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Conductivity near the percolation threshold : ウィキペディア英語版
Conductivity near the percolation threshold

In a mixture between a dielectric and a metallic component, the conductivity \sigma and the dielectric constant \epsilon of this mixture show a critical behavior if the fraction of the metallic component reaches the percolation threshold.〔 The behavior of the conductivity near this percolation threshold will show a smooth change over from the conductivity of the dielectric component to the conductivity of the metallic component and can be described using two critical exponents s and t, whereas the dielectric constant will diverge if the threshold is approached from either side. To include the frequency dependent behavior, a resistor-capacitor model (R-C model) is used.
== Geometrical percolation==
For describing such a mixture of a dielectric and a metallic component we use the model of bond-percolation.
On a regular lattice, the bond between two nearest neighbors can either be occupied with probability p or not occupied with probability 1-p . There exists a critical value p_c . For occupation probabilities p > p_c an infinite cluster of the occupied bonds is formed. This value p_c is called the percolation threshold. The region near to this percolation threshold can be described by the two critical exponents \nu and \beta (see Percolation critical exponents).
With these critical exponents we have the ''correlation length'', \xi
\xi(p) \propto (p_c - p)^
and the ''percolation probability'', P:
P(p) \propto (p - p_c)^

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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