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Magnetic moment equilibrium

In Eq. (41), Phs and Pls are the limiting values for the magnetic moment of the HS and LS state, respectively. Relaxation processes are introduced by a slight disturbance of the equilibrium, the equilibrium concentration of the components being changed by the same amount x according to ... [Pg.71]

Nickel(II) complexes of (505) exhibit spin equilibria in solution.1355 With the bidentate analogues (506), complexes [Ni(506)2] have been isolated.1356 When Rj = Ph, the complex is tetrahedral in solution. It has a temperature independent magnetic moment of 2.75pB- When R = Me, the complex exhibits square planar-tetrahedral equilibrium in solution. Both are, however, diamagnetic in the solid state. [Pg.366]

The solution of this equation is a precession of the vector M around H0 with an angular velocity equilibrium value. In order to explain how the spins approach their equilibrium distribution we must take account of the interactions of the spins among themselves and with the other degrees of freedom of the system. The simplest phenomenological description of the approach to equilibrium of an assembly of magnetic moments, placed in a constant field H0, is given by the equations... [Pg.291]

Magnetic susceptibilities of solutions — These are useful parameters for determining equilibrium constants for reactions involving spin changes. The Evans nmr method utilizes the observed shift in the resonance line (say of a proton of t-BuOH or hexamethyldisilox-ane) in solution when a paramagnetic substance is added. The paramagnetic shift A/ is related to the magnetic moment (jj, of the solution at TK by the approximate expression... [Pg.338]

At high temperatures, a nanoparticle is in a superparamagnetic state with thermal equilibrium properties as described in the previous section. At low temperatures, the magnetic moment is blocked in one potential well with a small probability to overcome the energy barrier, while at intermediate temperatures, where the relaxation time of a spin is comparable to the observation time, dynamical properties can be observed, including magnetic relaxation and a frequency-dependent ac susceptibility. [Pg.207]

The Point Charge Concept and the Related Divergence Quantized Charged Equilibrium B.4.1. Conditions on Spin and Magnetic Moment... [Pg.2]

Remark. We assumed that Y(t) is a Markov process. Usually, however, one is interested in materials in which a memory effect is present, because that provides more information about the microscopic magnetic moments and their interaction. In that case the above results are still formally correct, but the following qualification must be borne in mind. It is still true that p y0) is the distribution of Y at the time t0, at which the small field B is switched off. However, it is no longer true that this p(y0) uniquely specifies a subensemble and thereby the future of Y(t). It is now essential to know that the system has aged in the presence of B + AB, so that its density in phase space is canonical, not only with respect to Y, but also with respect to all other quantities that determine the future. Hence the formulas cannot be applied to time-dependent fields B(t) unless the variation is so slow that the system is able to maintain at all times the equilibrium distribution corresponding to the instantaneous B(t). [Pg.89]


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See also in sourсe #XX -- [ Pg.69 ]




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