Temperature Dependence of In-plane Resistivity and Inverse Hall Angle in NLED Holographic Model
Qing-Yu Gan(
),Peng Wang(),Hai-Tang Yang()
),Peng Wang(),Hai-Tang Yang()
.
Fig. 9. (Color online) The overlap between T-linear $R_{xx}$ and T-quadratic $\cot\Theta_{H}$ in the Born-Infeld case. Region plots of $-0.2<{\rm d}\log_{10}({\rm d}R_{xx}/{\rm d}T)/{\rm d}\log_{10}T<0.2$ and $0.8<{\rm d}\log_{10}({\rm d}\cot\Theta_{H}/{\rm d}T)/{\rm d}\log_{10}T<1.2$ versus $a$ and $\log _{10}(T/\alpha)$ for several fixed values of $h/\alpha^{2}$ and $\rho /\alpha^{2}$. The fixed $\rho/\alpha^{2}$ for each row, from upper to lower, are set as $0.01$, $1$ and $10$. And the fixed $h/\alpha^{2}$ for each column, from left to right, are set as $0.01$, $1$ and $10$. The regions in yellow and green correspond to the T-linear $R_{xx}$ and the T-quadratic $\cot\Theta_{H} $, respectively.
