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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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160 Appendix A<br />

(T/T C - 1) γ . From these data (Figure A- 4) γ = 1.17 ± 0.02 is estimated. The plot<br />

of 1/χ vs. T should be close to linear for high temperatures.<br />

2 )<br />

M 2 × |T/T C - 1| -2 β (µ B<br />

6.0<br />

5.0<br />

4.0<br />

3.0<br />

2.0<br />

1.0<br />

SrRuO 3 Crystal Scaled Arrott Plot<br />

T < T C<br />

T > T C<br />

0.0<br />

0 500 1000 1500 2000 2500<br />

H/M × |T/T - 1|<br />

C -γ (kOe/µ )<br />

B<br />

The M(H, T) data can be replotted using the scaling hypothesis [90] with<br />

β = 0.36 and γ = 1.17. According to the hypothesis, the magnetic equation of<br />

state in the critical region depends only on the scaled variables H/|T C /T - 1| β+γ<br />

and M/|T C /T - 1| β . A plot of the scaled M 2 and scaled H/M, shown in<br />

Figure A- 5, will then have only two curves: one branch for the T < T C data<br />

and another for T > T C . Not all the curves fit on a single line, this is due to<br />

the apparent change in β as discussed above.<br />

β = 0.36<br />

γ = 1.17<br />

T C =163.2K<br />

Figure A- 5. Scaled Arrott Plot of SrRuO 3 single crystal along<br />

easy [110] direction with β = 0.36 and γ =1.17. Symbols are the<br />

same as those used in Figure A- 2.<br />

The critical isotherm (T = T C ) should obey the relation M δ ∝ H, where<br />

according to the scaling relation δ = γ/β + 1. From the previously measured<br />

values of β and γ, the exponent δ is therefore expected to be 4.3 ± 0.5. This is<br />

in good agreement with the measured value (Figure A- 2) δ = 4.2 ± 0.2.

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