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Temperature dependence of magnetic

Ishikawa etal. proposed an approach for the determination of the ligand-field (LF) parameters of a set of isostructural lanthanide complexes. This method consists of a simultaneous fit of the temperature dependence of magnetic susceptibilities and NMR spectra for the whole isostructural series [18]. In order to avoid over-parametrization a key restriction is imposed each parameter is expressed as a linear function of the number of f electrons, n ... [Pg.31]

Fig. 3 For 3 Ln, left temperature dependence of magnetic susceptibilities right impendence spectroscopy of the electrical resistances at room temperature... Fig. 3 For 3 Ln, left temperature dependence of magnetic susceptibilities right impendence spectroscopy of the electrical resistances at room temperature...
Temperature dependence of magnetic susceptibility of the PF6 salt was measured from 300 to 4 K at 5 T [35], The spin susceptibility of this salt gradually decreases from 300 to 50 K. Below 50 K, the susceptibility exhibits a rapid decrease accompanied by anisotropic temperature dependence, which is an indication of the long-range antiferromagnetic ordering. A one-dimensional Heisenberg model is... [Pg.47]

The temperature dependence of magnetic susceptibility x measured on single crystals reveals magnetic ID behaviour. Below 50 K x is strongly anisotropic with the trigonal axis corresponding to the easy axis of magnetization and therefore to... [Pg.272]

Harrison R.J. and Putnis A. (1999) Determination of the mechanism of cation ordering in magnesioferrite (MgFe204) from the time- and temperature-dependence of magnetic susceptibility. Phys. Chem. Miner. 26, 322-332. [Pg.604]

Figure 9 Left Schematic representation of chemical or UV-induced synthesis of Pt nanowires and nanoparticles in zeolites FSM-16. Right Comparison of temperature dependence of magnetization for Pt nanowires and nanoparticles in FSM-16. (From Ref. 137.)... Figure 9 Left Schematic representation of chemical or UV-induced synthesis of Pt nanowires and nanoparticles in zeolites FSM-16. Right Comparison of temperature dependence of magnetization for Pt nanowires and nanoparticles in FSM-16. (From Ref. 137.)...
Figure 6.50 Temperature dependence of magnetic snsceptibility for a paramagnetic material. From K. M. Ralls, T. H. Conrtney, and J. Wnlff, Introduction to Materials Science and Engineering. Copyright 1976 by John Wiley Sons, Inc. This material is nsed by permission John Wiley Sons, Inc. Figure 6.50 Temperature dependence of magnetic snsceptibility for a paramagnetic material. From K. M. Ralls, T. H. Conrtney, and J. Wnlff, Introduction to Materials Science and Engineering. Copyright 1976 by John Wiley Sons, Inc. This material is nsed by permission John Wiley Sons, Inc.
Figure 6.25 (a) The chiolite structure (b) temperature dependence of magnetization of NajMjFj chiolites. (After Tressaud Dance, 1977.)... [Pg.338]

Even for complexes that do not exhibit spin crossover, the temperature dependence of magnetic properties can provide very important information. Pierre Curie established in 1895 that paramagnetic susceptibility is inversely proportional to the absolute temperature (Fig. 11.57a) ... [Pg.245]

Fig. 22 Temperature dependence of magnetic functions (level-6) for different axial crystal-field strength F4(z) of Ti(III) complexes. From left to right Fnixy) = 4000, 8000, 13000, and 18000 cnr1. Black lines refer to the regular octahedron. Note temperature axis runs oppositely between the top and bottom panels... Fig. 22 Temperature dependence of magnetic functions (level-6) for different axial crystal-field strength F4(z) of Ti(III) complexes. From left to right Fnixy) = 4000, 8000, 13000, and 18000 cnr1. Black lines refer to the regular octahedron. Note temperature axis runs oppositely between the top and bottom panels...
What should be taken into account to describe well the temperature dependence of magnetization ... [Pg.633]

Abstract. Two forms of CoO have been prepared from spec, pure Co metal and CoC03 and the magnetic susceptibility of CoO(I) and CoO(II) examined over a temperature range300-700 deg. K. The magnetic data of CoO(II) have shown an anomalous temperature dependence of that in this temperature range CoO(II) passes into CoO(I). This result is in conformity with Mossbauer spectra. Furthermore, D.T.A and temperature dependence of magnetic susceptibility of CoO(II) arises from a first order phase transition. [Pg.564]

During the measurements of the temperature dependence of magnetization (a(T)), the sample has been placed in a chamber with constant hydrogen pressure. In order to determine the hydrogen concentration x in the sample at any temperature (x(T)), a volumetric type experimental set-up [10, 11] has been used to study the hydrogen absorption-desorption properties at hydrogen pressures up to 4 atm in the temperature range from 300 to 700 K. [Pg.606]

Figure 1. Temperature dependencies of magnetization and hydrogen concentration for Er2Fei4BHx at hydrogen pressure P = 2.5 atm. Figure 1. Temperature dependencies of magnetization and hydrogen concentration for Er2Fei4BHx at hydrogen pressure P = 2.5 atm.
Figure 1. Temperature dependence of magnetization measured along the a-axis in magnetic field of 0.1 kOe for the Lu2Fe17 single crystal. Figure 1. Temperature dependence of magnetization measured along the a-axis in magnetic field of 0.1 kOe for the Lu2Fe17 single crystal.

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