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s = -1/2 level is not the ground state. Hence, one effective means of suppressing the Mn(II) signals is to reduce the observation temperature. This has the added advantage that the resonances arising from the mixed valence complexes become more intense with decreasing temperature since these signals arise from the ground state. The only disadvantage of using lower temperatures is the increased potential for saturation and passage artifacts. The spectra shown in Figures 2 and 3 were free of such artifacts.
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46
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11744262845
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note
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The fatting procedure started with the generation of 500 random starting points. These initial points were centered about the approximate g value corresponding to the center of the spectrum and 210 and 410 MHz for the two hyperfine couplings. The random starting points were distributed over a range of ±0.03 for G and ± 50 MHz for both hyperfine couplings. The resulting 500 minimized sets were sorted according to the RMS residual and the 50 best were retained and analyzed. In all cases, these 50 represented a single consistent set of the nine spin parameters. The spin parameters were further refined by a separate fitting of the 9 GHz data. Five hundred random starting points were generated centered about the mean value of the set of 50 best parameters. To ensure consistency between the 9 and 285 GHz data, a final round of minimization was carried out on the 285 GHz data using the 9 GHz refined estimates. For the high-field spectra, regions that contains large contribution from Mn(II) were excluded from the rms calculation. These regions did not contribute to the minimization.
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11744388223
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We use the fact that the g tensor equations can be rigorously separated into two independent equations, one for the isotropic value and the other for the anisotropic component.
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