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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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176 Appendix B<br />

Figure 3 at the 90% statistical confidence level. The T 3/2 term in Fe and Ni is<br />

quite small but has nevertheless been extracted from the heat capacity data<br />

[200-202].<br />

γ(H) (mJ/mol-K 2 )<br />

Field Dependence of the Density of States in SrRuO 3<br />

38<br />

37<br />

36<br />

35<br />

34<br />

34<br />

33<br />

32<br />

Predicted from M vs. T<br />

Single Crystal Data<br />

0 2 4 6 8<br />

Magnetic Field (Tesla)<br />

Figure B- 3. The linear term of the heat capacity γ as a<br />

function of magnetic field. Each circle is from a single c P,H<br />

datum between 4.3 and 5 K with phonons subtracted: γ(H) =<br />

(c P,H (T) - βT 3 )/T with β = 0.191 mJ/mol·K 4 . γ(H) for each square<br />

was determined by fitting 15-20 data points between 6 and 12 K<br />

to: c P,H (T) = γT + βT 3 . The triangles are calculated from the<br />

magnetization data of a single crystal.<br />

The linear-T term, γ, is significantly depressed in an 8 T magnetic field.<br />

The inset to Figure B- 1 shows the difference between the zero-field cooled<br />

data in zero field and each of the other two data sets, plotted as ∆c/T. The data

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