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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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 (%)