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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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Resistivity (10 -3 Ω cm)<br />

10<br />

8<br />

6<br />

4<br />

2<br />

Resistivity (10 -3 Ω cm)<br />

10<br />

9<br />

8<br />

7<br />

6<br />

5<br />

Intrinsic Properties of La 0.67 Ca 0.33 MnO 3<br />

La 0.67 Ca 0.33 MnO 3 Magnetoresistance<br />

La 0.67 Ca 0.33 MnO 3 Film<br />

Magnetization<br />

0 kOe<br />

∆R (0-70 kOe)<br />

240 245 250 255 260 265 270<br />

Temperature(K)<br />

0 kOe<br />

70 kOe<br />

0<br />

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

Temperature(K)<br />

Figure 4-7 Magnetoresistance of La0.67Ca0.33MnO3 film<br />

(LCM17). Inset, simultaneous magnetization and resistivity at<br />

20Oersted, along with the magnetoresistance [R(H = 0kOe) -<br />

R( H = 70kOe)].<br />

approximately linear with field (Figure 4-8). This effect is small enough for<br />

the analysis to be carried out with R 0 independent of magnetic field.<br />

Since polycrystalline material contains a significant contribution to the<br />

resistivity from grain or domain boundaries, as shown by microwave<br />

measurements [109-111] and higher R 0 values, analysis of the resistivity data<br />

is made only for the well annealed films and crystals. Data up to 70K and<br />

100K for La 0.67 Ca 0.33 MnO 3 and La 0.67 Sr 0.33 MnO 3 , respectively, are well described<br />

with an additional (R 2 ) term proportional to T 2 (Figure 4-8). A linear term in<br />

T did not significantly improve the fit and was not used in later calculations<br />

in order to keep the number of free parameters to a minimum. The field<br />

Magnetization (relative units)<br />

87

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