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1.
Rev Sci Instrum ; 84(8): 084904, 2013 Aug.
Artigo em Inglês | MEDLINE | ID: mdl-24007093

RESUMO

A lock-in technique for measurement of thermal conductivity and volumetric heat capacity of thin films is presented. The technique is based on the 3ω approach using electrical generation and detection of oscillatory heat along a thin metal strip. Thin films are deposited onto the backside of commercial silicon nitride membranes, forming a bilayer geometry with distinct thermal parameters. Stepwise comparison to an adapted heat diffusion model delivers these parameters for both layers. Highest sensitivity is found for metallic thin films.


Assuntos
Condutividade Térmica , Impedância Elétrica , Membranas Artificiais , Compostos de Silício , Temperatura
2.
Beilstein J Nanotechnol ; 4: 461-6, 2013.
Artigo em Inglês | MEDLINE | ID: mdl-23946915

RESUMO

Based on chemically synthesized powders of FeGa3, CoGa3, as well as of a Fe0.75Co0.25Ga3 solid solution, thin films (typical thickness 40 nm) were fabricated by flash evaporation onto various substrates held at ambient temperature. In this way, the chemical composition of the powders could be transferred one-to-one to the films as demonstrated by Rutherford backscattering experiments. The relatively low deposition temperature necessary for conserving the composition leads, however, to 'X-ray amorphous' film structures with immediate consequences on their transport properties: A practically temperature-independent electrical resistivity of ρ = 200 µΩ·cm for CoGa3 and an electrical resistivity of about 600 µΩ·cm with a small negative temperature dependence for FeGa3. The observed values and temperature dependencies are typical of high-resistivity metallic glasses. This is especially surprising in the case of FeGa3, which as crystalline bulk material exhibits a semiconducting behavior, though with a small gap of 0.3 eV. Also the thermoelectric performance complies with that of metallic glasses: Small negative Seebeck coefficients of the order of -6 µV/K at 300 K with almost linear temperature dependence in the range 10 K ≤ T ≤ 300 K.

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