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We have measured the thermopower and resistivity of vapor-deposited amorphous Cu-Ti films of widely varying composition, at temperatures from 4.2 to 300 K. An explanation of the temperature variation in resistivity, but not in thermopower, requires a mechanism additional to the temperature dependence of the structure factor in the Ziman-Faber model. The magnitude of the resistivity, its temperature variation, and the thermopower are all larger in a Cu₄₇{Ti}₅₃$ film than in corresponding melt-spun metallic glass ribbons, indicating greater disorder scattering, but differences between Cu-rich films and ribbons are more complex.
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Rathnayaka et al. (1986) studied this question.
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