Single crystal magnetic

The second is the breakthrough in understanding complex 4f magnetism through the applications of some advanced magnetic measurements and quantum chemistry calculation methods, such as the single-crystal magnetic measurement... 

Figure 5.6 (A) Single-crystal magnetization data and best-fits for Na[Dy(DOTA)(H20)] 4H20 in a dc field of 1 kOe. The inset shows the magnetization at low temperatures plotted against the reduced variable H7" 1. The solid lines are the best-fit as described in...

Figure 6.2 (a) Orientation of the main magnetic axis in the ground Kramers doublet of [Cp ErCOT], [62]. Colour scheme Er, purple C, yellow H, white, (b) Polar plot of the angular dependence of the single-crystal magnetic susceptibility recorded in the a-b plane, comparison between the results of the... 

The structures of the anhydrous vanadiumfiii) sulphates, 2(804)3, yellow (monoclinic) and green (rhombohedral), have been investigated, and a new double sulphate, (NH4)3V(S04)3, has been prepared and extensively characterized. Single-crystal magnetic susceptibility studies (1.5—20 K) of guanidi-nium vanadium(iii) sulphate have been reported, and the zero-field splitting has been estimated as 3.74 cm . ... 

Figure 6.27 Single-crystal magnetic susceptibility data of CsNiFj. (After Tressaud Dance, 1982.) The solid line is the theoretical curve for Jjk = 10.2 K.

Pseudocontact shifts are estimated using single crystal magnetic susceptibility data. 

In conclusion, field dependent single-crystal magnetization, specific-heat and neutron diffraction results are presented. They are compared with theoretical calculations based on the use of symmetry analysis and a phenomenological thermodynamic potential. For the description of the incommensurate magnetic structure of copper metaborate we introduced the modified Lifshits invariant for the case of two two-component order parameters. This invariant is the antisymmetric product of the different order parameters and their spatial derivatives. Our theory describes satisfactorily the main features of the behavior of the copper metaborate spin system under applied external magnetic field for the temperature range 2+20 K. The definition of the nature of the low-temperature magnetic state anomalies observed at temperatures near 1.8 K and 1 K requires further consideration. 

Fig. 69. Single-crystal magnetic susceptibility data for (a) Ti203 and (b) V2O3. (After Carr and Foner (116).)...

All samples studied in [293] were obtained obtained by crushing of large single crystals, magnetic separation of iron, hot concentrated HCl leaching, and water washing of the powder. The powder was then stored in a Pyrex glass beaker under water. 

Single crystal magnetic susceptibihty and electrical resistivity data reveal valence-fluctuating behavior for CeNiln with a significantly anisotropic Kondo effect, which arises from anisotropic c-f mixing along the a and c axes (Fujii et al., 1989). At 2K,CfT reaches a value of 60 mJ/molK, which is ten times larger than that in LaNiln without 4/ electrons. The physical properties of CePdIn and CeNiln have been reviewed and compared to those of UPdIn (Fujii et al., 1992). 

Fig. 176. Fe fPOi), 4H,0, single crystal. Magnetization a as function of the field H along the h direction of crystal at several temperatures [68M12].

Fig. 264. CsjCoCIs, single crystal. Magnetization <7 as function of magnetic field strength for the temperatures 1.35 K, 2.36 K, 3.27 K and 4.23 K. The lowest set of four lines refers to the magnetic moment in the gj direction and the upper curves to those in the gj direction [67M22],...

Fig. 344. NaNiO, single crystal. Temperature dependence Fig. 345. NaNiO, single crystal. Magnetization <7 of a...

Fig. 11. CtjSj single crystal. Magnetization M measured at T = 75 K and T= 2.5 K as function of magnetic field //, for h parallel and perpendicular to the (001) axis [71P25].

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