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MAGNETISM ELECTRON TRANSPORT MAGNETORESISTIVE LANTHANUM CALCIUM MANGANITE

MAGNETISM ELECTRON TRANSPORT MAGNETORESISTIVE LANTHANUM CALCIUM MANGANITE

MAGNETISM ELECTRON TRANSPORT MAGNETORESISTIVE LANTHANUM CALCIUM MANGANITE

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62 Chapter 3<br />

Curie temperature, the temperature where the linear extrapolation of the 1/χ<br />

curve crosses 1/χ = 0. Near the critical temperature however, 1/χ is not<br />

necessarily linear in T since 1/χ = (T - T C ) γ where γ is usually large than 1.<br />

Thus the paramagnetic Curie temperature is usually slightly larger than the<br />

true critical temperature.<br />

In principle the thermodynamic critical temperature can be found by<br />

fitting the divergence of all the measured quantities and using the scaling<br />

relations. This assumes a true critical region has been reached where the<br />

critical exponents do not change. The simpler method using the Arrot plots,<br />

described in the previous section (3.2.2.2.6) can give as accurate results. Thus,<br />

the Arrott T C is probably the best simple way of finding the critical<br />

temperature.<br />

The most basic definition of T C for a ferromagnet is the temperature where<br />

the spontaneous magnetization drops to zero (as the temperature is raised).<br />

Unfortunately due to demagnetization effects, the zero applied field<br />

magnetization will drop to zero at T C faster and less uniformly than expected.<br />

Nevertheless, the temperature where the magnetization, measured in zero or<br />

small applied field, is often used to measure the critical temperature and is<br />

called here the remnant T C .<br />

In an applied field, the magnetization does not drop to zero because of the<br />

large susceptibility near T C . However, below T C the magnetization has a<br />

negative curvature while above T C it has a positive curvature. Thus the<br />

inflection point of the M vs. T curve (denoted here as the inflection T C ) is<br />

often used to measure the Curie temperature. In the mean field model, the<br />

inflection T C is quite close to the real critical temperature. Figure 3-7 shows<br />

the calculated M vs. T of SrRuO 3 in various fields. In a 5 T applied field, the<br />

inflection point is 1.6 K higher than the true T C used for the calculation. This<br />

agrees well with the experimental data shown in Figure 3-9, where the

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