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MAGNETISM ELECTRON TRANSPORT MAGNETORESISTIVE LANTHANUM CALCIUM MANGANITE

MAGNETISM ELECTRON TRANSPORT MAGNETORESISTIVE LANTHANUM CALCIUM MANGANITE

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86 Chapter 4<br />

Resistivity (10 -3 Ω cm)<br />

6<br />

5<br />

4<br />

3<br />

2<br />

1<br />

Resistivity (10 -3 Ω cm)<br />

5<br />

4<br />

3<br />

2<br />

La 0.67 Sr 0.33 MnO 3 Magnetoresistance<br />

La 0.67 Sr 0.33 MnO 3 Film<br />

R (H=0)<br />

∆R/R<br />

M<br />

340 345 350 355 360 365 370 375 380<br />

Temperature(K)<br />

Pellet 0kOe<br />

Pellet 70kOe<br />

Film 0kOe<br />

Film 70kOe<br />

0<br />

0 50 100 150 200 250 300 350 400<br />

Temperature (K)<br />

Figure 4-6 Magnetoresistance of La 0.67 Sr 0.33 MnO 3<br />

polycrystalline pellet and Film (LSM1). Inset, simultaneous<br />

magnetization and resistivity of the film at 20Oersted, along<br />

with the magnetoresistance [R(H = 0 kOe)-R(H = 70 kOe)].<br />

4. 2. 1 Low Temperature Resistivity<br />

Low temperature resistivity data were analyzed using a polynomial<br />

expansion in temperature T. Since the resistivity is essentially constant for<br />

temperatures less than 10K for all samples, it is clear that the resistivity data<br />

both with and without an applied field require a temperature independent<br />

(R 0 ) term. As shown previously for related compounds [29, 104, 108], R 0 is a<br />

function of magnetization in polycrystalline La 0.67 AE 0.33 MnO 3 (Figure 4-8) as<br />

discussed in section 4.2.8. In contrast, the magnetoresistance of films and<br />

crystals at 5 K is over 100 times less: it is not even measurable in the<br />

La 0.67 Ca 0.33 MnO 3 crystal where the precision is 0.5%. Due to the higher<br />

resistance of the films, the magnetoresistance at 5 K is measurable and is<br />

28<br />

26<br />

24<br />

22<br />

Magnetoresistance (%)

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