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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7. Critical Transport and Magnetization of La 0.67Ca 0.33MnO 3<br />
In homogeneous La 0.67 Ca 0.33 MnO 3 , it is clear that the magnetoresistance<br />
maximizes near the ferromagnetic Curie temperature T C and rapidly<br />
decreases at lower or higher temperatures. The magnetoresistance also slowly<br />
saturates as the magnetic field is increased past several Tesla. Thus, the<br />
conductivity behaves much like the magnetization: above T C the<br />
conductivity and magnetization are low, while below T C the conductivity and<br />
magnetization rapidly increase. Furthermore, near T C both the conductivity<br />
and magnetic moment can be increased by an applied magnetic field. The<br />
theory of double exchange, which has been developed to explain these<br />
properties of the manganites [7, 112, 155], predicts this correlation between the<br />
conductivity and the magnetization.<br />
The relationship between the conductivity (or resistivity) and the<br />
magnetization has been examined both experimentally and theoretically.<br />
Several theoretical models [31, 112, 121, 155, 156, 161-164] predict an M 2<br />
dependence of the resistivity (or conductivity). The first term of the Taylor<br />
series expansion of the resistivity (or conductivity) in terms of M should be<br />
M 2 for all models due to symmetry considerations [150].<br />
Experimentally, a correlation between the resistivity and magnetization<br />
can be found by plotting one as a function of the other [24, 114, 115, 121, 158,<br />
165]. These plots show that the resistivity is roughly proportional to the<br />
square of the magnetization M 2 for small M. For larger M however, the<br />
resistance decreases more slowly in relationship to M 2 as if it were saturating<br />
before the magnetization does. Thus the relationship between the resistivity<br />
and the magnetization is more complicated than ρ ∝ M 2 . This relationship<br />
may instead be well described by an M 2 dependence of the conductivity in a<br />
slightly more complicated circuit [150]. In the previous chapter, only the<br />
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