong>th</strong>at knowledge of <strong>th</strong>e iH and 13C<br />
relaxation times T and T allows distinction between isotropic rotational diffusion<br />
i 10<br />
and discrete reorientations in <strong>th</strong>e two solid phases. In phase I adamantane spends<br />
a non-negligible time between its equilibrium orientations. In phase II <strong>th</strong>e experimen-<br />
tal results are well described by a discrete reorientational model. A broadening of<br />
<strong>th</strong>e 13C resonance observed while spin-locking <strong>th</strong>e protons occurs at increasing<br />
pressure.<br />
198