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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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Specific Heat of SrRuO 3<br />

energy magnetic excitations than the saturation magnetization, particularly<br />

for polycrystalline samples with large magnetocrystalline anisotropy such as<br />

SrRuO 3 .<br />

Like the magnetization measurements, the heat capacity measurements<br />

can be well described by a decrease in the magnetization proportional to T n<br />

where n ≈ 2. This can be understood by any of three mechanisms. First, if the<br />

corrections are included in the spin wave theory then an effective n > 3/2 is<br />

predicted. Second, single particle excitations are present. Third, the<br />

excitations interact (requiring a more generalized description [85]) to give an<br />

effective exponent n ≈ 2.<br />

The same phenomena can also be interpreted as a spin fluctuation<br />

enhancement of the electronic specific heat, which can be suppressed by a<br />

magnetic field.<br />

The help of K. A. Moler for the heat capacity measurements is greatly<br />

appreciated.<br />

181

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