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The metal-semiconductor transition in amorphous Si1-x Crx films: phenomenological model for the metallic region
Authors:A Möbius
Institution:(1) Zentralinstitut für Festkörperphysik and Werkstofforschung der Akademie der Wissenschaften der DDR, DDR-8027 Dresden, German Democratic Republic
Abstract:A detailed phenomenological re-analysis of previously published conductivity data, sgr(T, x), is presented. It was shown in 1] that the cusp-like low-temperature contribution can be described by 
$$\bar \beta (x) \cdot T^p $$
wherep=0.19±0.03. Starting from this result, two furtherT dependent contributions are separated: The high-temperature region is dominated by a positive contribution sgrht (T, x), which is approximately independent ofx, nearly linear inT above 100 K and nearly quadratic inT below 30 K. ForTlap 4 K, there is a small deviation, increasing withT, from the superposition of the above mechanisms. The relation between 
$$\bar \beta $$
, being negative, and theT independent part, 
$$\bar \alpha $$
, exhibits a singularity, 
$$\bar \beta  \sim (\bar \alpha  - \bar \alpha _0 )^\vartheta  $$
where 
$$\bar \alpha _0  = 270 \pm 50 \Omega ^{ - 1}  cm^{ - 1} $$
andthetav=0.68±0.05 –(p–0.19). This singularity should be related to the metal-semiconductor transition, taking place atT c ap0.14. The quantity 
$$\bar \alpha _0 $$
should be interpreted as minimum metallic conductivity. The limitingT dependences asxrarrx c +0 agrees quantitatively with that one obtained previously for the activated region,xrarrx c –0. Extrapolation of the phenomenological model obtained leads to the hypothesis that the interplay of 
$$\bar \beta  \cdot T^p $$
and sgrht could be the main origin of the temperature coefficient changing its sign in the Mooijregion, at sgr tc=0. The model enables several trend predictions concerning the value of sgr tc=0.
Keywords:
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