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Ndo.5Sro

Fig. 51. (a) Temperature dependence of the resistivity p(T) of Ndo.5Sro.5MnC>3 under various magnetic fields, (b) Temperature-field phase diagram after Shimomura et al. (1999). [Pg.327]

Figure 11. Temperature variation of (a) the magnetization and (b) the resistivity of Ndo.5Sro.5Mn03 (from Kuwahara et al.17). Figure 11. Temperature variation of (a) the magnetization and (b) the resistivity of Ndo.5Sro.5Mn03 (from Kuwahara et al.17).
Figure 13. Temperature-magnetic field phase diagram for Ndo.5Sro.5-Mn03 (from Tokura et al,18). Figure 13. Temperature-magnetic field phase diagram for Ndo.5Sro.5-Mn03 (from Tokura et al,18).
Figure 61 shows the ZFC and FC M(T) curves for the FMM phase II, which show a first-order transition at 7c where the bond-length fluctuations become frozen out to restore the phonon contribution to the thermal conductivity, fig. 62. In the I + II two-phase samples t = 0.973 and t = 0.974, phase II is suppressed and phase fluctuations inhibit phonon formation below Tco or 7c. Tokura et al. (1996) applied hydrostatic pressure to the FM phase II of (Ndo.i25Smo.875)o.5Sro.5Mn03 having / /c they reported the appearance of a CE AFI second phase having a volume fraction that increased with pressure below Too = 7n- Since pressure... [Pg.341]


See other pages where Ndo.5Sro is mentioned: [Pg.326]    [Pg.337]    [Pg.290]    [Pg.293]    [Pg.295]    [Pg.296]    [Pg.312]    [Pg.9]    [Pg.9]    [Pg.10]    [Pg.289]    [Pg.290]    [Pg.290]    [Pg.293]    [Pg.293]    [Pg.294]    [Pg.295]    [Pg.102]    [Pg.102]    [Pg.326]    [Pg.337]    [Pg.290]    [Pg.293]    [Pg.295]    [Pg.296]    [Pg.312]    [Pg.9]    [Pg.9]    [Pg.10]    [Pg.289]    [Pg.290]    [Pg.290]    [Pg.293]    [Pg.293]    [Pg.294]    [Pg.295]    [Pg.102]    [Pg.102]    [Pg.288]    [Pg.247]   
See also in sourсe #XX -- [ Pg.3 , Pg.5 , Pg.326 , Pg.337 ]




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