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Flaviu Cipcigan edited scattering 2.tex
over 10 years ago
Commit id: ec8e56eccae0acd504d82b26705cbe01e9d66241
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index b95f403..706e6a7 100644
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Therefore, we can conclude the following: the resistivity, inversely proportional to the conductivity, has the following behaviour:
\begin{equation}
\begin{split}
\rho &= \rho_\mathrm{impurity} +
A_\mathrm{qp--qp} T^2 A_\textrm{qp--qp} &T^2 \quad T \ll T_F \\
\rho &= \rho_\mathrm{impurity} +
B_\mathrm{qp--ph} T B_\textrm{qp--ph} &T \quad T \gg T_F \\
\end{split}
\end{equation}