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Magnetic hyperfine field variation with temperature

Fig. 2. Qualitative variation of the nuclear magnetic resonance frequency with the strength of an applied external field for a spherical ferromagnetic sample with negligible magnetic anisotropy and isotropic, positive hyperfine field at low temperature (saturated magnetization). Fig. 2. Qualitative variation of the nuclear magnetic resonance frequency with the strength of an applied external field for a spherical ferromagnetic sample with negligible magnetic anisotropy and isotropic, positive hyperfine field at low temperature (saturated magnetization).
Figure 4. Temperature variation of the a, /3t, and P-2 fluorine hyperfine splittings of the 300°K radical with the magnetic field parallel to a, b, and c. The spectra become too complex to analyze where the curves are shown dashed. From Reference 12. Figure 4. Temperature variation of the a, /3t, and P-2 fluorine hyperfine splittings of the 300°K radical with the magnetic field parallel to a, b, and c. The spectra become too complex to analyze where the curves are shown dashed. From Reference 12.

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