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首页> 外文期刊>Journal of Applied Physics >Transport and structural properties of binary skutterudite CoSb_(3) thin films grown by dc magnetron sputtering technique
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Transport and structural properties of binary skutterudite CoSb_(3) thin films grown by dc magnetron sputtering technique

机译:Transport and structural properties of binary skutterudite CoSb_(3) thin films grown by dc magnetron sputtering technique

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摘要

The results of the studies of structural, electrical, and thermoelectric properties of binary skutterudite CoSb_(3) thin films are presented. The n-type films were prepared without intentional doping on oxidized Si(100) and ceramic Al_(2)O_(3) substrates using magnetron dc sputtering technique. The electron probe microanalysis has shown that the composition of the films is strongly affected by the preparation conditions. The x-ray measurements indicate the films to be amorphous if they are deposited on substrates kept at room temperature. On the basis of the differential thermal and x-ray analyses data, the temperature of the transition from the amorphous to crystalline state was established to be (153±1)℃. The films are polycrystalline with a preferential orientation of the growth along the (310) direction of the CoSb_(3) lattice if grown on substrates kept at 200℃. The electrical resistivity ρ(T) and the Seebeck coefficient S(T) were measured from room temperature up to about 700 K. The value of ρ(T) decreases with increasing temperature. The maximum absolute value of the Seebeck coefficient is found to be -250 μV/K at around 550 K for both substrates. This is the highest value of the Seebeck coefficient for CoSb_(3) films deposited by dc magnetron sputtering. The predominant mechanisms of the scattering in CoSb_(3) are discussed on the basis of the temperature dependence of the Hall mobility. The carrier concentration n(T) is found to be around 1.2×10~(19) cm~(-3) at 300 K and is almost constant over the temperature range of (250-400) K. The room temperature measurements of the thermal conductivity carried out by the 3ω method have shown a value of about 3 W/(m K), which is significantly lower than that reported for bulk material.

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