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Kazumasa Yamada

Publications and source records attributed to Kazumasa Yamada.

2 recordsLinked to original sources

Weak Localization and Magnetoconductance in Percolative Superconducting Aluminum Films

In order to investigate the crossover from the homogeneous behavior to inhomogeneous (percolative) one, the temperature $T$ and magnetic field H dependence of the sheet resistance $R_\square$ have been measured for two-dimensional granular aluminum films. Fitting the theory to data of magnetoconductance near $T_C$ with use of the diffusion constant $D(T)$ as a fitting parameter, we have obtained the anomalous $T$-dependent diffusion constant $D$. From the analysis of $D(T)$, the electron diffusion index $θ$, a certain critical exponent in percolation theory, has been obtained. In the relation $R_\square-θ$, the value of $θ$ varies abruptly near $1.5kω$. This behavior suggesting the above mentioned crossover is similar to our previous results determined from the temperature dependence of the upper critical field. For percolative films in $H = 5\mathrm{T}$, we have found the strong $R_\square$ dependence of the prefactor $α_T$ in the expression$σ=[α_T e^2/(2π^2\hbar)]\ln T+σ_0$. The relation $α_T\propto1/R_\square$ can be explained qualitatively by a model of scaling law for percolation.

cond-mat.supr-con↗

Temperature dependence of mobility of conducting polymer polyaniline with secondary dopant

The conductivity $σ$ and carrier density $n$ of the conducting polymer polyaniline were investigated by changing the concentration $x$ of a secondary dopant, meta-cresol. We found that $σ$ changes by four orders of magnitude within the $x$-range of 1-10 %, while $n$, as estimated from the Hall measurements, shows a weak dependence on $x$ in the region of 2% <$x$< 50%. These results suggest that $σ$ can be enhanced by the change in the mobility $μ$. We analyzed the temperature dependence of $μ$ by not only the combination of two different types of scattering mechanism, but also by the polaron hopping model. The experimental data of $μ(T)$ can be explained well by the latter model with reasonable fitting parameter values of a small-polaron binding energy and a longitudinal optical phonon frequency.

cond-mat.mtrl-sci↗