The quantitative simulation of the electron nuclear double resonance (ENDOR) spectra of low‐symmetry, randomly oriented molecules is discussed with particular attention paid to those systems where electron cross relaxation effectively couples the spin packets of the electron paramagnetic resonance (EPR) spectrum. ENDOR transition frequencies are calculated employing the high field approximation; frequency shifts arising from g anisotropy and the SxIx and SyIy terms of the hyperfine Hamiltonian are then evaluated by perturbation theory. ENDOR signal intensities are considered to be determined by transition moments and by electron and nuclear spin relaxation processes. The ENDOR spectra of polycrystalline samples of the x‐irradiated aliphatic diacids, HOOC(CH2)nCOOH where n=1 to 8, and the alicyclic diacids, (CH2)mC(COOH)2 where m=2 to 4, have been recorded at 4.2°K and theoretical spectra computed. Reasonably good agreement is observed between experimental spectra and spectra computed assuming complete coupling of the spin packets by cross relaxation and isotropic relaxation rates. These assumptions are compatible with pulsed microwave measurements of electron relaxation rates.

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We have attempted to measure nuclear spin‐lattice, spin‐spin, and spin diffusion times by nuclear spin echo methods; unfortunately, poor signal to noise ratios have prevented definitive evaluation of relaxation times. Likewise, attempted analysis of nuclear relaxation times from ENDOR signal decay kinetics following application of pulsed rf fields and investigation of stationary saturation behavior has yielded only semiquantitative information. However when correlated with precise electron relaxation data, the above measurements can be used to establish limits for the effective nuclear relaxation times T1N and T2N.
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