Magnetization determination

Fig. 4.1.3 Intrinsic magnetization determined by the relaxation data corresponding to the selected voxel in the Bentheimer sample.

Ito H, Watanabe M, Nogami Y, Ishiguro T, Komatsu T, Saito G, Hosoito N (1991) Magnetic determination of Ginzburg-Landau coherence length for organic superconductor /c-(BEDT-TTF)2X (X = Cu(NCS)2, Cu[N(CN)2]Br) effect of isotope substitution. J Phys Soc Jpn 60 ... 

Fig. 9. Magnetic field dependence of the magnetization at selected temperatures for a 150-nm thick Ga xMn As film with a Mn composition x = 0.03S. The magnetic field is applied parallel to the sample surface (direction of magnetic easy axis) except for the closed circles at 5 K taken in perpendicular geometry. The solid line for S K shows the magnetization determined from transport measurements. The upper left inset shows a magnified view of the magnetization in the parallel field at 5 K. The lower right inset shows the temperature dependence of the remanent magnetization (Ohno et al. 1996a).

Fig. II. (a) Temperature dependence of the magnetization for 200-nm thick Ga, MnrAs with x =0.053. The magnetic field is applied perpendicular to the sample surface (hard axis). The inset shows the temperature dependence of the remanent magnetization (0 T) and the magnetization at 1 T in a field parallel to the film surface, (b) Temperature dependence of the saturation magnetization determined from the data shown in (a) by using ArTott plots (closed circles). Open circles show inverse magnetic susceptibility and the Curie-Weiss fit is depicted by the solid straight line (Ohno and Matsukura 2001).

Fig. 21. Faraday rotation for a 2- m thick film of Ga Mn.rAs with x = 0.043 measured as a function of the photon energy in a magnetic field of 6 T at 10 and 300 K (a) and as a function of the magnetic field at 10 K, 1.55 eV and at 300 K, 1.49 eV (b). Solid lines show the magnetization determined from magnetotransport measurements at the given temperatures (scaled to match the open symbols) (Kuroiwa et al. 1998).

Magnetic Determination of Structure and Electron Density in Functioning Catalytic Solids... 

Brushless DC drives have an advantage in that the motor does not contain brushes. As a result, the drive is less maintenance intensive. The motor contains permanent magnets the size of the magnets determines the horsepower capability of the motor. The maximum power available today is around 600 hp. A schematic of the brushless DC drive is shown in Fig. 3.6. 

The lanthanide contributions to the magnetization, determined by magnetic measurements coincides generally with the gJ values (Burzo 1984, 1985b, Boltich et al. 1985, Yamauchi et al. 1986). Friedt et al. (1984) and Gubbens et al. (1985,... 

In contrast to the conventional behavior described above, almost no evidence of a critical anomaly at the magnetization-determined Tc is observed in amor phous TbFe (or HoFe2) as shown in fig. 16.16a. Only a weak inflection in the scattering is observed at Tc which is not sharp, but of a rounded character as... 

With purine and derivatives [Co(OHy6-C,H,N NH3)] ) 293- 79 11820 4.66 42 sign of 6>p uncertain magnetism determined from Curie-Weiss law 69B40... 

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