The magnetization M(H) has been measured in the weakly helimagnetic itinerant compound MnSi under high pressure up to 10.2 kbar and high magnetic field up to 9 Tesla. We interpret the simultaneous decrease under pressure of the saturated magnetization, ps, and the Curie temperature, Tc in the frame of the self-consistent renormalization theory (SCR) of spin fluctuations. From the analysis of the so-called Arrot-plot (H/p[H,T] versus p2 [H,T]) and the respective volume dependence of ps and Tc, we estimate the evolution of the characteristic spin fluctuation temperatures, T0 and TA when the system approaches its critical pressure, Pc=15 kbar, corresponding to the disappearance of the long range magnetic order at T = 0.
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Thessieu et al. (1998) studied this question.
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