From 580c6daf2748aeca527eacc86dcf7bcd599dd7e4 Mon Sep 17 00:00:00 2001 From: hackbard Date: Mon, 10 Dec 2007 17:04:22 +0100 Subject: [PATCH] finished solution for tutorial 4 + added hall fig --- solid_state_physics/tutorial/1_04s.tex | 25 ++++++++++++++++- solid_state_physics/tutorial/hall.fig | 37 ++++++++++++++++++++++++++ 2 files changed, 61 insertions(+), 1 deletion(-) create mode 100644 solid_state_physics/tutorial/hall.fig diff --git a/solid_state_physics/tutorial/1_04s.tex b/solid_state_physics/tutorial/1_04s.tex index b5d60e3..d99b994 100644 --- a/solid_state_physics/tutorial/1_04s.tex +++ b/solid_state_physics/tutorial/1_04s.tex @@ -60,7 +60,30 @@ \stackrel{dt\rightarrow 0}{\Rightarrow} \quad \frac{dp(t)}{dt}=-\frac{p(t)}{\tau}+f(t) \] - \item + \item \includegraphics[width=14cm]{hall.eps} + \item \[ + \frac{dp}{dt}=-e\left(E+\frac{p}{m}\times B\right)-\frac{p}{\tau} + \] + steady state ($\frac{dp}{dt}=0$): + \begin{itemize} + \item $x$ component: $0=-eE_x-\frac{eB}{m}p_y-\frac{p_x}{\tau}$ + \item $y$ component: $0=-eE_y-\frac{eB}{m}p_x-\frac{p_y}{\tau}$ + \end{itemize} + setting $j_y$ to zero in the second equation ($\Rightarrow p_y=0$): + \[ + E_y=-\left(\frac{B}{m}\right)p_x + \stackrel{j=-ne\frac{p}{m}}{=}-\left(\frac{B}{ne}\right)j_x + \] + \[ + \Rightarrow R_H=-\frac{1}{ne} + \] + \item \begin{itemize} + \item electron density: $n=\frac{V\rho}{A_ru}/V=\frac{\rho}{A_ru}$ + \item $R_H=-\frac{1}{ne}=-\frac{A_ru}{e\rho}$ + \item $j_x=\frac{I}{ld}$ + \item $E_{Hall}=E_y=R_HBj_x=\ldots=5.3 \cdot 10^{-5} \, \frac{V}{m}$ + \item $U_{Hall}=E_y l=\ldots=-7.95 \, \mu V$ + \end{itemize} \end{enumerate} \end{document} diff --git a/solid_state_physics/tutorial/hall.fig b/solid_state_physics/tutorial/hall.fig new file mode 100644 index 0000000..c12b8a0 --- /dev/null +++ b/solid_state_physics/tutorial/hall.fig @@ -0,0 +1,37 @@ +#FIG 3.2 Produced by xfig version 3.2.5 +Landscape +Center +Metric +A4 +100.00 +Single +-2 +1200 2 +2 2 0 1 0 7 50 -1 -1 0.000 0 0 -1 0 0 5 + 2565 3780 7560 3780 7560 4230 2565 4230 2565 3780 +2 1 0 1 0 7 50 -1 -1 0.000 0 0 -1 0 0 2 + 2565 3780 4275 2070 +2 1 0 1 0 7 50 -1 -1 0.000 0 0 -1 0 0 2 + 4275 2070 9225 2070 +2 1 0 1 0 7 50 -1 -1 0.000 0 0 -1 0 0 2 + 7560 3780 9270 2070 +2 1 0 2 0 7 50 -1 -1 0.000 0 0 -1 1 0 2 + 1 1 3.00 60.00 120.00 + 5805 3015 5805 1575 +2 1 0 2 0 7 50 -1 -1 0.000 0 0 -1 1 0 2 + 1 1 3.00 60.00 120.00 + 8505 3105 9405 3105 +2 1 0 2 0 7 50 -1 -1 0.000 0 0 -1 1 0 2 + 1 1 3.00 60.00 120.00 + 2385 2925 3285 2925 +2 1 0 1 0 7 50 -1 -1 0.000 0 0 -1 0 0 4 + 7560 4230 9270 2520 9270 2070 9090 2070 +2 1 0 1 0 7 50 -1 -1 0.000 0 0 -1 1 0 2 + 1 1 1.00 60.00 120.00 + 7155 2565 6480 3240 +4 0 0 50 -1 0 12 0.0000 6 180 540 2475 2790 $E_x$\001 +4 0 0 50 -1 0 12 0.0000 4 105 4605 4320 2250 + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + +\001 +4 0 0 50 -1 0 12 0.0000 4 60 3315 2835 3735 - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - -\001 +4 0 0 50 -1 0 12 0.0000 6 165 345 5850 2475 $B$\001 +4 0 0 50 -1 0 12 0.0000 6 195 540 6975 2970 $E_y$\001 +4 0 0 50 -1 0 12 0.0000 6 195 480 8955 2970 $j_x$\001 -- 2.20.1