The pressure induced quantum phase transition of the weakly ferromagnetic metal MnSi is studied using zero-field ²⁹Si NMR spectroscopy and relaxation. Below P*≈1.2 GPa, the intensity of the signal and the nuclear spin-lattice relaxation are independent of pressure, even though the amplitude of the magnetization drops by $20%$ from the ambient-pressure amplitude. For P>P*, the decreasing intensity within the experimentally detectable bandwidth signals the onset of an inhomogeneous phase that persists to the highest pressure measured, P≥1.75 GPa, which is well beyond the known critical pressure Pc=1.46 GPa. Implications for the non-Fermi liquid behavior observed for P>Pc are discussed.
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Yu et al. (2004) studied this question.
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