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MAGNETISM ELECTRON TRANSPORT MAGNETORESISTIVE LANTHANUM CALCIUM MANGANITE

MAGNETISM ELECTRON TRANSPORT MAGNETORESISTIVE LANTHANUM CALCIUM MANGANITE

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166 Appendix A<br />

T 3/2 Coefficient (10 -6 /K 3/2 )<br />

200<br />

150<br />

100<br />

50<br />

0<br />

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

-50<br />

0 25 50 75 100 125<br />

Maximum Temperature of Fitting Range<br />

150<br />

3.2.2.2.3) includes both types of interacting magnetic excitations and predicts<br />

n = 3/2 for H = 0, T = 0 but also n ≈ 2 in calculations [86].<br />

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

25<br />

20<br />

15<br />

Correlation of A and B<br />

10<br />

-20 0 20 40 60 80<br />

T 3/2 Coefficient (10 -6 /K 3/2 )<br />

Figure A- 8. Variation of the T 3/2 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. The upper inset<br />

shows the correlation of the A and B parameters. In the<br />

region where A is relatively stable (around T max = 60 K), A<br />

decreases as T max is lowered. The symbols are the same as<br />

those used in Figure A- 9.<br />

Experimental results on metallic ferromagnets with substantial saturation<br />

moments such as Fe, Ni [88, 189-192] and La 0.67 Sr 0.33 MnO 3 ([97], section 4.1.1)<br />

can display n = 3/2 consistent with the spin wave stiffness determined by<br />

neutron diffraction if significant corrections are included and only low<br />

temperature data is analyzed. In contrast “weak” itinerant-electron

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