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MAGNETISM ELECTRON TRANSPORT MAGNETORESISTIVE LANTHANUM CALCIUM MANGANITE

MAGNETISM ELECTRON TRANSPORT MAGNETORESISTIVE LANTHANUM CALCIUM MANGANITE

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T 2 Coefficient (10 -6 /K 2 )<br />

Critical Behavior and Anisotropy in Single Crystal SrRuO 3<br />

50<br />

40<br />

30<br />

20<br />

10<br />

-10<br />

0 25 50 75 100 125 150<br />

Maximum Temperature of Fitting Range<br />

ferromagnets such as ZrZn 2 , Ni 3 Al and Sc 3 In, show n = 2 [86, 193-195] over a<br />

wide temperature range.<br />

0<br />

As shown above (Figure A- 6) the magnetization of SrRuO 3 single crystal<br />

can be well described by M = M S (1 - (T/Θ n ) n ) with n = 2 in the temperature<br />

range of reliable measurement, 5 K to 100 K. A fit with n = 3/2 in this<br />

temperature range is unsatisfactory.<br />

B parameter in fit to M = M 0 (1 - AT 3/2 - BT 2 )<br />

7T T 2 term<br />

6T T 2 term<br />

5T T 2 term<br />

4T T 2 term<br />

3T T 2 term<br />

2T T 2 term<br />

1T T 2 term<br />

2kOe T 2 term<br />

1kOe T 2 term<br />

Figure A- 9. Variation of the T 2 parameter in fitting the<br />

magnetization data of single crystal SrRuO 3 to M = M S (1 -<br />

AT 3/2 - BT 2 ) as the fitting range is increased. In the region<br />

where B is relatively stable (around T max = 60 K), B increases as<br />

T max is lowered.<br />

If one assumes n = 2 arises from Stoner excitations and collective<br />

excitations result in n = 3/2, then one may expect the variation of<br />

167

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