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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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24 Chapter 3<br />

Hall effect measurements have several assumptions which need to be<br />

considered. First, since it is basically a resistance measurement, the I vs. V<br />

curve should be checked and V 0 subtracted as above. Second, it is often<br />

assumed that the Hall voltage is linear in the applied magnetic field<br />

E y = j x R H H. This is often not the case, as described above (section 3.1.1.4) for<br />

magnetic materials or semiconductors with more than one type of carrier.<br />

Finally, the effect of the magnetoresistance needs to be subtracted.<br />

Traditionally, and theoretically this can be done by balancing the Hall voltage<br />

so that it reads zero at H = 0, and then the magnetoresistance should also be<br />

subtracted for H ≠ 0. In practice, this does not work. There is usually some<br />

magnetoresistive component in the measurement perhaps due to some<br />

anisotropy or inhomogeneity in the material. Since the magnetoresistance is<br />

an even function of H while the Hall effect is an odd function of H, I have<br />

found it easiest to examine the Hall effect by plotting V y (H) - V y (-H) as a<br />

function of H. This give the antisymmetric portion of the Hall voltage<br />

(subtracting the symmetric magnetoresistive contribution) without assuming<br />

a Hall effect which is linear in the applied field H.<br />

3.1.2.2 Geometry<br />

In order to calculate the resistivity from the measured resistance, the<br />

geometric ratio relating the two must be known. Most analyses are based o n<br />

some temperature or field dependence, and therefore it is more important<br />

that this geometric factor does not change during the experiment than it is to<br />

know the value precisely. The geometrical factor can change if the sample<br />

has internal cracks or if the contacts are flowing or cracking.<br />

For resistivity measurements, the resistance of the entire circuit must be<br />

taken into account. A tiny metallic sample may have a resistance much<br />

smaller than that of the contacts or even the wires leading to the voltmeter.<br />

For this reason, four probe measurements are used. A known current is<br />

applied through the sample from two of the contacts. The voltage across a

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